Systems and methods for synthesizing data for training statistical models on different imaging modalities including polarized images

Information

  • Patent Grant
  • 11797863
  • Patent Number
    11,797,863
  • Date Filed
    Monday, January 4, 2021
    4 years ago
  • Date Issued
    Tuesday, October 24, 2023
    a year ago
  • CPC
  • Field of Search
    • CPC
    • G06F18/214
    • G06N33/045
    • G06N3/088
    • G06T15/00
    • G06T17/00
    • G06T17/20
  • International Classifications
    • G06N3/088
    • G06F18/214
    • G06N3/045
Abstract
A method of generating synthetic images of virtual scenes includes: placing, by a synthetic data generator implemented by a processor and memory, three-dimensional (3-D) models of objects in a 3-D virtual scene; adding, by the synthetic data generator, lighting to the 3-D virtual scene, the lighting including one or more illumination sources; applying, by the synthetic data generator, imaging modality-specific materials to the 3-D models of objects in the 3-D virtual scene in accordance with a selected multimodal imaging modality, each of the imaging modality-specific materials including an empirical model; setting a scene background in accordance with the selected multimodal imaging modality; and rendering, by the synthetic data generator, a two-dimensional image of the 3-D virtual scene based on the selected multimodal imaging modality to generate a synthetic image in accordance with the selected multimodal imaging modality.
Description
FIELD

Aspects of embodiments of the present disclosure relate to machine learning techniques, in particular the synthesis or generation of data for training machine learning models.


BACKGROUND

Statistical models such as machine learning models are generally trained using large amounts of data. In the field of computer vision, the training data generally includes labeled images, which are used to train deep learning models, such as convolutional neural networks, to perform computer vision tasks such as image classification and instance segmentation. However, manually collecting photographs of various scenes and labeling the photographs is time consuming and expensive. Some techniques for augmenting these training data sets include generating synthetic training data. For example, three-dimensional (3-D) computer graphics rendering engines (e.g., scanline rendering engines and ray tracing rendering engines) are capable of generating photorealistic two-dimensional (2-D) images of virtual environments of arrangements of 3-D models of objects that can be used for training deep learning models.


SUMMARY

Aspects of embodiments of the present disclosure relate to machine learning techniques, in particular the synthesis or generation of data for training machine learning models. In particular, aspects of embodiments of the present disclosure relate to synthesizing images for training machine learning models to perform computer vision tasks on input images that are captured based on imaging modalities other than images of the intensity of visible light in a scene.


According to one embodiment of the present disclosure, a method of generating synthetic images of virtual scenes includes: placing, by a synthetic data generator implemented by a processor and memory, three-dimensional (3-D) models of objects in a 3-D virtual scene; adding, by the synthetic data generator, lighting to the 3-D virtual scene, the lighting including one or more illumination sources; applying, by the synthetic data generator, imaging modality-specific materials to the 3-D models of objects in the 3-D virtual scene in accordance with a selected imaging modality, each of the imaging modality-specific materials including an empirical model; setting a scene background in accordance with the selected imaging modality; and rendering, by the synthetic data generator, a two-dimensional image of the 3-D virtual scene based on the selected imaging modality to generate a synthetic image in accordance with the selected imaging modality.


The empirical model may be generated based on sampled images captured of a surface of a material using an imaging system configured to capture images using the selected imaging modality, the sampled images may include images captured of the surface of the material from a plurality of different poses with respect to a normal direction of the surface of the material.


The selected imaging modality may be polarization and the imaging system includes a polarization camera.


The selected imaging modality may be thermal and the imaging system may include a thermal camera. The thermal camera may include a polarizing filter.


Each of the sampled images may be stored in association with the corresponding angle of its pose with respect to the normal direction of the surface of the material.


The sampled images may include: a first plurality of sampled images captured of the surface of the material illuminated by light having a first spectral profile; and a second plurality of sampled images captured of the surface of the material illuminated by light having a second spectral profile different from the first spectral profile.


The empirical model may include a surface light field function computed by interpolating between two or more of the sampled images.


The empirical model may include a surface light field function computed by a deep neural network trained on the sampled images.


The empirical model may include a surface light field function computed by a generative adversarial network trained on the sampled images.


The empirical model may include a surface light field function computed by a mathematical model generated based on the sampled images.


The method may further include applying style transfer to the synthetic image.


According to one embodiment of the present disclosure, a method for generating tensors in polarization feature space for a 3-D virtual scene, includes: rendering, by a synthetic data generator implemented by a processor and memory, an image of surface normals of a 3-D virtual scene including a plurality of 3-D models of objects, the surface normals including an azimuth angle component and a zenith angle component; determining, by the synthetic data generator, for a surface of a 3-D model of an object of the 3-D virtual scene, a material of the object; and computing, by the synthetic data generator, the tensors in polarization feature space in accordance with the azimuth angle component and the zenith angle component of the surface normal, the tensors in polarization feature space including: a degree of linear polarization; and an angle of linear polarization at the surface of the object.


The method may further include: determining whether the surface of the 3-D model of the object is specular dominant; computing the tensors in polarization feature space based on specular polarization equations in response to determining that the surface of the 3-D model of the object is specular dominant; and computing the tensors in polarization feature space based on diffuse polarization equations in response to determining that the surface of the 3-D model of the object is specular dominant.


The method may further include: computing the tensors in polarization feature space based on diffuse polarization equations.


The method may further include applying style transfer to the tensors in polarization feature space.


According to one embodiment of the present disclosure, a method for synthesizing a training data set based on generating a plurality of synthetic images generated in accordance with any of the above methods.


According to one embodiment of the present disclosure, a method for training a machine learning model includes: generating a training data set in accordance with any of the above methods; and computing parameters of the machine learning model based on the training data set.


According to one embodiment of the present disclosure, a system for generating synthetic images of virtual scenes includes: a processor; and memory storing instructions that, when executed by the processor, cause the processor to implement a synthetic data generator to: place three-dimensional (3-D) models of objects in a 3-D virtual scene; add lighting to the 3-D virtual scene, the lighting including one or more illumination sources; apply imaging modality-specific materials to the 3-D models of objects in the 3-D virtual scene in accordance with a selected imaging modality, each of the imaging modality-specific materials including an empirical model; set a scene background in accordance with the selected imaging modality; and render a two-dimensional image of the 3-D virtual scene based on the selected imaging modality to generate a synthetic image in accordance with the selected imaging modality.


The empirical model may be generated based on sampled images captured of a surface of a material using an imaging system configured to capture images using the selected imaging modality, and the sampled images may include images captured of the surface of the material from a plurality of different poses with respect to a normal direction of the surface of the material.


The selected imaging modality may be polarization and the imaging system may include a polarization camera.


The selected imaging modality may be thermal and the imaging system may include a thermal camera. The thermal camera may include a polarizing filter.


Each of the sampled images may be stored in association with the corresponding angle of its pose with respect to the normal direction of the surface of the material.


The sampled images may include: a first plurality of sampled images captured of the surface of the material illuminated by light having a first spectral profile; and a second plurality of sampled images captured of the surface of the material illuminated by light having a second spectral profile different from the first spectral profile.


The empirical model may include a surface light field function computed by interpolating between two or more of the sampled images.


The empirical model may include a surface light field function computed by a deep neural network trained on the sampled images.


The empirical model may include a surface light field function computed by a generative adversarial network trained on the sampled images.


The empirical model may include a surface light field function computed by a mathematical model generated based on the sampled images.


The memory may further store instructions that, when executed by the processor, cause the synthetic data generator to apply style transfer to the synthetic image.


According to one embodiment of the present disclosure, a system for generating tensors in polarization feature space for a 3-D virtual scene includes: a processor; and memory storing instructions that, when executed by the processor, cause the processor to implement a synthetic data generator to: render an image of surface normals of a 3-D virtual scene including a plurality of 3-D models of objects, the surface normals including an azimuth angle component and a zenith angle component; determine for a surface of a 3-D model of an object of the 3-D virtual scene, a material of the object; and compute the tensors in polarization feature space in accordance with the azimuth angle component and the zenith angle component of the surface normal, the tensors in polarization feature space including: a degree of linear polarization; and an angle of linear polarization at the surface of the object.


The memory may further store instructions that, when executed by the processor, cause the synthetic data generator to: determine whether the surface of the 3-D model of the object is specular dominant; compute the tensors in polarization feature space based on specular polarization equations in response to determining that the surface of the 3-D model of the object is specular dominant; and compute the tensors in polarization feature space based on diffuse polarization equations in response to determining that the surface of the 3-D model of the object is specular dominant.


The memory may further store instructions that, when executed by the processor, cause the synthetic data generator to: compute the tensors in polarization feature space based on diffuse polarization equations.


The memory may further store instructions that, when executed by the processor, cause the synthetic data generator to: apply style transfer to the tensors in polarization feature space.


According to one embodiment of the present disclosure, a system for synthesizing a training data set is configured to synthesize the training data set using the system of any of the above systems.


According to one embodiment of the present disclosure, a system for training a machine learning model includes: a processor; and memory storing instructions that, when executed by the processor, cause the processor to: receive a training data set generated by any of the above systems; and compute parameters of the machine learning model based on the training data set.





BRIEF DESCRIPTION OF THE DRAWINGS

The accompanying drawings, together with the specification, illustrate exemplary embodiments of the present invention, and, together with the description, serve to explain the principles of the present invention.



FIG. 1 is a block diagram depicting a system for training a statistical model to perform computer vision tasks based on images in various modalities, where the training is performed using data generated in accordance with embodiments of the present disclosure.



FIG. 2 is a schematic block diagram of a computer vision system configured to use polarization imaging and that can be trained based on synthetic polarization imaging data generated according to one embodiment of the present invention.



FIG. 3A is an image or intensity image of a scene with one real transparent ball placed on top of a printout of photograph depicting another scene containing two transparent balls (“spoofs”) and some background clutter.



FIG. 3B depicts the intensity image of FIG. 3A with an overlaid segmentation mask as computed by a comparative Mask Region-based Convolutional Neural Network (Mask R-CNN) identifying instances of transparent balls, where the real transparent ball is correctly identified as an instance, and the two spoofs are incorrectly identified as instances.



FIG. 3C is an angle of polarization image computed from polarization raw frames captured of the scene according to one embodiment of the present invention.



FIG. 3D depicts the intensity image of FIG. 3A with an overlaid segmentation mask as computed using polarization data in accordance with an embodiment of the present invention, where the real transparent ball is correctly identified as an instance and the two spoofs are correctly excluded as instances.



FIG. 4 is a high-level depiction of the interaction of light with transparent objects and non-transparent (e.g., diffuse and/or reflective) objects.



FIG. 5 is a graph of the energy of light that is transmitted versus reflected over a range of incident angles to a surface having a refractive index of approximately 1.5.



FIG. 6 is a flowchart depicting a pipeline for generating synthetic mages according to one embodiment of the present disclosure.



FIG. 7 is a schematic diagram of the sampling a real material from multiple angles using a polarization camera system according to one embodiment of the present disclosure.



FIG. 8 is a flowchart depicting a method for capturing images of a material from different perspectives using a particular imaging modality to be modeled according to one embodiment of the present disclosure.



FIG. 9 is a flowchart depicting a method for rendering a portion of a virtual object based on the empirical model of a material according to one embodiment of the present disclosure.



FIG. 10 is a flowchart depicting a method for computing synthetic features or tensors in polarization representation spaces for a virtual scene according to one embodiment of the present disclosure.



FIG. 11 is a flowchart depicting a method for generating a training data set according to one embodiment of the present disclosure.





DETAILED DESCRIPTION

In the following detailed description, only certain exemplary embodiments of the present invention are shown and described, by way of illustration. As those skilled in the art would recognize, the invention may be embodied in many different forms and should not be construed as being limited to the embodiments set forth herein. Like reference numerals designate like elements throughout the specification.


Aspects of embodiments of the present disclosure relate to systems and methods for synthesizing or generating data for training machine learning models for performing computer vision tasks on images captured based on modalities other than standard modalities such as color or monochrome cameras configured to capture images based on the intensity of visible light. Examples of other modalities include images captured based on polarized light (e.g., images captured with a polarizing filter or polarization filter in an optical path of the camera for capturing circularly and/or linearly polarized light), non-visible or invisible light (e.g., light in the infrared or ultraviolet ranges), and combinations thereof (e.g., polarized infrared light), however, embodiments of the present disclosure are not limited thereto and may be applied to other multi-spectral imaging techniques.


In more detail, aspects of embodiments of the present disclosure relate to generating synthetic images of objects in different imaging modalities for training a machine learning model to perform a computer vision task.


Generally, a computer vision system for computing segmentation maps that classify objects depicted in a scene may include a trained convolutional neural network that takes two-dimensional images (e.g., as captured by a color camera) as input and outputs segmentation maps based on those images. Such a convolutional neural network may be a pre-trained on an existing data set such as ImageNet (see, e.g., see, e.g., J. Deng, W. Dong, R. Socher, L.-J. Li, K. Li and L. Fei-Fei, ImageNet: A Large-Scale Hierarchical Image Database. IEEE Computer Vision and Pattern Recognition (CVPR), 2009). However, these existing data sets may contain images that are not representative of the images that are expected to be encountered in the particular application of the computer vision system, and therefore these pre-trained models may have poor performance on the particular computer vision task that the computer vision system is intended to perform. For example, a computer vision system for a manufacturing environment is more likely to encounter images of tools, partially assembled products, manufacturing components, and the like, rather than images of people, animals, household objects, and outdoors environments that may be found in more “general purpose” data sets.


As such, “retraining” relates to updating the parameters (e.g., connection weights) of a pre-trained model based on additional training data from a particular target domain associated with the task to be performed by the re-trained model. Continuing the above example, labeled images of tools, partially assembled products, components, and the like from a particular manufacturing environment may be used as training data for retraining a pre-trained model (e.g., a pre-trained convolutional neural network) to improve its performance in detecting and classifying objects encountered in that manufacturing environment. However, manually collecting different images of typical scenes in that manufacturing environment and labeling these images based on their ground truth values (e.g., identifying pixels that correspond to different classes of objects) is generally a time consuming and expensive task.


As noted above, three-dimensional (3-D) rendering computer graphics software may be used to generate training data for training machine learning models for performing computer vision tasks. For example, existing 3-D models of those tools, partially assembled products, and manufacturing components may be arranged in a virtual scene in accordance with the variety of ways in which such objects may be encountered in the real-world (e.g., including lighting conditions and 3-D models of support surfaces and equipment in the environment). For example, partially assembled products may be placed on a 3-D model of a conveyor belt, components may be located in a parts bin, and tools may be placed on a tool bench and/or within a scene in the process of positioning a component within a partially assembled product. Accordingly, a 3-D computer graphics rendering system is used to generate photorealistic images of the range of typical arrangements of objects in a particular environment. These generated images can also be automatically labeled. In particular, when the particular 3-D models used to depict each of the different types of objects are already associated with class labels (e.g., screws of various sizes, pre-assembled components, products at various stages of assembly, particular types of tools, etc.), segmentation maps can be automatically generated (e.g., by mapping surfaces of objects to their particular class labels).


However, 3-D rendering computer graphics software systems are generally tailored for generating images that represent typical imaging modalities based on the intensity of visible light (e.g., the intensities of red, green, and blue light). Such 3-D rendering software, such as Blender® by the Blender Foundation, generally does not account for behaviors of electromagnetic radiation that may be invisible or otherwise negligible when rendering photorealistic scenes. Examples of these additional behaviors include the polarization of light (e.g., as polarized light interacts with transparent objects and reflective objects in a scene, as detected by a camera with a polarizing filter in its optical path), thermal or infrared radiation (e.g., as emitted by warm objects in a scene and as detected by a camera system sensitive to detect infrared light), ultraviolet radiation (e.g., as detected by a camera system sensitive to ultraviolet light), combinations thereof (e.g., polarization with thermal radiation, polarization with visible light, polarization with ultraviolet light, etc.), and the like.


Therefore, aspects of embodiments of the present disclosure relate to systems and methods for modeling the behavior of various materials when imaged based on polarization or other imaging modalities. The data (e.g., images) generated in accordance with embodiments of the present disclosure may then be used as training data for training deep learning models such as deep convolutional neural networks to compute predictions based on imaging modalities other than standard imaging modalities (e.g., the intensity of visible light or light in a visible portion of the electromagnetic spectrum).


As a motivating example, embodiments of the present disclosure will be described in the context of generating synthetic images of objects captured through a polarizing filter (referred to herein as “polarization raw frames”), where these images may be used in training a deep neural network such as a convolutional neural network to perform a task based on polarization raw frames. However, embodiments of the present disclosure are not limited to generating synthetic polarization raw frames for training a convolutional neural network that takes polarization raw frames (or features extracted therefrom) as input data.



FIG. 1 is a block diagram depicting a system for training a statistical model to perform computer vision tasks based on images in various modalities, where the training is performed using data generated in accordance with embodiments of the present disclosure. as shown in FIG. 1, training data 5 is supplied to a model training system 7, which takes a model 30 (e.g., a pre-trained model or a model architecture with initialized weights) and uses the training data 5 to generate a trained model (or re-trained model) 32. The model 30 and the trained model 32 may be a statistical model such as a deep neural network (deep neural networks include convolutional neural networks). A synthetic data generator 40 according to embodiments of the present disclosure generates synthesized data 42, which may be included with the training data 5 for generating the trained model 32. The model training system 7 may apply an iterative process for updating the parameters of the model 30 to generate the trained model 32 in accordance with the supplied training data 5 (e.g., including the synthesized data 42). The updating of the parameters of the model 30 may include, for example, applying gradient descent (and, in the case of a neural network, backpropagation) in accordance with a loss function measuring a difference between the labels and the output of the model in response to the training data. The model training system 7 and the synthetic data generator 40 may be implemented using one or more electronic circuits.


According to various embodiments of the present disclosure, the model training system 7 and/or the synthetic data generator 40 are implemented using one or more electronic circuits configured to perform various operations as described in more detail below. Types of electronic circuits may include a central processing unit (CPU), a graphics processing unit (GPU), an artificial intelligence (AI) accelerator (e.g., a vector processor, which may include vector arithmetic logic units configured efficiently perform operations common to neural networks, such dot products and softmax), a field programmable gate array (FPGA), an application specific integrated circuit (ASIC), a digital signal processor (DSP), or the like. For example, in some circumstances, aspects of embodiments of the present disclosure are implemented in program instructions that are stored in a non-volatile computer readable memory where, when executed by the electronic circuit (e.g., a CPU, a GPU, an AI accelerator, or combinations thereof), perform the operations described herein to compute a segmentation map 20 from input polarization raw frames 18. The operations performed by the model training system 7 and the synthetic data generator 40 may be performed by a single electronic circuit (e.g., a single CPU, a single GPU, or the like) or may be allocated between multiple electronic circuits (e.g., multiple GPUs or a CPU in conjunction with a GPU). The multiple electronic circuits may be local to one another (e.g., located on a same die, located within a same package, or located within a same embedded device or computer system) and/or may be remote from one other (e.g., in communication over a network such as a local personal area network such as Bluetooth®, over a local area network such as a local wired and/or wireless network, and/or over wide area network such as the internet, such a case where some operations are performed locally and other operations are performed on a server hosted by a cloud computing service). One or more electronic circuits operating to implement the model training system 7 and the synthetic data generator 40 may be referred to herein as a computer or a computer system, which may include memory storing instructions that, when executed by the one or more electronic circuits, implement the systems and methods described herein.



FIG. 2 is a schematic block diagram of a computer vision system configured to use polarization imaging and that can be trained based on synthetic polarization imaging data generated according to one embodiment of the present invention.


For context, FIG. 2 is a schematic depiction of a system in which a polarization camera images a scene and supplies polarization raw frames to a computer vision system that includes a model that is trained to perform computer vision tasks based on polarization raw frames or polarization features computed based on polarization raw frames


A polarization camera 10 has a lens 12 with a field of view, where the lens 12 and the camera 10 are oriented such that the field of view encompasses the scene 1. The lens 12 is configured to direct light (e.g., focus light) from the scene 1 onto a light sensitive medium such as an image sensor 14 (e.g., a complementary metal oxide semiconductor (CMOS) image sensor or charge-coupled device (CCD) image sensor).


The polarization camera 10 further includes a polarizer or polarizing filter or polarization mask 16 placed in the optical path between the scene 1 and the image sensor 14. According to various embodiments of the present disclosure, the polarizer or polarization mask 16 is configured to enable the polarization camera 10 to capture images of the scene 1 with the polarizer set at various specified angles (e.g., at 45° rotations or at 60° rotations or at non-uniformly spaced rotations).


As one example, FIG. 2 depicts an embodiment where the polarization mask 16 is a polarization mosaic aligned with the pixel grid of the image sensor 14 in a manner similar to a red-green-blue (RGB) color filter (e.g., a Bayer filter) of a color camera. In a manner similar to how a color filter mosaic filters incoming light based on wavelength such that each pixel in the image sensor 14 receives light in a particular portion of the spectrum (e.g., red, green, or blue) in accordance with the pattern of color filters of the mosaic, a polarization mask 16 using a polarization mosaic filters light based on linear polarization such that different pixels receive light at different angles of linear polarization (e.g., at 0°, 45°, 90°, and 135°, or at 0°, 60° degrees, and 120°). Accordingly, the polarization camera 10 using a polarization mask 16 such as that shown in FIG. 2 is capable of concurrently or simultaneously capturing light at four different linear polarizations. One example of a polarization camera is the Blackfly® S Polarization Camera produced by FLIR® Systems, Inc. of Wilsonville, Oreg.


While the above description relates to some possible implementations of a polarization camera using a polarization mosaic, embodiments of the present disclosure are not limited thereto and encompass other types of polarization cameras that are capable of capturing images at multiple different polarizations. For example, the polarization mask 16 may have fewer than or more than four different polarizations, or may have polarizations at different angles (e.g., at angles of polarization of: 0°, 60° degrees, and 120° or at angles of polarization of 0°, 30°, 60°, 90°, 120°, and 150°). As another example, the polarization mask 16 may be implemented using an electronically controlled polarization mask, such as an electro-optic modulator (e.g., may include a liquid crystal layer), where the polarization angles of the individual pixels of the mask may be independently controlled, such that different portions of the image sensor 14 receive light having different polarizations. As another example, the electro-optic modulator may be configured to transmit light of different linear polarizations when capturing different frames, e.g., so that the camera captures images with the entirety of the polarization mask set to, sequentially, to different linear polarizer angles (e.g., sequentially set to: 0 degrees; 45 degrees; 90 degrees; or 135 degrees). As another example, the polarization mask 16 may include a polarizing filter that rotates mechanically, such that different polarization raw frames are captured by the polarization camera 10 with the polarizing filter mechanically rotated with respect to the lens 12 to transmit light at different angles of polarization to image sensor 14.


A polarization camera may also refer to an array of multiple cameras having substantially parallel optical axes, such that each of the cameras captures images of a scene from substantially the same pose. The optical path of each camera of the array includes a polarizing filter, where the polarizing filters have different angles of polarization. For example, a two-by-two (2×2) array of four cameras may include one camera having a polarizing filter set at an angle of 0°, a second camera having a polarizing filter set at an angle of 45°, a third camera having a polarizing filter set at an angle of 90°, and a fourth camera having a polarizing filter set at an angle of 135°.


As a result, the polarization camera captures multiple input images 18 (or polarization raw frames) of the scene 1, where each of the polarization raw frames 18 corresponds to an image taken behind a polarization filter or polarizer at a different angle of polarization ϕpol (e.g., 0 degrees, 45 degrees, 90 degrees, or 135 degrees). Each of the polarization raw frames is captured from substantially the same pose with respect to the scene 1 (e.g., the images captured with the polarization filter at 0 degrees, 45 degrees, 90 degrees, or 135 degrees are all captured by a same polarization camera located at a same location and orientation), as opposed to capturing the polarization raw frames from disparate locations and orientations with respect to the scene. The polarization camera 10 may be configured to detect light in a variety of different portions of the electromagnetic spectrum, such as the human-visible portion of the electromagnetic spectrum, red, green, and blue portions of the human-visible spectrum, as well as invisible portions of the electromagnetic spectrum such as infrared and ultraviolet.



FIGS. 3A, 3B, 3C, and 3D provide background for illustrating the segmentation maps computed by a comparative approach and semantic segmentation or instance segmentation according to embodiments of the present disclosure. In more detail, FIG. 3A is an image or intensity image of a scene with one real transparent ball placed on top of a printout of photograph depicting another scene containing two transparent balls (“spoofs”) and some background clutter. FIG. 3B depicts an segmentation mask as computed by a comparative Mask Region-based Convolutional Neural Network (Mask R-CNN) identifying instances of transparent balls overlaid on the intensity image of FIG. 3A using different patterns of lines, where the real transparent ball is correctly identified as an instance, and the two spoofs are incorrectly identified as instances. In other words, the Mask R-CNN algorithm has been fooled into labeling the two spoof transparent balls as instances of actual transparent balls in the scene.



FIG. 3C is an angle of linear polarization (AOLP) image computed from polarization raw frames captured of the scene according to one embodiment of the present invention. As shown in FIG. 3C, transparent objects have a very unique texture in polarization space such as the AOLP domain, where there is a geometry-dependent signature on edges and a distinct or unique or particular pattern that arises on the surfaces of transparent objects in the angle of linear polarization. In other words, the intrinsic texture of the transparent object (e.g., as opposed to extrinsic texture adopted from the background surfaces visible through the transparent object) is more visible in the angle of polarization image of FIG. 3C than it is in the intensity image of FIG. 3A.



FIG. 3D depicts the intensity image of FIG. 3A with an overlaid segmentation mask as computed using polarization data in accordance with an embodiment of the present invention, where the real transparent ball is correctly identified as an instance using an overlaid pattern of lines and the two spoofs are correctly excluded as instances (e.g., in contrast to FIG. 3B, FIG. 3D does not include overlaid patterns of lines over the two spoofs). While FIGS. 3A, 3B, 3C, and 3D illustrate an example relating to detecting a real transparent object in the presence of spoof transparent objects, embodiments of the present disclosure are not limited thereto and may also be applied to other optically challenging objects, such as transparent, translucent, and non-matte or non-Lambertian objects, as well as non-reflective (e.g., matte black objects) and multipath inducing objects.


Polarization Feature Representation Spaces


Some aspects of embodiments of the present disclosure relate to systems and methods for extracting features from polarization raw frames, where these extracted features are used by the processing system 100 for the robust detection of optically challenging characteristics in the surfaces of objects. In contrast, comparative techniques relying on intensity images alone may fail to detect these optically challenging features or surfaces (e.g., comparing the intensity image of FIG. 3A with the AOLP image of FIG. 3C, discussed above). The term “first tensors” in “first representation spaces” will be used herein to refer to features computed from (e.g., extracted from) polarization raw frames 18 captured by a polarization camera, where these first representation spaces include at least polarization feature spaces (e.g., feature spaces such as AOLP and DOLP that contain information about the polarization of the light detected by the image sensor) and may also include non-polarization feature spaces (e.g., feature spaces that do not require information regarding the polarization of light reaching the image sensor, such as images computed based solely on intensity images captured without any polarizing filters).


The interaction between light and transparent objects is rich and complex, but the material of an object determines its transparency under visible light. For many transparent household objects, the majority of visible light passes straight through and a small portion (˜4% to ˜8%, depending on the refractive index) is reflected. This is because light in the visible portion of the spectrum has insufficient energy to excite atoms in the transparent object. As a result, the texture (e.g., appearance) of objects behind the transparent object (or visible through the transparent object) dominate the appearance of the transparent object. For example, when looking at a transparent glass cup or tumbler on a table, the appearance of the objects on the other side of the tumbler (e.g., the surface of the table) generally dominate what is seen through the cup. This property leads to some difficulties when attempting to detect surface characteristics of transparent objects such as glass windows and glossy, transparent layers of paint, based on intensity images alone:



FIG. 4 is a high-level depiction of the interaction of light with transparent objects and non-transparent (e.g., diffuse and/or reflective) objects. As shown in FIG. 4, a polarization camera 10 captures polarization raw frames of a scene that includes a transparent object 402 in front of an opaque background object 403. A light ray 410 hitting the image sensor 14 of the polarization camera 10 contains polarization information from both the transparent object 402 and the background object 403. The small fraction of reflected light 412 from the transparent object 402 is heavily polarized, and thus has a large impact on the polarization measurement, in contrast to the light 413 reflected off the background object 403 and passing through the transparent object 402.


Similarly, a light ray hitting the surface of an object may interact with the shape of the surface in various ways. For example, a surface with a glossy paint may behave substantially similarly to a transparent object in front of an opaque object as shown in FIG. 4, where interactions between the light ray and a transparent or translucent layer (or clear coat layer) of the glossy paint causes the light reflecting off of the surface to be polarized based on the characteristics of the transparent or translucent layer (e.g., based on the thickness and surface normals of the layer), which are encoded in the light ray hitting the image sensor. Similarly, as discussed in more detail below with respect to shape from polarization (SfP) theory, variations in the shape of the surface (e.g., direction of the surface normals) may cause significant changes in the polarization of light reflected by the surface of the object. For example, smooth surfaces may generally exhibit the same polarization characteristics throughout, but a scratch or a dent in the surface changes the direction of the surface normals in those areas, and light hitting scratches or dents may be polarized, attenuated, or reflected in ways different than in other portions of the surface of the object. Models of the interactions between light and matter generally consider three fundamentals: geometry, lighting, and material. Geometry is based on the shape of the material. Lighting includes the direction and color of the lighting. Material can be parameterized by the refractive index or angular reflection/transmission of light. This angular reflection is known as a bi-directional reflectance distribution function (BRDF), although other functional forms may more accurately represent certain scenarios. For example, the bidirectional subsurface scattering distribution function (BSSRDF) would be more accurate in the context of materials that exhibit subsurface scattering (e.g. marble or wax).


A light ray 410 hitting the image sensor 16 of a polarization camera 10 has three measurable components: the intensity of light (intensity image/I), the percentage or proportion of light that is linearly polarized (degree of linear polarization/DOLP/ρ), and the direction of that linear polarization (angle of linear polarization/AOLP/ϕ). These properties encode information about the surface curvature and material of the object being imaged, which can be used by the predictor 800 to detect transparent objects, as described in more detail below. In some embodiments, the predictor 800 can detect other optically challenging objects based on similar polarization properties of light passing through translucent objects and/or light interacting with multipath inducing objects or by non-reflective objects (e.g., matte black objects).


Therefore, some aspects of embodiments of the present invention relate synthesizing polarization raw frames that can be used to compute first tensors in one or more first representation spaces, which may include derived feature maps based on the intensity I, the DOLP ρ, and the AOLP ϕ. Some aspects of embodiments of the present disclosure also relate to directly synthesizing tensors in one or more representation spaces such as DOLP p and AOLP for use in training deep learning systems to perform computer vision tasks based on information regarding the polarization of light in a scene (and, in some embodiments, based on other imaging modalities such as thermal imaging and combinations of thermal and polarized imaging).


Measuring intensity I, DOLP ρ, and AOLP at each pixel requires 3 or more polarization raw frames of a scene taken behind polarizing filters (or polarizers) at different angles, ϕpol (e.g., because there are three unknown values to be determined: intensity I, DOLP ρ, and AOLP ϕ. For example, the FLIR® Blackfly® S Polarization Camera described above captures polarization raw frames with polarization angles ϕpol at 0 degrees, 45 degrees, 90 degrees, or 135 degrees, thereby producing four polarization raw frames Iϕpol, denoted herein as I0, I45, I90, and I135.


The relationship between Iϕpol and intensity I, DOLP ρ, and AOLP ϕ at each pixel can be expressed as:

Iϕpol=I(1+ρ cos(2(ϕ−ϕpol)))  (1)


Accordingly, with four different polarization raw frames Iϕpol (I0, I45, I90, and I135), a system of four equations can be used to solve for the intensity I, DOLP ρ, and AOLP ϕ.


Shape from Polarization (SfP) theory (see, e.g., Gary A Atkinson and Edwin R Hancock. Recovery of surface orientation from diffuse polarization. IEEE transactions on image processing, 15(6):1653-1664, 2006.) states that the relationship between the refractive index (n), azimuth angle (θa) and zenith angle (θz) of the surface normal of an object and the and p components of the light ray coming from that object follow the following characteristics when diffuse reflection is dominant:









ρ
=




(

n
-

1
n


)

2




sin
2

(

θ
z

)



2
+

2


n
2


-



(

n
+

1
n


)

2



sin
2



θ
z


+

4


cos



θ
z





n
2

-


sin
2



θ
z











(
2
)












ϕ
=

θ
a





(
3
)








and when the specular reflection is dominant:









ρ
=


2



sin
2



θ
z



cos



θ
z





n
2

-


sin
2




θ
z







n
2

-


sin
2




θ
z


-


n
2




sin
2




θ
z


+

2



sin
4




θ
z








(
4
)












ϕ
=


θ
a

-

π
2






(
5
)








Note that in both cases ρ increases exponentially as θz increases and if the refractive index is the same, specular reflection is much more polarized than diffuse reflection.


Accordingly, some aspects of embodiments of the present disclosure relate to applying SfP theory to generate synthetic raw polarization frames 18 and/or AOLP and DOLP images based on the shapes of surfaces (e.g., the orientation of surfaces) in a virtual environment.


Light rays coming from a transparent objects have two components: a reflected portion including reflected intensity Ir, reflected DOLP ρr, and reflected AOLP ϕr and the refracted portion including refracted intensity It, refracted DOLP ρt, and refracted AOLP ϕt. The intensity of a single pixel in the resulting image can be written as:

I=Ir+It  (6)


When a polarizing filter having a linear polarization angle of ϕpol is placed in front of the camera, the value at a given pixel is:

Iϕpol=(1+ρr cos(2(ϕr−ϕpol)))+It(1+ρt cos(2(ϕt−ϕpol)))  (7)


Solving the above expression for the values of a pixel in a DOLP ρ image and a pixel in an AOLP ϕ image in terms of Ir, ρr, ϕr, It, Pt, and ϕt:









ρ
=





(


I
r



ρ
r


)

2

+


(


I
t



ρ
t


)

2

+

2


I
t



ρ
t



I
r



ρ
r



cos

(

2


(


ϕ
r

-

ϕ
t


)


)






I
r

+

I
t







(
8
)












ϕ
=


arctan

(



I
r



ρ
r



sin

(

2


(


ϕ
r

-

ϕ
t


)


)





I
t



ρ
t


+


I
r



ρ
r



cos

(

2


(


ϕ
r

-

ϕ
t


)


)




)

+

ϕ
r






(
9
)







Accordingly, equations (7), (8), and (9), above provide a model for forming first tensors 50 in first representation spaces that include an intensity image I, a DOLP image ρ, and an AOLP image ϕ according to one embodiment of the present disclosure, where the use of polarization images or tensor in polarization representation spaces (including DOLP image ρ and an AOLP image ϕ based on equations (8) and (9)) enables trained computer vision systems to reliably detect of optically challenging surface characteristics of objects that are generally not detectable by comparative systems that use only intensity I images as input.


In more detail, first tensors in polarization representation spaces (among the derived feature maps) such as the polarization images DOLP ρ and AOLP ϕ can reveal surface characteristics of objects that might otherwise appear textureless in an intensity I domain. A transparent object may have a texture that is invisible in the intensity domain I because this intensity is strictly dependent on the ratio of Ir/It (see equation (6)). Unlike opaque objects where It=0, transparent objects transmit most of the incident light and only reflect a small portion of this incident light. As another example, thin or small deviations in the shape of an otherwise smooth surface (or smooth portions in an otherwise rough surface) may be substantially invisible or have low contrast in the intensity I domain (e.g., a domain in which polarization of light is not taken into account), but may be very visible or may have high contrast in a polarization representation space such as DOLP ρ or AOLP ϕ.


As such, one exemplary method to acquire surface topography is to use polarization cues in conjunction with geometric regularization. The Fresnel equations relate the AOLP and the DOLP ρ with surface normals. These equations can be useful for anomaly detection by exploiting what is known as polarization patterns of the surface. A polarization pattern is a tensor of size [M, N, K] where M and N are horizontal and vertical pixel dimensions, respectively, and where K is the polarization data channel, which can vary in size. For example, if circular polarization is ignored and only linear polarization is considered, then K would be equal to two, because linear polarization has both an angle and a degree of polarization (AOLP ϕ and DOLP ρ). Analogous to a Moire pattern, in some embodiments of the present disclosure, the feature extraction module 700 extracts a polarization pattern in polarization representation spaces (e.g., AOLP space and DOLP space). In the example characterization output 20 shown in FIG. 1A and FIG. 1B shown above, the horizontal and vertical dimensions correspond to the lateral field of view of a narrow strip or patch of a surface of an object captured by the polarization camera 10. However, this is one exemplary case: in various embodiments, the strip or patch of the surface may be vertical (e.g., much taller than wide), horizontal (e.g., much wider than tall), or have a more conventional field of view (FoV) that tends closer toward a square (e.g., a 4:3 ratio or 16:9 ratio of width to height).


While the preceding discussion provides specific examples of polarization representation spaces based on linear polarization in the case of using a polarization camera having one or more linear polarizing filters to capture polarization raw frames corresponding to different angles of linear polarization and to compute tensors in linear polarization representation spaces such as DOLP and AOLP, embodiments of the present disclosure are not limited thereto. For example, in some embodiments of the present disclosure, a polarization camera includes one or more circular polarizing filters configured to pass only circularly polarized light, and where polarization patterns or first tensors in circular polarization representation space are further extracted from the polarization raw frames. In some embodiments, these additional tensors in circular polarization representation space are used alone, and in other embodiments they are used together with the tensors in linear polarization representation spaces such as AOLP and DOLP. For example, a polarization pattern including tensors in polarization representation spaces may include tensors in circular polarization space, AOLP, and DOLP, where the polarization pattern may have dimensions [M, N, K], where K is three to further include the tensor in circular polarization representation space.



FIG. 5 is a graph of the energy of light that is transmitted versus reflected over a range of incident angles to a surface having a refractive index of approximately 1.5. As shown in FIG. 5, the slopes of the transmitted energy (shown in FIG. 5 with a solid line) and reflected energy (shown in FIG. 5 with a dotted line) lines are relatively small at low incident angles (e.g., at angles closer to perpendicular to the plane of the surface). As such, small differences in the angle of the surface may be difficult to detect (low contrast) in the polarization pattern when the angle of incidence is low (e.g., close to perpendicular to the surface, in other words, close to the surface normal). On the other hand, the slope of the reflected energy increases from flat, as the angle of incidence increases, and the slope of the transmitted energy decreases from flat (to have a larger absolute value) as the angle of incidence increases. In the example shown in FIG. 5 with an index of refraction of 1.5, the slopes of both lines are substantially steeper beginning at an incident angle of around 60°, and their slopes are very steep at an incident angle of around 80°. The particular shapes of the curves may change for different materials in accordance with the refractive index of the material. Therefore, capturing images of surfaces under inspection at incident angles corresponding to steeper portions of the curves (e.g., angles close to parallel to the surface, such as around 80° in the case of a refractive index of 1.5, as shown in FIG. 5) can improve the contrast and detectability of variations in the surface shapes in the polarization raw frames 18 and may improve the detectability of such features in tensors in polarization representation spaces, because small changes in incident angle (due to the small changes in the surface normal) can cause large changes in the captured polarization raw frames.


The use of polarization cameras to detect the presence and shape of optically challenging objects and surfaces is described in more detail, for example, in PCT Patent Application No. US/2020/048604, filed on Aug. 28, 2020 and in PCT Patent Application No. US/2020/051243, filed on Sep. 17, 2020, the entire disclosures of which are incorporated by reference herein. Such computer vision systems may be trained to perform computer vision tasks on polarization data based on training data generated in accordance with embodiments of the present disclosure. In some embodiments, these computer vision systems use machine learning models such as deep neural networks (e.g., convolutional neural networks) to perform the computer vision tasks, where the deep learning models are configured to take, as input, polarization raw frames and/or features in polarization representation spaces.


Simulating the physics of polarization for different materials is a complex task requiring an understanding of the material properties, the spectral profile and polarization parameters of the illumination used, and the angle at which the reflected light is observed by the observer. To truly simulate the physics of light polarization and its impact on the illumination of objects would not only be a complex task but would also be an intensely compute intensive task, such as by applying a complex forward model that typically produces highly inaccurate (unrealistic) images. Accordingly, various comparative 3-D computer graphics systems typically do not accurately model the physics of light polarization and its impact on the illumination of objects, and therefore are not capable of synthesizing or rendering images of virtual environments in a manner that realistically represents how a corresponding real environment would appear if imaged with a camera with a polarizing filter in its optical path (e.g., a polarization camera). As such, comparative techniques for generating synthetic data for training computer vision systems that operate on standard imaging modalities (such as visible light images without polarizing filters) are generally incapable of generating training data for training computer vision systems that operate on other imaging modalities (e.g., polarization cameras, thermal cameras, and the like).


As discussed above, aspects of embodiments of the present disclosure relate to generating or synthesizing data for training machine learning models to take, as input, data captured using imaging modalities other than images captured by a standard camera (e.g., a camera configured to capture the intensity of visible light without the use of filters such as polarizing filters), which will be referred to herein as multimodal images or plenoptic images. The term “multimodal” refers to the plenoptic theory of light, where each dimension of the plenoptic domain (e.g., wavelength, polarization, angle, etc.) is an example of a modality of light. Accordingly, multimodal or plenoptic imaging includes, but is not limited to, the concurrent use of multiple imaging modalities. For example, the term “multimodal” may be used herein to refer to a single imaging modality, where that single imaging modality is a modality different from the intensity of visible light without the use of filters such as polarizing filters. Polarization raw frames captured by one or more polarization cameras and/or tensors in polarization representation spaces are one example of a class of inputs in a multimodal or plenoptic imaging modality (e.g., using multimodal imaging or plenoptic imaging).


Generally, various aspects of embodiments of the present disclosure relate to four techniques may be used separately or in combination as part of a pipeline for generating synthetic training data in accordance with multimodal or plenoptic imaging modalities such as a polarized imaging modality. These techniques include: domain randomization, texture mapping, normal mapping, and style transfer, and will be discussed in more detail below.



FIG. 6 is a flowchart depicting a pipeline for generating synthetic mages according to one embodiment of the present disclosure. In some embodiments of the present disclosure, the operations of FIG. 6 are performed by the synthetic data generator 40, for example, in special-purpose program instructions stored in a memory of the synthetic data generator 40 that, when executed by the processor of the synthetic data generator 40, cause the synthetic data generator 40 to perform the special-purpose operations described herein for generating synthetic images based on the physical simulation of optical phenomena. For the sake of convenience, aspects of embodiments of the present disclosure will be described in the context of applying polarization imaging in a manufacturing context to perform computer vision tasks on optically challenging manufacturing components and tools, such as objects having transparent, shiny metal, and/or dark matte surfaces.


In operation 610, the synthetic data generator 40 places 3-D models of objects in a virtual scene. In the context of generating synthetic images of scenes in a manufacturing environment, 3-D models of objects may be readily available from computer aided design (CAD) models of components and partially or fully assembled manufactured products. These CAD models may have previously been produced in the product design phase and may be obtained from, for example, the vendor of the component (e.g., from the vendor who supplied the components to the manufacturer), publicly available information (e.g., data sheets), or from internal product designers employed by the manufacturer. In some circumstances the CAD models may be manually generated based on specifications of a component.


In some embodiments of the present disclosure, the 3-D models of objects are placed in a virtual scene in a manner resembling the arrangement of those objects as they would be expected to be encountered for the particular computer vision task that the machine learning model will be trained to perform.


In the above example of computer vision in a manufacturing context, one task is to perform instance segmentation on a bin of components, where the components may be homogeneous (e.g., all the components in the bin are the same, such as a bin of springs or screws) or heterogeneous (e.g., a mix of different types of components, such as screws of different sizes or screws mixed with matching nuts). The objects may be randomly arranged within the bin, where the components may be oriented in many different directions in the bin, and where, in a bin of heterogeneous components, the different types of components are mixed together, as opposed to being separated in different parts of the bin. A computer vision system may be trained to compute a segmentation map of the bin, to identify the location and orientation of individual components within the bin (and, in the case of a bin of heterogenous components, the types of the objects). This segmentation map can then be used by an actuator system, such that a robotic arm, to pick components out of the bin and add the picked components to a partially assembled product.


Accordingly, in some embodiments of the present disclosure, the synthetic data generator 40 generates a scene of components in a bin by placing a 3-D model of a virtual bin in a scene, and dropping 3-D models of components into the virtual bin, as simulated using a physics simulation engine, such as a physics engine incorporated into a 3-D computer graphics rendering system. For example, the Blender® 3-D rendering software includes a physics system that simulates various physical real-world phenomena such as the movement, collision, and potential deformation of rigid bodies, cloth, soft bodies, fluids, and the like, as affected by gravity or other forces. Accordingly, a rigid body simulation may be used for simulating the dropping of rigid components (e.g., screws, bolts, relatively stiff springs) into a rigid virtual bin, and a soft body simulation may be used for elastic or deformable components (e.g., string, wire, plastic sheeting, etc.) into a rigid virtual bin.


In more detail, a variety of difference scenes representing different potential states of the bin may be generated, such as by dropping various numbers of instances of the 3-D models of the components into a virtual bin. For example, if a typical bin has a maximum capacity of 1,000 screws, various scenes can be generated by dropping 1,000 screws, 900 screws, 500 screws, 100 screws, and 10 screws into a virtual bin to generate different scenes representing different potential fullness states of the virtual bin. In addition, multiple scenes may be generated for any given number of screws (or the number of screws may be randomized between the generation of different scenes), where the arrangement of components within the bin is also randomized, such as by dropping components into the bin, one at a time, from different random locations above the bin.


Accordingly, in operation 610, the synthetic data generator 40 generates a scene containing an arrangement of representative objects.


In operation 630, the synthetic data generator 40 adds lighting to the virtual scene generated in operation 610. In particular, the synthetic data generator 40 adds one or more light sources to the virtual scene, where the light sources illuminate part or all of the surfaces of the objects in the bin. In some embodiments, the position of the one or more light sources is randomized, and multiple scenes are generated with light sources in different locations (e.g., different angles and distances) relative to the bin of parts in order to improve the robustness of the training. In some embodiments of the present disclosure, the virtual lighting includes virtual light sources that are representative of the light sources that would be found in environments in which the computer vision system is trained to operate. Examples of potential representative light sources include different color temperatures corresponding to, for example, incandescent lights, fluorescent lights, light emitting diode (LED) bulbs, natural light from a simulated window in the environment, and other forms of lighting technology, where the shape of the virtual lights (e.g., the direction of the rays emitted by the lights) may be in a range from direct light to diffuse light. In some embodiments of the present disclosure, the character of the light (e.g., color temperature and shape) is also randomized to generate different scenes with different types of lighting.


In operation 650, the synthetic data generator 40 applies modality-specific materials to the objects in the 3-D virtual scene. For example, in the case of generating synthesized polarization imaging data, polarization-specific materials are applied to the objects in the virtual scene, whereas in the case of generating synthesized thermal imaging data, thermal imaging-specific materials may be applied to the objects in the virtual scene. For the sake of illustration, polarization-specific materials will be described in detail herein, but embodiments of the present disclosure are not limited thereto and may also be applied to generating and applying materials specific to multimodal imaging modalities and/or plenoptic imaging modalities.


Some aspects of embodiments of the present disclosure relate to domain randomization, in which the material appearance of objects in a scene are randomized beyond the typical appearance of the objects. For example, in some embodiments, a large number of materials with random colors (e.g., thousands of different materials of different, randomly selected colors) are applied to the different objects in the virtual scene. In a real-world environment, the objects in a scene generally have well-defined colors (e.g., rubber washers generally all look matte black and screws may be particular shades of shiny black, matte black, gold, or shiny metal). However, real-world objects can often have different appearances due to changes in lighting conditions, such as the color temperature of lights, reflections, specular highlights, and the like. Accordingly, applying randomization to the colors of the materials applied to the objects when generating training data expands the domain of the training data to also encompass unrealistic colors, thereby increasing diversity in the training data for training a more robust machine learning model that is capable of making accurate predictions (e.g., more accurate instance segmentation maps) in a wider variety of real-world conditions.


Some aspects of embodiments of the present disclosure relate to performing texture mapping to generate models of materials that are dependent on one or more parameters (parameterized materials) in accordance with the imaging modality. For example, as discussed above, the appearance of a given surface in a scene, as imaged by a polarization camera system, may change based on the properties of the material of the surface, the spectral profile and polarization parameters of the illumination source or illumination sources (light sources) in the scene, the incident angle of light onto the surface, and the viewpoint angle of the observer (e.g., the polarization camera system). As such, simulating the physics of polarization for different materials is a complex and computationally-intensive task.


As such, some aspects of embodiments of the present disclosure relate to emulating the physics of various imaging modalities based on empirical data, such as real-world images captured of real-world materials. In more detail, an imaging system implementing the particular imaging modality of interest (e.g., a polarization camera system) is used to collect sample images from an object made of the particular material of interest. In some embodiments, the collected sample images are used to compute an empirical model of the material, such as its surface light-field function (e.g., a bi-directional reflectance density function or BRDF).



FIG. 7 is a schematic diagram of the sampling a real material from multiple angles using a polarization camera system according to one embodiment of the present disclosure. FIG. 8 is a flowchart depicting a method 800 for capturing images of a material from different perspectives using a particular imaging modality to be modeled according to one embodiment of the present disclosure. As shown in FIG. 7, a surface 702 of a physical object (e.g., a washer, a screw, or the like) is made of a material of interest (e.g., respectively, black rubber, chrome plated stainless steel, or the like). In operation 810, this material is placed into a physical scene (e.g., on a laboratory benchtop). In operation 830, a physical illumination source 704, such as an LED lamp or a fluorescent lamp is placed in the scene and arranged to illuminate at least a portion of the surface 702. For example, as shown in FIG. 7, ray 706 emitted from the physical illumination source 704 is incident on a particular point 708 of the surface 702 at an incident angle α at a particular point 708 on the surface 702 with respect to the normal direction 714 of the surface 702 at that particular point 708.


In operation 850, an imaging system is used to capture images of the surface 702 of the object from multiple poses with respect to the normal direction of the surface. In the embodiment shown in FIG. 7, a polarization camera system 710 is used as the imaging system to capture images of the surface 702, including the portions illuminated by the physical illumination source 704 (e.g., including the particular point 708). The polarization camera system 710 captures images the surface 702 from different poses 712, such as by moving the polarization camera system 710 from one pose to the next, and capturing polarization raw frames from each pose. In the embodiment shown in FIG. 7, the polarization camera system 710 images the surface 702 at a fronto-parallel observer angle β of 0° in first pose 712A (e.g., a fronto-parallel view from directly above or aligned with the surface normal 714 at the point 708), at an intermediate observer angle β such as an angle of 45° with respect to the surface normal 714 in second pose 712B, and at a shallow observer angle β (e.g., slightly less than 90°, such as 89°) with respect to the surface normal 714 in third pose 712C.


As discussed above, a polarization camera system 710 is generally configured to capture polarization raw frames with polarization filters at different angles (e.g., with a polarization mosaic having four different angles of polarization in the optical path of a single lens and sensor system, with an array of four cameras, each of the cameras having a linear polarization filter at a different angle, with a polarizing filter set at a different angle for different frames captured at different times from the same pose, or the like).


In operation 870, the images captured by the imaging system are stored in with the relative poses of the camera with respect to the normal direction of the surface (e.g., the observer angle β). For example, the observer angle may be stored in the metadata associated with the images and/or the images may be indexed, in part, based on the observer angle β. In some embodiments, the images may be indexed by parameters which include: observer angle β (or angle of camera position with respect to surface normal), material type, and illumination type.


Accordingly, in the arrangement shown in FIG. 7 and using, for example, the method of FIG. 8, the polarization camera system 710 captures multiple images (e.g., four images at linear polarization angles of 0°, 45°, 90°, and 135°) of the material in given illumination conditions (e.g., where the spectral profile of the physical illumination source 704 is known) at different angles of reflection (e.g., at different poses 712).


Each of these perspectives or poses 712 gives a different polarization signal due to the nature of the physics of polarization. Accordingly, by capturing images of the surface 702 from different observer angles, a model of the BRDF of the material can be estimated based on interpolating between the images captured with the physical illumination source 704 at one or more closest corresponding incident angles α by the camera system at the one or more poses 712 having closest corresponding observer angles β.


While the embodiment of FIG. 7 merely depicts three poses 712 for convenience, embodiments of the present disclosure are not limited thereto and the material may be sampled at higher rates, such as with 5° spacing between adjacent poses, or smaller spacings. For example, in some embodiments, the polarization camera system 712 is configured to operate as a video camera system, where polarization raw frames are captured at a high rate, such as 30 frames per second, 60 frames per second, 120 frames per second, or 240 frames per second, thereby resulting in a high density of images captured at a large number of angles with respect to the surface normal.


Similarly, in some embodiments, the pose of the physical illumination source 704 with respect to the surface 702 is modified, such that rays of light emitted from the physical illumination source 704 are incident on the surface 702 at different angles α, where multiple images of the surface are similarly captured by the polarization camera system 710 from different poses 712.


The sampling rates of the different angles (e.g., the incident angle α and the observer or polarization camera system angle β) can be chosen such that intermediate perspectives can be interpolated (e.g., bilinearly interpolated) without significant loss of realism. In various embodiments of the present disclosure, the spacing of the intervals may depend on physical characteristics of the imaging modality, where some imaging modalities exhibit more angle sensitivity than others, and therefore high accuracy may be possible with fewer poses (spaced more widely apart) for modalities that are less angle-sensitive, whereas modalities having higher angle-sensitivity may use larger numbers of poses (spaced more closely together). For example, in some embodiments, when capturing polarization raw frames for a polarization imaging modality, the poses 712 of the polarization camera system 710 are set at interval angles of approximately five degrees (5°) apart, and the images of the surface 702 may also be captured with the physical illumination source 704 at various positions, similarly spaced at angles of approximately five degrees (5°) apart.


In some circumstances, the appearance of a material under the imaging modality of the empirical model is also dependent on the type of illumination source, such as incandescent lights, fluorescent lights, light emitting diode (LED) bulbs, sunlight, and therefore parameters of the illumination source or illumination sources used to light the real-world scene are included as parameters of the empirical model. In some embodiments, different empirical models are trained for different illumination sources (e.g., one model of a material under natural lighting or sunlight and another model of the material under fluorescent lighting).


Referring back to FIG. 6, in some embodiments, in operation 670 the synthetic data generator 40 sets a virtual background for the scene. In some embodiments, the virtual background is an image captured using the same imaging modality as the modality being simulated by the synthetic data generator 40. For example, in some embodiments, when generating synthetic polarization images, the virtual background is a real image captured using a polarization camera, and when generating synthetic thermal images, the virtual background is a real image captured using a thermal camera. In some embodiments, the virtual background is an image of an environment similar to the environments in which the trained machine learning model is intended to operate (e.g., a manufacturing facility or factory in the case of computer vision systems for manufacturing robots). In some embodiments, the virtual background is randomized, thereby increasing the diversity of the synthetic training data set.


In operation 690, the synthetic data generator 40 renders the 3-D scene based on the specified imaging modality (e.g., polarization, thermal, etc.) using one or more of the empirically derived, modality-specific models of materials. Some aspects of embodiments of the present disclosure relate to rendering images based on an empirical model of a material according to one embodiment of the present disclosure. The empirical model of the material may be developed as discussed above, based on samples collected from images captured of real-world objects made of the material of interest.


Generally, a 3-D computer graphics rendering engine generates 2-D renderings of virtual scenes by computing the color of each pixel in the output image in accordance with the color of a surface of the virtual scene that is depicted by that pixel. For example, in a ray tracing rendering engine, a virtual ray of light is emitted from the virtual camera into the virtual scene (in reverse of the typical path of light in the real world), where the virtual ray of light interacts with the surfaces of 3-D models of objects in the virtual scene. These 3-D models are typically represented using geometric shapes such as meshes of points that define flat surfaces (e.g., triangles), where these surfaces may be assigned materials that describe how the virtual ray of light interacts with the surface, such as reflection, refraction, scattering, dispersion, and other optical effects, as well as a texture that represents the color of the surface (e.g., the texture may be a solid color or may be, for example, a bitmap image that is applied to the surface). The path of each virtual ray of light is followed (or “traced”) through the virtual scene until it reaches a light source in the virtual scene (e.g., a virtual light fixture) and the accumulated modifications of the textures encountered along the path from the camera to the light source are combined with the characteristics of the light source (e.g., color temperature of the light source) to compute the color of the pixel. This general process may be modified as understood by those skilled in the art, such as performing anti-aliasing (or smoothing) by tracing multiple rays through different parts of each pixel and computing the color of the pixel based on a combination (e.g., average) of the different colors computed by tracing the different rays interacting with the scene.



FIG. 9 is a flowchart depicting a method 900 for rendering a portion of a virtual object based on the empirical model of a material according to one embodiment of the present disclosure. In particular, FIG. 9 describes one embodiment relating to computing a color when tracing of one ray through one pixel of a virtual scene as the ray interacts with a surface having a material modeled according to one embodiment of the present disclosure. However, a person having ordinary skill in the art before the effective filing date of the present application would understand how the technique described herein may be applied as a part of a larger rendering process, where multiple colors are computed for a given pixel of an output image and combined or where a scanline rendering process is used instead of ray tracing.


In more detail, the embodiment of FIG. 9 depicts a method for rendering a surface of an object in a virtual scene based on a view from a virtual camera in the virtual scene, where the surface has a material modeled in accordance with embodiments of the present disclosure. Given that the objects are being rendered synthetically, and the synthetic data generator 40 has access to the ground truth geometry of each object being rendered, the per-pixel normal, material type, and illumination type are all known parameters that appropriately modulate the graphical rendering of the material. During the rendering process, camera rays are traced from the optical center of the virtual camera to each 3-D point on the object that is visible from the camera. Each 3-D point (e.g., having X-Y-Z coordinates) on the object is mapped to a 2-D coordinate (e.g., having U-V coordinates) on the surface of the object. Each U-V coordinate on the surface of the object has its own surface light-field function (e.g., a bi-directional reflectance function or BRDF) represented as a model that is generated based on the images of real materials, as described above, for example, with respect to FIGS. 7 and 8.


In operation 910, the synthetic data generator 40 (e.g., running a 3-D computer graphics rendering engine) determines a normal direction of the given surface (e.g., with respect to a global coordinate system). In operation 930, the synthetic data generator 40 determines the material of the surface of the object as assigned to the surface as part of the design of the virtual scene.


In operation 950, the synthetic data generator 40 determines an observer angle β of the surface, e.g., based on a direction from which the ray arrived at the surface (e.g., if the surface is the first surface reached by the ray from the camera, then the angle from the virtual camera to the surface, otherwise the angle from which the ray arrived at the surface from another surface in the virtual scene). In some embodiments, in operation 950, the incident angle α is also determined, based on the angle at which the ray leaves the surface (e.g., in a direction toward a virtual light source in the scene, due to the reversal of ray directions during ray tracing). In some circumstances, the incident angle α depends on characteristics of the material determined in operation 930, such as whether the material is transparent, reflective, refractive, diffuse (e.g., matte), or combinations thereof.


In operations 970 and 990, the synthetic data generator 40 configures a model of the material based on the observer angle β (and, if applicable, the incident angle α and other conditions, such as the spectral profile or polarization parameters of illumination sources in the scene) and computes a color of the pixel based, in part, on the configured model of the material. The model of the material may be retrieved from a collection or data bank of models of different standard materials (e.g., models materials have been empirically generated based on types of materials expected to be depicted in virtual scenes generated by the synthetic data generator 40 for generating training data for a particular application or usage scenario, such as materials of components used in manufacturing a particular electronic device in the case of computer vision for supporting robotics in manufacturing the electronic device), where the models are generated based on images of real materials captured as described above in accordance with embodiments of the present disclosure. For example, in operation 930, the synthetic data generator 40 may determine that the surface of the object in the virtual scene is made of black rubber, in which case a model of a material generated from captured images of a real surface made of black rubber is loaded and configured in operation 970.


In some circumstances, the virtual scene includes objects having surfaces made of materials that are not represented in the data bank or collection of models of materials. Accordingly, some aspects of embodiments of the present disclosure relate to simulating the appearance of materials that do not have exact or similar matches in the data bank of models of materials by interpolating between the predictions made by different real models. In some embodiments, the existing materials are represented in an embedding space based on a set of parameters characterizing the material. More formally, interpretable material embeddings M, such that F(Mglass, θout, ϕout, x, y) would give the polarized surface light field for glass with observer angle β represented by (θout, ϕout), and at a location (x, y) on the surface (mapped to (u, v) coordinate space on the 3-D surface), and a similar embedding may be performed for another material such as rubber F (Mrubber, θout, ϕout, x, y). This embedding of the materials in embedding space can then be parameterized in an interpretable way using, for example, beta variational autoencoders (VAEs) and then interpolated to generate new materials that are not based directly on empirically collected samples, but, instead, are interpolations between multiple different models that were separately constructed based on their own empirically collected samples. The generation of additional materials in this way further extends the domain randomization of synthetic training data generated in accordance with embodiments of the present disclosure and improves the robustness of deep learning models trained based on this synthetic data.


Various embodiments of the present disclosure relate to different ways the model of the material may be implemented.


In various embodiments of the present disclosure, the model representing the surface-light field function or BRDF of the material is represented using, for example, a deep learning based BRDF function (e.g., based on a deep neural network such as a convolutional neural network), a mathematically modeled BRDF function (e.g., a set of one or more closed-form equations or one or more open-form equations that can be solved numerically), or a data-driven BRDF function that uses linear interpolation.


In operation 970, the synthetic data generator 40 configures a model of the material identified in operation 950 based on the current parameters, such as the incident angle α and the observer angle β. In the case of a data-driven BRDF function using linear interpolation, in operation 970, the synthetic data generator 40 retrieves images of the material identified in operation 950 that are closest in parameter space to the parameters of the current ray. In some embodiments, the materials are indexed (e.g., stored in a database or other data structure) and accessible in accordance with the material type, the illumination type, the incident angle of the light, and the angle of the camera with respect to the surface normal of the material (e.g., the observer angle). However, embodiments of the present disclosure are not limited to the parameters listed above, and other parameters may be used, depending on the characteristics of the imaging modality. For example, for some materials, the incident angle and/or the illumination type may have no effect on the appearance of the material, and therefore these parameters may be omitted and need not be determined as part of method 900.


Accordingly, in the case of a data-driven BRDF function with linear interpolation, in operation 970, the synthetic data generator 40 retrieves one or more images that are closest to the given parameters of the current ray associated with the current pixel being rendered. For example, the observer angle may be at 53° from the surface normal of the surface of the object, and samples of the real-world material may include images captured at observer angles spaced 5° apart, in this example, images captured at 50° and at 55° with respect to the surface normal of the real-world object made of the material of interest. Accordingly, the images of the real-world material that were captured at 50° and 55° would be retrieved (in circumstances where additional parameters are used, these parameters, such as incident angle and illumination type, are further identify particular images to be retrieved).


Continuing the example of a data-driven BRDF function with linear interpolation, operation 990, the synthetic data generator 40 computes a color of the surface for the pixel based on the closest images. In circumstances where there is only one matching image (e.g., if observer angle in the virtual scene matches an observer angle of one of the sampled images), then the sampled image is used directly for computing the color of the surface. In circumstances where there are multiple matching images, the synthetic data generator 40 interpolates the colors of the multiple images. For example, in some embodiments, linear interpolation is used to interpolate between the multiple images. More specifically, if the observer angle is between four different sample images that have different observer angles in the azimuthal angle with respect to the surface normal and polar angle with respect to an incident angle of the illumination source, then bilinear interpolation may be used to interpolate between the four images along the azimuthal and polar directions. As another example, if the appearance of the material is further dependent on incident angle, then further interpolation may be performed based on images captured at different incident angles (along with interpolating between images captured at different observer angles for each of the different incident angles). Accordingly, in operation 990, a color of the surface of the scene is computed for the current pixel based on combining one or more images captured of real-world materials.


In some embodiments of the present disclosure where the model is a deep learning network, a surface light field function of the material is implemented with a model includes training a deep neural network to predict the value of a bi-directional reflectance function directly from a set of parameters. In more detail, the images captured of a real material from a plurality of different poses, as discussed above, for example, with respect to FIGS. 7 and 8, are used to generate training data relating parameters such as observer angle β, incident angle α, spectral properties of the illumination source, and the like, to the observed appearance of a portion of the material (e.g., at the center of the image). As such, in some embodiments, a deep neural network is trained (e.g., applying backpropagation) to estimate a BRDF function based on training data collected from images collected of real materials. In these embodiments, a model is configured in operation 970 by, if there are multiple deep neural networks, selecting a deep neural network from a plurality of deep neural networks associated with the model (e.g., selected based on matching parameters of the virtual scene with parameters of the data used to train the deep neural network, such as parameters of an illumination source) and supplying parameters to the input of the selected deep neural network (or only deep neural network, if there is only one deep neural network associated with the model), such as the observer angle β, the incident angle α, and the like. In operation 990, the synthesized data generator 40 computes the color of the surface of the virtual object from the configured model by forward propagating through the deep neural network to compute a color at the output, where the computed color is the color of the surface of the virtual scene, as predicted by the deep neural network of the configured model.


In some embodiments of the present disclosure where the model is a deep learning network, a surface light field function of the material is implemented with a model includes one or more conditional generative adversarial networks (see, e.g., Goodfellow, Ian, et al. “Generative adversarial nets.” Advances in Neural Information Processing Systems. 2014.). Each conditional generative adversarial network may be trained to generate images of a material based on a random input and one or more conditions, where the conditions include the current parameters of the viewing of a surface (e.g., observer angle incident angle α of each illumination source, polarization states of each illumination source, and material properties of the surface). According to some embodiments, a discriminator is trained in an adversarial manner to determine, based on an input image and a set of conditions associated with the image, whether the input image was a real image captured under the given conditions or generated by the conditional generator conditioned based on the set of conditions. By alternatingly retraining the generator to generate images that can “fool” the discriminator and training the discriminator to discriminate between generated images and real images, the generator is trained to generate realistic images of materials captured under various capture conditions (e.g., at different observer angles), thereby enabling the trained generator to represent the surface light-field function of the material. In some embodiments of the present disclosure, different generative adversarial networks are trained for different conditions for the same material, such as for different types of illumination sources, different polarization states of the illumination sources, and the like. In these embodiments, a model is configured in operation 970 by, if there are multiple conditional generative adversarial networks (GANs) associated with the model, selecting a conditional GAN from a plurality of conditional GANs associated with the model (e.g., selected based on matching parameters of the virtual scene with parameters of the data used to train the deep neural network, such as parameters of an illumination source) and supplying the parameters of the virtual scene as the conditions of the conditional GAN, such as the observer angle β the incident angle α, and the like. In operation 990, the synthesized data generator 40 computes the color of the surface of the virtual object from the configured model by forward propagating through the conditional GAN to compute a color at the output (e.g., a synthesized image of the surface of the object based on the current parameters), where the computed color is the color of the surface of the virtual scene, as generated by the conditional GAN of the configured model.


In some embodiments of the present disclosure, the surface light field function is modeled using a closed-form mathematically derived bidirectional reflectance distribution function (BRDF) configured by the empirically collected samples (e.g., pictures or photographs) of the real material, as captured from different angles, such as in accordance with the method described with respect to FIG. 8. Examples of techniques for configuring a BRDF based on collected pictures or photographs of a material from different angles or poses are described, e.g., in Ramamoorthi, Ravi, and Pat Hanrahan. “A Signal-Processing Framework for Inverse Rendering.” Proceedings of the 28th Annual Conference on Computer Graphics and Interactive Techniques. 2001. and Ramamoorthi, Ravi. A Signal-Processing Framework for Forward and Inverse Rendering. Stanford University, 2002, 52-79. Accordingly, in some embodiments, a closed-form mathematically derived BRDF is configured using empirically collected samples of a real material and included as a component of a material model for modeling multimodal and/or plenoptic characteristics of a material for the computer rendering of multimodal and/or plenoptic images of virtual scenes.


In some embodiments, virtual objects made of multiple materials that are either bi-modal or multimodal would have a similar set of images for each type of material used in the virtual object in question. The appearances of the different materials are then combined in the final rendering of the image (e.g., additively combined in accordance with weights associated with each material in the virtual model). In some embodiments, this same approach of combining multiple materials is applied to multi-layered materials such as transparent coatings on shiny materials, and the like. In some embodiments, multi-layered materials are modeled by separately sampling (e.g., capturing images of) the multi-layered material.


The end effect of the rendering process using an empirical model of materials according to embodiments of the present disclosure is that the final rendering has an emulated polarization signal that is close to the real polarization signal in a real environment. The accuracy of the empirical model in rendering the materials depicted in the virtual environment depends on how closely the conditions of the virtual environment match the conditions under which samples were captured of the real-world material (e.g., how closely the spectral profile of the illumination source in the virtual scene matched the real-world illumination source, how closely the observer angles in the virtual scene matched the observer angles used when performing sampling, and the like).


As noted above, while aspects of embodiments of the present disclosure are described herein in the context of simulating or emulating the appearance of polarization, embodiments of the present disclosure are not limited thereto. The appearance of materials under multimodal imaging modalities and/or plenoptic imaging modalities, such as thermal, thermal with polarization, and the like, can also be captured in accordance with embodiments of the present disclosure. For example, the behavior of materials in a thermal imaging modality (e.g., infrared imaging) can similarly be modeled by capturing images of a material from multiple poses using a thermal camera in an arrangement similar to that shown in FIG. 7 and a method as described in FIG. 8. Based on these captured images, an appearance of a material under thermal imaging can then be simulated in a 3-D rendering engine by retrieving corresponding images and interpolating images, as necessary, in a manner similar to that shown in FIG. 9.


Accordingly, some aspects of embodiments of the present disclosure relate to systems and methods for generating synthetic image data of virtual scenes as they would appear under various imaging modalities such as polarization imaging and thermal imaging, by rendering images of the virtual scenes using empirical models of materials in the virtual scene. In some embodiments, these empirical models may include images captured of real-world objects using one or more imaging modalities such as polarization imaging and thermal imaging. These synthetic image data can then be used to train machine learning models to operate on image data captured by imaging systems using these imaging modalities.


Some aspects of embodiments of the present disclosure relate to generating synthetic data relating to image features that would typically be generated from imaging data. As a specific example, some aspects of embodiments of the present disclosure relate to generating synthetic features or tensors in polarization representation spaces (e.g., in degree of linear polarization or DOLP ρ and angle of linear polarization or AOLP ϕ). As discussed above, shape from polarization (SfP) provides a relationship between the DOLP ρ and the AOLP ϕ and the refractive index (n), azimuth angle (θa) and zenith angle (θz) of the surface normal of an object.


Accordingly, some aspects of embodiments relate to generating a synthetic degree of linear polarization or DOLP ρ and angle of linear polarization or AOLP ϕ for surfaces of a virtual scene that are visible to the virtual camera based on the refractive index n, azimuth angle (θa) and zenith angle (θz) of the surface of the virtual scene, all of which are known parameters of the virtual 3-D scene.



FIG. 10 is a flowchart depicting a method 1000 for computing synthetic features or tensors in polarization representation spaces for a virtual scene according to one embodiment of the present disclosure. In operation 1010, the synthetic data generator 40 renders a normal image (e.g., an image where every pixel corresponds to the direction of the surface normal of the virtual scene at that pixel). The normal vector at each component includes an azimuth angle θa component and a zenith angle θz component. In operation 1030, the synthetic data generator 40 separates the normal vector at each point of the normal image into two components: the azimuth angle θa and the zenith angle θz at that pixel. As noted above, these components can be used to compute an estimate of the DOLP ρ and AOLP ϕ by using the shape from polarization equations (2) and (3) for the diffuse case and equations (4) and (5) for the specular case. To simulate realistic polarization error, in some embodiments of the present disclosure, the synthetic data generator 40 applies a semi-global perturbation to the normal map before applying the polarization equations (e.g., equations (2), (3), (4), and (5)). This perturbation changes the magnitude of the normals while preserving the gradient of the normals. This simulates errors caused by the material properties of the object and their interactions with polarization. In operation 1050, for a given pixel, the synthetic data generator 40 determines the material of the surface of the object based on the parameters of the objects in the virtual scene (e.g., the material associated with the surface at each pixel of the normal map), and the material is used in conjunction with the geometry of the scene, in accordance with 3-D rendering techniques, to determine whether the given pixel is specular dominant. If so, then the synthetic data generator 40 computes the DOLP ρ and AOLP ϕ based on the specular equations (4) and (5) in operation 1092. If not, then the synthetic data generator 40 computes the DOLP ρ and AOLP ϕ based on the diffuse equations (2) and (3) in operation 1094.


In some embodiments, it is assumed that all of the surfaces are diffuse, and therefore operations 1050 and 1070 can be omitted and the synthetic DOLP ρ and AOLP are computed based on the shape from polarization equations (2) and (3) for the diffuse case.


In some embodiments, the synthesized DOLP ρ and AOLP ϕ data are rendered into color images by applying a colormap such as the “viridis” colormap or the “Jet” colormap (see, e.g., Liu, Yang, and Jeffrey Heer. “Somewhere over the rainbow: An empirical assessment of quantitative colormaps.” Proceedings of the 2018 CHI Conference on Human Factors in Computing Systems. 2018.). These color mapped versions of the synthesized tensors in polarization space may be more easily supplied as input for retraining a pre-trained machine learning model such as convolutional neural network. In some embodiments, when synthesizing DOLP ρ and AOLP ϕ data, random colormaps are applied to the various synthesized data such that the synthesized training data set includes color images representing DOLP ρ and AOLP ϕ data in a variety of different colormaps, such that, at inference time, the network will be able to perform predictions without regard to the particular colormap used to encode the real DOLP ρ and AOLP data. In other embodiments of the present disclosure, the same colormap is applied to all of the synthetic DOLP ρ and AOLP ϕ data (or a first colormap is used for DOLP ρ and a second, different colormap is used for AOLP ϕ), and at inference time, colormaps are applied to the extracted tensors in polarization representation space to match the synthetic training data (e.g., the same first colormap is used for encoding the DOLP ρ extracted from the captured real polarization raw frames and the same second colormap is used for encoding AOLP ϕ extracted from the captured real polarization raw frames).


Accordingly, some aspects of embodiments of the present disclosure relate to synthesizing features in representation spaces specific to particular imaging modalities, such by synthesizing DOLP ρ and AOLP ϕ in polarization representation spaces for a polarization imaging modality.


Some aspects of embodiments of the present disclosure relate to combinations of the above techniques for generating synthetic images for training machine learning models. FIG. 11 is a flowchart depicting a method for generating a training data set according to one embodiment of the present disclosure. One or more virtual scenes representative of the target domain may be generated as discussed above (e.g., for generating images of bins of components, by selecting one or more 3-D models of components and dropping instances of the 3-D models into a container). For example, some aspects of embodiments of the present disclosure relate to forming a training data set based on: (1) images generated purely by domain randomization in operation 1110, (2) images generated purely through texture mapping (e.g., generated in accordance with embodiments of FIG. 9) in operation 1112, and (3) images generated purely through normal mapping (e.g., generated in accordance with embodiments of FIG. 10) in operation 1114.


In addition, the training data set may include images generated using models of materials generated by interpolating between different empirically generated models, as parameterized in embedding space, as discussed above.


In some embodiments of the present disclosure, the images generated in accordance with (1) domain randomization, (2) texture mapping, and (3) normal mapping are further processed by applying style transfer or other filter to the generated image in operations 1120, 1122, and 1124, respectively, before adding the image to the training data set. Applying style transfer causes images that appear somewhat different, as generated using the three techniques described above, to have a more consistent appearance. In some embodiments, the style transfer process transforms the synthesized input images to appear more similar to an image captured based on the imaging modality of interest (e.g., causing images generated using (1) domain randomization and feature maps generated using (3) normal mapping to appear more like polarization raw frames) or by causing the synthesized input images to appear more artificial, such as by applying an unrealistic painterly style to the input images (e.g., causing images generated using (1) domain randomization, (2) renderings using texture mapping, and feature maps generated using (3) normal mapping to appear like a painting made with a paintbrush on canvas).


In some embodiments, a neural style transfer network is trained and used to perform the style transfer in operation 1122 on the images selected for the training data set, such as SytleGAN (see, e.g., Karras, Tero, et al. “Analyzing and improving the image quality of stylegan.” Proceedings of the IEEE/CVF Conference on Computer Vision and Pattern Recognition. 2020.) for complex global style transfers; patched based networks (see, e.g., Chen, Tian Qi, and Mark Schmidt. “Fast patch-based style transfer of arbitrary style.” arXiv preprint arXiv:1612.04337 (2016).) for local style transfers; and networks using domain adaptation (see, e.g., Dundar, Aysegul, et al. “Domain stylization: A strong, simple baseline for synthetic to real image domain adaptation.” arXiv preprint arXiv:1807.09384 (2018).). As a result, all of the images in the training data set may have a similar style or appearance regardless of the method by which the images were obtained (e.g., whether through (1) domain randomization, (2) texture mapping, (3) normal mapping, or other sources such as real images of objects as captured using an imaging system implementing the modality of interest, such as polarization imaging or thermal imaging), as transformed by a style transfer operation.


In some embodiments of the present disclosure, the images for the training data set are sampled from the synthesized data sets (1), (2), and (3) based on hard example mining (see, e.g., Smirnov, Evgeny, et al. “Hard example mining with auxiliary embeddings.” Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition Workshops. 2018.) Using hard example mining to sample the synthesized data sets can improve the efficiency of the training process by reducing the size of the training set to remove substantially redundant images that would not have much impact on the training process while keeping the “hard examples” that have more of an impact on the resulting trained model.


As briefly mentioned above, when generating training data for supervised learning, the synthetic data generator 40 also automatically generates labels (e.g., desired outputs) for the synthesized images. For example, when generating training data for training a machine learning model to perform an image classification task, the generated label for a given image may include the classes of the objects depicted in the image. These classification label may be generated by identifying each unique type of object that is visible in the virtual scene. As another example, when generating training data for training a machine learning model to perform an instance segmentation task, the generated label may include a segmentation map where each instance of each object is uniquely identified (e.g., with a different instance identifier) along with its class (e.g., where objects of the same type have the same class identifier). For example, a segmentation map may be generated by tracing rays from the camera into the virtual scene, where each ray may intersect with some first surface of the virtual scene. Each pixel of the segmentation map is labeled accordingly based on the instance identifier and class identifier of the object containing the surface that was struck by the ray emitted from the camera through the pixel.


As discussed above, and referring to FIG. 1 the resulting training data set of synthesized data 42 generated by the synthetic data generator 40 is then used as training data 5 by a model training system 7 to train a model 30, such as a pre-trained model or a model initialized with random parameters, to produce a trained model 32. Continuing the example presented above in the case of generating training data in accordance with a polarization imaging modality, the training data set 5 may be used to train the model 30 to operate on polarization input features such as polarization raw frames (e.g., the images generated through texture mapping) and tensors in polarization representation spaces (e.g., images generated through normal mapping).


Accordingly, the training data 5 including the synthesized data 42 is used to train or retrain a machine learning model 30 to perform a computer vision task based on a particular imaging modality. For example, synthetic data in accordance with a polarization imaging modality may be used to retrain a convolutional neural network that may have been pre-trained to perform instance segmentation based on standard color images to perform instance segmentation based on polarization input features.


In deployment, a trained model 32 trained based on training data generated in accordance with embodiments of the present disclosure is then configured to take input similar to the training data such as polarization raw frames and/or tensors in polarization representation spaces (where these input images are further modified by the same style transfer, if any, that was applied when generating the training data) to generate predicted outputs such as segmentation maps.


While some embodiments of the present disclosure are described herein with respect to a polarization imaging modality, embodiments of the present disclosure are not limited thereto and include with multimodal imaging modalities and/or plenoptic imaging modalities such as thermal imaging, thermal imaging with polarization (e.g., with a polarizing filter), and ultraviolet imaging. In these embodiments using different modalities, real-world image samples captured from real-world materials using imaging systems implementing those modalities are used to generate models of materials as they would appear under those imaging modalities, and the surface light field functions of the materials with respect to those modalities are modeled as described above (e.g., using a deep neural network, a generative network, linear interpolation, explicit mathematical model, or the like) and used to render images in accordance with those modalities using a 3-D rendering engine. The rendered images in the modality may then be used to train or retrain one or more machine learning models, such as convolutional neural networks, to perform computer vision tasks based on input images captured using those modalities.


As such, aspects of embodiments of the present disclosure relate to systems and methods for generating simulated or synthetic data representative of image data captured by imaging systems using a variety of different imaging modalities such as polarization, thermal, ultraviolet, and combinations thereof. The simulated or synthetic data can be used to as a training data set and/or to augment a training data set for training a machine learning model to perform tasks, such as computer vision tasks, on data captured using an imaging modality corresponding to the imaging modality of the simulated or synthetic data.


While the present invention has been described in connection with certain exemplary embodiments, it is to be understood that the invention is not limited to the disclosed embodiments, but, on the contrary, is intended to cover various modifications and equivalent arrangements included within the spirit and scope of the appended claims, and equivalents thereof.


In some embodiments of the present disclosure, the order in which operations are performed may differ from those as depicted in the figures and as described herein. For example, For example, while FIG. 6 depicts one example of a method for generating synthetic images, embodiments of the present disclosure are not limited thereto. For example, some of the operations shown in FIG. 6 may be performed in a different order, or may be performed concurrently. As specific examples, in various embodiments of the present disclosure, the operations of placing 3-D models of objects in a virtual scene 610, adding lighting to the virtual scene 630, applying modality-specific materials to objects in the virtual scene 650, and setting the scene background 670 may be performed in various orders before rendering the 3-D scene based on a specified imaging modality in operation 690. As another example, while FIG. 8 depicts an embodiment in which lighting is placed in a real-world scene after placing a real-world object into a scene, embodiments of the present disclosure are not limited thereto and lighting may be added to a scene before placing real-world objects in the scene.


In some embodiments of the present disclosure, some operations may be omitted or not performed, and in some embodiments, additional operations not described herein may be performed before, after, or between various operations described herein.

Claims
  • 1. A computer-implemented method comprising: obtaining, by a synthetic data generator, a three-dimensional (3-D) model of an object in a 3-D virtual scene;adding, by the synthetic data generator, lighting to the 3-D virtual scene, the lighting comprising one or more virtual illumination sources;obtaining a model that emulates polarization properties of objects having a particular surface material;determining an observer angle of the object in the virtual scene,generating, by the synthetic data generator, a degree-of-linear-polarization (DOLP) image and an angle-of-linear-polarization (AOLP) image from the observer angle for the object having the particular surface material, including: providing the observer angle as input to the empirical model to generate data representing a respective polarization signal for the particular surface material at each location in the scene corresponding to the object, andcomputing the DOLP image and the AOLP image from the data representing the respective polarization signals at each location in the scene corresponding to the object; andtraining a machine learning model using the generated DOLP image and AOLP image generated by the synthetic data generator.
  • 2. The method of claim 1, wherein the empirical model is generated based on sampled images captured of a surface of the material using an imaging system configured to capture polarization signals, and wherein the sampled images comprise images captured of the surface of the material from a plurality of different poses with respect to a normal direction of the surface of the material.
  • 3. The method of claim 2, wherein the imaging system comprises a polarization camera.
  • 4. The method of claim 2, wherein each of the sampled images is stored in association with the corresponding angle of its pose with respect to the normal direction of the surface of the material.
  • 5. The method of claim 2, wherein the sampled images comprise: a first plurality of sampled images captured of the surface of the material illuminated by light having a first spectral profile; anda second plurality of sampled images captured of the surface of the material illuminated by light having a second spectral profile different from the first spectral profile.
  • 6. The method of claim 2, wherein the empirical model comprises a surface light field function computed by interpolating between two or more of the sampled images.
  • 7. The method of claim 2, wherein the empirical model comprises a surface light field function implemented by a deep neural network trained on the sampled images.
  • 8. The method of claim 2, wherein the empirical model comprises a surface light field function implemented by a generative adversarial network trained on the sampled images.
  • 9. The method of claim 2, wherein the empirical model comprises a surface light field function implemented by a mathematical model generated based on the sampled images.
  • 10. A system for generating synthetic images of virtual scenes comprising: one or more computers; andmemory storing instructions that, when executed by the one or more computers, cause the one or more computers to perform operations comprising:obtaining, by a synthetic data generator, a three-dimensional (3-D) model of an object in a 3-D virtual scene;adding, by the synthetic data generator, lighting to the 3-D virtual scene, the lighting comprising one or more virtual illumination sources;obtaining a model that emulates polarization properties of objects having a particular surface material;determining an observer angle of the object in the virtual scene,generating, by the synthetic data generator, a degree-of-linear-polarization (DOLP) image and an angle-of-linear-polarization (AOLP) image from the observer angle for the object having the particular surface material, including: providing the observer angle as input to the empirical model to generate data representing a respective polarization signal for the particular surface material at each location in the scene corresponding to the object, andcomputing the DOLP image and the AOLP image from the data representing the respective polarization signals at each location in the scene corresponding to the object; andtraining a machine learning model using the generated DOLP image and AOLP image generated by the synthetic data generator.
  • 11. The system of claim 10, wherein the empirical model is generated based on sampled images captured of a surface of the material using an imaging system configured to capture polarization signals, and wherein the sampled images comprise images captured of the surface of the material from a plurality of different poses with respect to a normal direction of the surface of the material.
  • 12. The system of claim 11, wherein the imaging system comprises a polarization camera.
  • 13. The system of claim 11, wherein each of the sampled images is stored in association with the corresponding angle of its pose with respect to the normal direction of the surface of the material.
  • 14. The system of claim 11, wherein the sampled images comprise: a first plurality of sampled images captured of the surface of the material illuminated by light having a first spectral profile; anda second plurality of sampled images captured of the surface of the material illuminated by light having a second spectral profile different from the first spectral profile.
  • 15. The system of claim 11, wherein the empirical model comprises a surface light field function computed by interpolating between two or more of the sampled images.
  • 16. The system of claim 11, wherein the empirical model comprises a surface light field function implemented by a deep neural network trained on the sampled images.
  • 17. The system of claim 11, wherein the empirical model comprises a surface light field function implemented by a generative adversarial network trained on the sampled images.
  • 18. The system of claim 11, wherein the empirical model comprises a surface light field function implemented by a mathematical model generated based on the sampled images.
  • 19. One or more non-transitory computer storage media encoded with computer program instructions that when executed by one or more computers cause the one or more computers to perform operations comprising: obtaining, by a synthetic data generator, a three-dimensional (3-D) model of an object in a 3-D virtual scene;adding, by the synthetic data generator, lighting to the 3-D virtual scene, the lighting comprising one or more virtual illumination sources;obtaining a model that emulates polarization properties of objects having a particular surface material;determining an observer angle of the object in the virtual scene,generating, by the synthetic data generator, a degree-of-linear-polarization (DOLP) image and an angle-of-linear-polarization (AOLP) image from the observer angle for the object having the particular surface material, including: providing the observer angle as input to the empirical model to generate data representing a respective polarization signal for the particular surface material at each location in the scene corresponding to the object, andcomputing the DOLP image and the AOLP image from the data representing the respective polarization signals at each location in the scene corresponding to the object; andtraining a machine learning model using the generated DOLP image and AOLP image generated by the synthetic data generator.
  • 20. The one or more computer storage media of claim 19, wherein the empirical model is generated based on sampled images captured of a surface of the material using an imaging system configured to capture polarization signals, and wherein the sampled images comprise images captured of the surface of the material from a plurality of different poses with respect to a normal direction of the surface of the material.
  • 21. The one or more computer storage media of claim 20, wherein the imaging system comprises a polarization camera.
  • 22. The one or more computer storage media of claim 20, wherein each of the sampled images is stored in association with the corresponding angle of its pose with respect to the normal direction of the surface of the material.
  • 23. The one or more computer storage media of claim 20, wherein the sampled images comprise: a first plurality of sampled images captured of the surface of the material illuminated by light having a first spectral profile; anda second plurality of sampled images captured of the surface of the material illuminated by light having a second spectral profile different from the first spectral profile.
  • 24. The one or more computer storage media of claim 20, wherein the empirical model comprises a surface light field function computed by interpolating between two or more of the sampled images.
  • 25. The one or more computer storage media of claim 20, wherein the empirical model comprises a surface light field function implemented by a deep neural network trained on the sampled images.
  • 26. The one or more computer storage media of claim 20, wherein the empirical model comprises a surface light field function implemented by a generative adversarial network trained on the sampled images.
  • 27. The one or more computer storage media of claim 20, wherein the empirical model comprises a surface light field function implemented by a mathematical model generated based on the sampled images.
CROSS-REFERENCE TO RELATED APPLICATION(S)

This application is a U.S. National Phase Patent Application of International Application Number PCT/US2021/012073 filed on Jan. 4, 2021, which claims priority to and the benefit of U.S. Provisional Patent Application No. 62/968,038, filed in the United States Patent and Trademark Office on Jan. 30, 2020, the entire disclosure of each of which is incorporated by reference herein.

PCT Information
Filing Document Filing Date Country Kind
PCT/US2021/012073 1/4/2021 WO
Publishing Document Publishing Date Country Kind
WO2021/154459 8/5/2021 WO A
US Referenced Citations (1283)
Number Name Date Kind
4124798 Thompson Nov 1978 A
4198646 Alexander et al. Apr 1980 A
4323925 Abell et al. Apr 1982 A
4460449 Montalbano Jul 1984 A
4467365 Murayama et al. Aug 1984 A
4652909 Glenn Mar 1987 A
4888645 Mitchell et al. Dec 1989 A
4899060 Lischke Feb 1990 A
4962425 Rea Oct 1990 A
5005083 Grage et al. Apr 1991 A
5070414 Tsutsumi Dec 1991 A
5144448 Hornbaker et al. Sep 1992 A
5157499 Oguma et al. Oct 1992 A
5325449 Burt et al. Jun 1994 A
5327125 Iwase et al. Jul 1994 A
5463464 Ladewski Oct 1995 A
5475422 Suzuki et al. Dec 1995 A
5488674 Burt et al. Jan 1996 A
5517236 Sergeant et al. May 1996 A
5629524 Stettner et al. May 1997 A
5638461 Fridge Jun 1997 A
5675377 Gibas et al. Oct 1997 A
5703961 Rogina et al. Dec 1997 A
5710875 Hsu et al. Jan 1998 A
5757425 Barton et al. May 1998 A
5793900 Nourbakhsh et al. Aug 1998 A
5801919 Griencewic Sep 1998 A
5808350 Jack et al. Sep 1998 A
5832312 Rieger et al. Nov 1998 A
5833507 Woodgate et al. Nov 1998 A
5880691 Fossum et al. Mar 1999 A
5911008 Niikura et al. Jun 1999 A
5933190 Dierickx et al. Aug 1999 A
5963664 Kumar et al. Oct 1999 A
5973844 Burger Oct 1999 A
6002743 Telymonde Dec 1999 A
6005607 Uomori et al. Dec 1999 A
6034690 Gallery et al. Mar 2000 A
6069351 Mack May 2000 A
6069365 Chow et al. May 2000 A
6084979 Kanade et al. Jul 2000 A
6095989 Hay et al. Aug 2000 A
6097394 Levoy et al. Aug 2000 A
6124974 Burger Sep 2000 A
6130786 Osawa et al. Oct 2000 A
6137100 Fossum et al. Oct 2000 A
6137535 Meyers Oct 2000 A
6141048 Meyers Oct 2000 A
6160909 Melen Dec 2000 A
6163414 Kikuchi et al. Dec 2000 A
6172352 Liu Jan 2001 B1
6175379 Uomori et al. Jan 2001 B1
6185529 Chen et al. Feb 2001 B1
6198852 Anandan et al. Mar 2001 B1
6205241 Melen Mar 2001 B1
6239909 Hayashi et al. May 2001 B1
6292713 Jouppi et al. Sep 2001 B1
6340994 Margulis et al. Jan 2002 B1
6358862 Ireland et al. Mar 2002 B1
6373518 Sogawa Apr 2002 B1
6419638 Hay et al. Jul 2002 B1
6443579 Myers Sep 2002 B1
6445815 Sato Sep 2002 B1
6476805 Shum et al. Nov 2002 B1
6477260 Shimomura Nov 2002 B1
6502097 Chan et al. Dec 2002 B1
6525302 Dowski, Jr. et al. Feb 2003 B2
6546153 Hoydal Apr 2003 B1
6552742 Seta Apr 2003 B1
6563537 Kawamura et al. May 2003 B1
6571466 Glenn et al. Jun 2003 B1
6603513 Berezin Aug 2003 B1
6611289 Yu et al. Aug 2003 B1
6627896 Hashimoto et al. Sep 2003 B1
6628330 Lin Sep 2003 B1
6628845 Stone et al. Sep 2003 B1
6635941 Suda Oct 2003 B2
6639596 Shum et al. Oct 2003 B1
6647142 Beardsley Nov 2003 B1
6657218 Noda Dec 2003 B2
6671399 Berestov Dec 2003 B1
6674892 Melen Jan 2004 B1
6750488 Driescher et al. Jun 2004 B1
6750904 Lambert Jun 2004 B1
6765617 Tangen et al. Jul 2004 B1
6771833 Edgar Aug 2004 B1
6774941 Boisvert et al. Aug 2004 B1
6788338 Dinev et al. Sep 2004 B1
6795253 Shinohara Sep 2004 B2
6801653 Wu et al. Oct 2004 B1
6819328 Moriwaki et al. Nov 2004 B1
6819358 Kagle et al. Nov 2004 B1
6833863 Clemens Dec 2004 B1
6879735 Portniaguine et al. Apr 2005 B1
6897454 Sasaki et al. May 2005 B2
6903770 Kobayashi et al. Jun 2005 B1
6909121 Nishikawa Jun 2005 B2
6917702 Beardsley Jul 2005 B2
6927922 George et al. Aug 2005 B2
6958862 Joseph Oct 2005 B1
6985175 Iwai et al. Jan 2006 B2
7013318 Rosengard et al. Mar 2006 B2
7015954 Foote et al. Mar 2006 B1
7085409 Sawhney et al. Aug 2006 B2
7161614 Yamashita et al. Jan 2007 B1
7199348 Olsen et al. Apr 2007 B2
7206449 Raskar et al. Apr 2007 B2
7215364 Wachtel et al. May 2007 B2
7235785 Hornback et al. Jun 2007 B2
7245761 Swaminathan et al. Jul 2007 B2
7262799 Suda Aug 2007 B2
7292735 Blake et al. Nov 2007 B2
7295697 Satoh Nov 2007 B1
7333651 Kim et al. Feb 2008 B1
7369165 Bosco et al. May 2008 B2
7391572 Jacobowitz et al. Jun 2008 B2
7408725 Sato Aug 2008 B2
7425984 Chen et al. Sep 2008 B2
7430312 Gu Sep 2008 B2
7471765 Jaffray et al. Dec 2008 B2
7496293 Shamir et al. Feb 2009 B2
7564019 Olsen et al. Jul 2009 B2
7599547 Sun et al. Oct 2009 B2
7606484 Richards et al. Oct 2009 B1
7620265 Wolff et al. Nov 2009 B1
7633511 Shum et al. Dec 2009 B2
7639435 Chiang Dec 2009 B2
7639838 Nims Dec 2009 B2
7646549 Zalevsky et al. Jan 2010 B2
7657090 Omatsu et al. Feb 2010 B2
7667824 Moran Feb 2010 B1
7675080 Boettiger Mar 2010 B2
7675681 Tomikawa et al. Mar 2010 B2
7706634 Schmitt et al. Apr 2010 B2
7723662 Levoy et al. May 2010 B2
7738013 Galambos et al. Jun 2010 B2
7741620 Doering et al. Jun 2010 B2
7782364 Smith Aug 2010 B2
7826153 Hong Nov 2010 B2
7840067 Shen et al. Nov 2010 B2
7912673 Hébert et al. Mar 2011 B2
7924321 Nayar et al. Apr 2011 B2
7956871 Fainstain et al. Jun 2011 B2
7965314 Miller et al. Jun 2011 B1
7973834 Yang Jul 2011 B2
7986018 Rennie Jul 2011 B2
7990447 Honda et al. Aug 2011 B2
8000498 Shih et al. Aug 2011 B2
8013904 Tan et al. Sep 2011 B2
8027531 Wilburn et al. Sep 2011 B2
8044994 Vetro et al. Oct 2011 B2
8055466 Bryll Nov 2011 B2
8077245 Adamo et al. Dec 2011 B2
8089515 Chebil et al. Jan 2012 B2
8098297 Crisan et al. Jan 2012 B2
8098304 Pinto et al. Jan 2012 B2
8106949 Tan et al. Jan 2012 B2
8111910 Tanaka Feb 2012 B2
8126279 Marcellin et al. Feb 2012 B2
8130120 Kawabata et al. Mar 2012 B2
8131097 Lelescu et al. Mar 2012 B2
8149323 Li et al. Apr 2012 B2
8164629 Zhang Apr 2012 B1
8169486 Corcoran et al. May 2012 B2
8180145 Wu et al. May 2012 B2
8189065 Georgiev et al. May 2012 B2
8189089 Georgiev et al. May 2012 B1
8194296 Compton et al. Jun 2012 B2
8212914 Chiu Jul 2012 B2
8213711 Tam Jul 2012 B2
8231814 Duparre Jul 2012 B2
8242426 Ward et al. Aug 2012 B2
8244027 Takahashi Aug 2012 B2
8244058 Intwala et al. Aug 2012 B1
8254668 Mashitani et al. Aug 2012 B2
8279325 Pitts et al. Oct 2012 B2
8280194 Wong et al. Oct 2012 B2
8284240 Saint-Pierre et al. Oct 2012 B2
8289409 Chang Oct 2012 B2
8289440 Pitts et al. Oct 2012 B2
8290358 Georgiev Oct 2012 B1
8294099 Blackwell, Jr. Oct 2012 B2
8294754 Jung et al. Oct 2012 B2
8300085 Yang et al. Oct 2012 B2
8305456 McMahon Nov 2012 B1
8315476 Georgiev et al. Nov 2012 B1
8345144 Georgiev et al. Jan 2013 B1
8360574 Ishak et al. Jan 2013 B2
8400555 Georgiev et al. Mar 2013 B1
8406562 Bassi et al. Mar 2013 B2
8411146 Twede Apr 2013 B2
8416282 Lablans Apr 2013 B2
8446492 Nakano et al. May 2013 B2
8456517 Spektor et al. Jun 2013 B2
8493496 Freedman et al. Jul 2013 B2
8514291 Chang Aug 2013 B2
8514491 Duparre Aug 2013 B2
8541730 Inuiya Sep 2013 B2
8542933 Venkataraman et al. Sep 2013 B2
8553093 Wong et al. Oct 2013 B2
8558929 Tredwell Oct 2013 B2
8559705 Ng Oct 2013 B2
8559756 Georgiev et al. Oct 2013 B2
8565547 Strandemar Oct 2013 B2
8576302 Yoshikawa Nov 2013 B2
8577183 Robinson Nov 2013 B2
8581995 Lin et al. Nov 2013 B2
8619082 Ciurea et al. Dec 2013 B1
8648918 Kauker et al. Feb 2014 B2
8648919 Mantzel et al. Feb 2014 B2
8655052 Spooner et al. Feb 2014 B2
8682107 Yoon et al. Mar 2014 B2
8687087 Pertsel et al. Apr 2014 B2
8692893 McMahon Apr 2014 B2
8754941 Sarwari et al. Jun 2014 B1
8773536 Zhang Jul 2014 B1
8780113 Ciurea et al. Jul 2014 B1
8787691 Takahashi et al. Jul 2014 B2
8792710 Keselman Jul 2014 B2
8804255 Duparre Aug 2014 B2
8823813 Mantzel et al. Sep 2014 B2
8830375 Ludwig Sep 2014 B2
8831367 Venkataraman et al. Sep 2014 B2
8831377 Pitts et al. Sep 2014 B2
8836793 Kriesel et al. Sep 2014 B1
8842201 Tajiri Sep 2014 B2
8854433 Rafii Oct 2014 B1
8854462 Herbin et al. Oct 2014 B2
8861089 Duparre Oct 2014 B2
8866912 Mullis Oct 2014 B2
8866920 Venkataraman et al. Oct 2014 B2
8866951 Keelan Oct 2014 B2
8878950 Lelescu et al. Nov 2014 B2
8885059 Venkataraman et al. Nov 2014 B1
8885922 Ito et al. Nov 2014 B2
8896594 Xiong et al. Nov 2014 B2
8896719 Venkataraman et al. Nov 2014 B1
8902321 Venkataraman et al. Dec 2014 B2
8928793 McMahon Jan 2015 B2
8977038 Tian et al. Mar 2015 B2
9001226 Ng et al. Apr 2015 B1
9019426 Han et al. Apr 2015 B2
9025894 Venkataraman et al. May 2015 B2
9025895 Venkataraman et al. May 2015 B2
9030528 Pesach et al. May 2015 B2
9031335 Venkataraman et al. May 2015 B2
9031342 Venkataraman May 2015 B2
9031343 Venkataraman May 2015 B2
9036928 Venkataraman May 2015 B2
9036931 Venkataraman et al. May 2015 B2
9041823 Venkataraman et al. May 2015 B2
9041824 Lelescu et al. May 2015 B2
9041829 Venkataraman et al. May 2015 B2
9042667 Venkataraman et al. May 2015 B2
9047684 Lelescu et al. Jun 2015 B2
9049367 Venkataraman et al. Jun 2015 B2
9055233 Venkataraman et al. Jun 2015 B2
9060120 Venkataraman et al. Jun 2015 B2
9060124 Venkataraman et al. Jun 2015 B2
9077893 Venkataraman et al. Jul 2015 B2
9094661 Venkataraman et al. Jul 2015 B2
9100586 McMahon et al. Aug 2015 B2
9100635 Duparre et al. Aug 2015 B2
9123117 Ciurea et al. Sep 2015 B2
9123118 Ciurea et al. Sep 2015 B2
9124815 Venkataraman et al. Sep 2015 B2
9124831 Mullis Sep 2015 B2
9124864 Mullis Sep 2015 B2
9128228 Duparre Sep 2015 B2
9129183 Venkataraman et al. Sep 2015 B2
9129377 Ciurea et al. Sep 2015 B2
9143711 McMahon Sep 2015 B2
9147254 Florian et al. Sep 2015 B2
9185276 Rodda et al. Nov 2015 B2
9188765 Venkataraman et al. Nov 2015 B2
9191580 Venkataraman et al. Nov 2015 B2
9197821 McMahon Nov 2015 B2
9210392 Nisenzon et al. Dec 2015 B2
9214013 Venkataraman et al. Dec 2015 B2
9235898 Venkataraman et al. Jan 2016 B2
9235900 Ciurea et al. Jan 2016 B2
9240049 Ciurea et al. Jan 2016 B2
9247117 Jacques Jan 2016 B2
9253380 Venkataraman et al. Feb 2016 B2
9253397 Lee et al. Feb 2016 B2
9256974 Hines Feb 2016 B1
9264592 Rodda et al. Feb 2016 B2
9264610 Duparre Feb 2016 B2
9361662 Lelescu et al. Jun 2016 B2
9374512 Venkataraman et al. Jun 2016 B2
9412206 McMahon et al. Aug 2016 B2
9413953 Maeda Aug 2016 B2
9426343 Rodda et al. Aug 2016 B2
9426361 Venkataraman et al. Aug 2016 B2
9438888 Venkataraman et al. Sep 2016 B2
9445003 Lelescu et al. Sep 2016 B1
9456134 Venkataraman et al. Sep 2016 B2
9456196 Kim et al. Sep 2016 B2
9462164 Venkataraman et al. Oct 2016 B2
9485496 Venkataraman et al. Nov 2016 B2
9497370 Venkataraman et al. Nov 2016 B2
9497429 Mullis et al. Nov 2016 B2
9516222 Duparre et al. Dec 2016 B2
9519972 Venkataraman et al. Dec 2016 B2
9521319 Rodda et al. Dec 2016 B2
9521416 McMahon et al. Dec 2016 B1
9536166 Venkataraman et al. Jan 2017 B2
9576369 Venkataraman et al. Feb 2017 B2
9578237 Duparre et al. Feb 2017 B2
9578259 Molina Feb 2017 B2
9602805 Venkataraman et al. Mar 2017 B2
9633442 Venkataraman et al. Apr 2017 B2
9635274 Lin et al. Apr 2017 B2
9638883 Duparre May 2017 B1
9661310 Deng et al. May 2017 B2
9706132 Nisenzon et al. Jul 2017 B2
9712759 Venkataraman et al. Jul 2017 B2
9729865 Kuo et al. Aug 2017 B1
9733486 Lelescu et al. Aug 2017 B2
9741118 Mullis Aug 2017 B2
9743051 Venkataraman et al. Aug 2017 B2
9749547 Venkataraman et al. Aug 2017 B2
9749568 McMahon Aug 2017 B2
9754422 McMahon et al. Sep 2017 B2
9766380 Duparre et al. Sep 2017 B2
9769365 Jannard Sep 2017 B1
9774789 Ciurea et al. Sep 2017 B2
9774831 Venkataraman et al. Sep 2017 B2
9787911 McMahon et al. Oct 2017 B2
9794476 Nayar et al. Oct 2017 B2
9800856 Venkataraman et al. Oct 2017 B2
9800859 Venkataraman et al. Oct 2017 B2
9807382 Duparre et al. Oct 2017 B2
9811753 Venkataraman et al. Nov 2017 B2
9813616 Lelescu et al. Nov 2017 B2
9813617 Venkataraman et al. Nov 2017 B2
9826212 Newton et al. Nov 2017 B2
9858673 Ciurea et al. Jan 2018 B2
9864921 Venkataraman et al. Jan 2018 B2
9866739 McMahon Jan 2018 B2
9888194 Duparre Feb 2018 B2
9892522 Smirnov et al. Feb 2018 B2
9898856 Yang et al. Feb 2018 B2
9917998 Venkataraman et al. Mar 2018 B2
9924092 Rodda et al. Mar 2018 B2
9936148 McMahon Apr 2018 B2
9942474 Venkataraman et al. Apr 2018 B2
9955070 Lelescu et al. Apr 2018 B2
9986224 Mullis May 2018 B2
10009538 Venkataraman et al. Jun 2018 B2
10019816 Venkataraman et al. Jul 2018 B2
10027901 Venkataraman et al. Jul 2018 B2
10089740 Srikanth et al. Oct 2018 B2
10091405 Molina Oct 2018 B2
10119808 Venkataraman et al. Nov 2018 B2
10122993 Venkataraman et al. Nov 2018 B2
10127682 Mullis Nov 2018 B2
10142560 Venkataraman et al. Nov 2018 B2
10182216 Mullis et al. Jan 2019 B2
10218889 McMahan Feb 2019 B2
10225543 Mullis Mar 2019 B2
10250871 Ciurea et al. Apr 2019 B2
10261219 Duparre et al. Apr 2019 B2
10275676 Venkataraman et al. Apr 2019 B2
10306120 Duparre May 2019 B2
10311649 McMohan et al. Jun 2019 B2
10334241 Duparre et al. Jun 2019 B2
10366472 Lelescu et al. Jul 2019 B2
10375302 Nayar et al. Aug 2019 B2
10375319 Venkataraman et al. Aug 2019 B2
10380752 Ciurea et al. Aug 2019 B2
10390005 Nisenzon et al. Aug 2019 B2
10412314 McMahon et al. Sep 2019 B2
10430682 Venkataraman et al. Oct 2019 B2
10455168 McMahon Oct 2019 B2
10455218 Venkataraman et al. Oct 2019 B2
10462362 Lelescu et al. Oct 2019 B2
10482618 Jain et al. Nov 2019 B2
10540806 Yang et al. Jan 2020 B2
10542208 Lelescu et al. Jan 2020 B2
10547772 Molina Jan 2020 B2
10560684 Mullis Feb 2020 B2
10574905 Srikanth et al. Feb 2020 B2
10638099 Mullis et al. Apr 2020 B2
10643383 Venkataraman May 2020 B2
10674138 Venkataraman et al. Jun 2020 B2
10694114 Venkataraman et al. Jun 2020 B2
10708492 Venkataraman et al. Jul 2020 B2
10735635 Duparre Aug 2020 B2
10742861 McMahon Aug 2020 B2
10767981 Venkataraman et al. Sep 2020 B2
10805589 Venkataraman et al. Oct 2020 B2
10818026 Jain et al. Oct 2020 B2
10839485 Lelescu et al. Nov 2020 B2
10909707 Ciurea et al. Feb 2021 B2
10944961 Ciurea et al. Mar 2021 B2
10958892 Mullis Mar 2021 B2
10984276 Venkataraman et al. Apr 2021 B2
11022725 Duparre et al. Jun 2021 B2
11024046 Venkataraman Jun 2021 B2
20010005225 Clark et al. Jun 2001 A1
20010019621 Hanna et al. Sep 2001 A1
20010028038 Hamaguchi et al. Oct 2001 A1
20010038387 Tomooka et al. Nov 2001 A1
20020003669 Kedar et al. Jan 2002 A1
20020012056 Trevino et al. Jan 2002 A1
20020015536 Warren et al. Feb 2002 A1
20020027608 Johnson et al. Mar 2002 A1
20020028014 Ono Mar 2002 A1
20020039438 Mori et al. Apr 2002 A1
20020057845 Fossum et al. May 2002 A1
20020061131 Sawhney et al. May 2002 A1
20020063807 Margulis May 2002 A1
20020075450 Aratani et al. Jun 2002 A1
20020087403 Meyers et al. Jul 2002 A1
20020089596 Yasuo Jul 2002 A1
20020094027 Sato et al. Jul 2002 A1
20020101528 Lee et al. Aug 2002 A1
20020113867 Takigawa et al. Aug 2002 A1
20020113888 Sonoda et al. Aug 2002 A1
20020118113 Oku et al. Aug 2002 A1
20020120634 Min et al. Aug 2002 A1
20020122113 Foote Sep 2002 A1
20020128060 Belhumeur et al. Sep 2002 A1
20020163054 Suda Nov 2002 A1
20020167537 Trajkovic Nov 2002 A1
20020171666 Endo et al. Nov 2002 A1
20020177054 Saitoh et al. Nov 2002 A1
20020190991 Efran et al. Dec 2002 A1
20020195548 Dowski, Jr. et al. Dec 2002 A1
20030025227 Daniell Feb 2003 A1
20030026474 Yano Feb 2003 A1
20030086079 Barth et al. May 2003 A1
20030124763 Fan et al. Jul 2003 A1
20030140347 Varsa Jul 2003 A1
20030156189 Utsumi et al. Aug 2003 A1
20030179418 Wengender et al. Sep 2003 A1
20030188659 Merry et al. Oct 2003 A1
20030190072 Adkins et al. Oct 2003 A1
20030198377 Ng Oct 2003 A1
20030211405 Venkataraman Nov 2003 A1
20030231179 Suzuki Dec 2003 A1
20040003409 Berstis Jan 2004 A1
20040008271 Hagimori et al. Jan 2004 A1
20040012689 Tinnerino et al. Jan 2004 A1
20040027358 Nakao Feb 2004 A1
20040047274 Amanai Mar 2004 A1
20040050104 Ghosh et al. Mar 2004 A1
20040056966 Schechner et al. Mar 2004 A1
20040061787 Liu et al. Apr 2004 A1
20040066454 Otani et al. Apr 2004 A1
20040071367 Irani et al. Apr 2004 A1
20040075654 Hsiao et al. Apr 2004 A1
20040096119 Williams et al. May 2004 A1
20040100570 Shizukuishi May 2004 A1
20040105021 Hu Jun 2004 A1
20040114794 Vlasic Jun 2004 A1
20040114807 Lelescu et al. Jun 2004 A1
20040141659 Zhang Jul 2004 A1
20040151401 Sawhney et al. Aug 2004 A1
20040165090 Ning Aug 2004 A1
20040169617 Yelton et al. Sep 2004 A1
20040170340 Tipping et al. Sep 2004 A1
20040174439 Upton Sep 2004 A1
20040179008 Gordon et al. Sep 2004 A1
20040179834 Szajewski et al. Sep 2004 A1
20040196379 Chen et al. Oct 2004 A1
20040207600 Zhang et al. Oct 2004 A1
20040207836 Chhibber et al. Oct 2004 A1
20040212734 Macinnis et al. Oct 2004 A1
20040213449 Safaee-Rad et al. Oct 2004 A1
20040218809 Blake et al. Nov 2004 A1
20040234873 Venkataraman Nov 2004 A1
20040239782 Equitz et al. Dec 2004 A1
20040239885 Jaynes et al. Dec 2004 A1
20040240052 Minefuji et al. Dec 2004 A1
20040251509 Choi Dec 2004 A1
20040264806 Herley Dec 2004 A1
20050006477 Patel Jan 2005 A1
20050007461 Chou et al. Jan 2005 A1
20050009313 Suzuki et al. Jan 2005 A1
20050010621 Pinto et al. Jan 2005 A1
20050012035 Miller Jan 2005 A1
20050036778 DeMonte Feb 2005 A1
20050047678 Jones et al. Mar 2005 A1
20050048690 Yamamoto Mar 2005 A1
20050068436 Fraenkel et al. Mar 2005 A1
20050083531 Millerd et al. Apr 2005 A1
20050084179 Hanna et al. Apr 2005 A1
20050111705 Waupotitsch et al. May 2005 A1
20050117015 Cutler Jun 2005 A1
20050128509 Tokkonen et al. Jun 2005 A1
20050128595 Shimizu Jun 2005 A1
20050132098 Sonoda et al. Jun 2005 A1
20050134698 Schroeder et al. Jun 2005 A1
20050134699 Nagashima Jun 2005 A1
20050134712 Gruhlke et al. Jun 2005 A1
20050147277 Higaki et al. Jul 2005 A1
20050151759 Gonzalez-Banos et al. Jul 2005 A1
20050168924 Wu et al. Aug 2005 A1
20050175257 Kuroki Aug 2005 A1
20050185711 Pfister et al. Aug 2005 A1
20050203380 Sauer et al. Sep 2005 A1
20050205785 Hornback et al. Sep 2005 A1
20050219264 Shum et al. Oct 2005 A1
20050219363 Kohler et al. Oct 2005 A1
20050224843 Boemler Oct 2005 A1
20050225654 Feldman et al. Oct 2005 A1
20050265633 Piacentino et al. Dec 2005 A1
20050275946 Choo et al. Dec 2005 A1
20050286612 Takanashi Dec 2005 A1
20050286756 Hong et al. Dec 2005 A1
20060002635 Nestares et al. Jan 2006 A1
20060007331 Izumi et al. Jan 2006 A1
20060013318 Webb et al. Jan 2006 A1
20060018509 Miyoshi Jan 2006 A1
20060023197 Joel Feb 2006 A1
20060023314 Boettiger et al. Feb 2006 A1
20060028476 Sobel et al. Feb 2006 A1
20060029270 Berestov et al. Feb 2006 A1
20060029271 Miyoshi et al. Feb 2006 A1
20060033005 Jerdev et al. Feb 2006 A1
20060034003 Zalevsky Feb 2006 A1
20060034531 Poon et al. Feb 2006 A1
20060035415 Wood Feb 2006 A1
20060038891 Okutomi et al. Feb 2006 A1
20060039611 Rother et al. Feb 2006 A1
20060046204 Ono et al. Mar 2006 A1
20060049930 Zruya et al. Mar 2006 A1
20060050980 Kohashi et al. Mar 2006 A1
20060054780 Garrood et al. Mar 2006 A1
20060054782 Olsen et al. Mar 2006 A1
20060055811 Frtiz et al. Mar 2006 A1
20060069478 Iwama Mar 2006 A1
20060072029 Miyatake et al. Apr 2006 A1
20060087747 Ohzawa et al. Apr 2006 A1
20060098888 Morishita May 2006 A1
20060103754 Wenstrand et al. May 2006 A1
20060119597 Oshino Jun 2006 A1
20060125936 Gruhike et al. Jun 2006 A1
20060138322 Costello et al. Jun 2006 A1
20060139475 Esch et al. Jun 2006 A1
20060152803 Provitola Jul 2006 A1
20060153290 Watabe et al. Jul 2006 A1
20060157640 Perlman et al. Jul 2006 A1
20060159369 Young Jul 2006 A1
20060176566 Boettiger et al. Aug 2006 A1
20060187322 Janson et al. Aug 2006 A1
20060187338 May et al. Aug 2006 A1
20060197937 Bamji et al. Sep 2006 A1
20060203100 Ajito et al. Sep 2006 A1
20060203113 Wada et al. Sep 2006 A1
20060210146 Gu Sep 2006 A1
20060210186 Berkner Sep 2006 A1
20060214085 Olsen et al. Sep 2006 A1
20060215924 Steinberg et al. Sep 2006 A1
20060221250 Rossbach et al. Oct 2006 A1
20060239549 Kelly et al. Oct 2006 A1
20060243889 Farnworth et al. Nov 2006 A1
20060251410 Trutna Nov 2006 A1
20060274174 Tewinkle Dec 2006 A1
20060278948 Yamaguchi et al. Dec 2006 A1
20060279648 Senba et al. Dec 2006 A1
20060289772 Johnson et al. Dec 2006 A1
20070002159 Olsen et al. Jan 2007 A1
20070008575 Yu et al. Jan 2007 A1
20070009150 Suwa Jan 2007 A1
20070024614 Tam et al. Feb 2007 A1
20070030356 Yea et al. Feb 2007 A1
20070035707 Margulis Feb 2007 A1
20070036427 Nakamura et al. Feb 2007 A1
20070040828 Zalevsky et al. Feb 2007 A1
20070040922 McKee et al. Feb 2007 A1
20070041391 Lin et al. Feb 2007 A1
20070052825 Cho Mar 2007 A1
20070083114 Yang et al. Apr 2007 A1
20070085917 Kobayashi Apr 2007 A1
20070092245 Bazakos et al. Apr 2007 A1
20070102622 Olsen et al. May 2007 A1
20070116447 Ye May 2007 A1
20070126898 Feldman et al. Jun 2007 A1
20070127831 Venkataraman Jun 2007 A1
20070139333 Sato et al. Jun 2007 A1
20070140685 Wu Jun 2007 A1
20070146503 Shiraki Jun 2007 A1
20070146511 Kinoshita et al. Jun 2007 A1
20070153335 Hosaka Jul 2007 A1
20070158427 Zhu et al. Jul 2007 A1
20070159541 Sparks et al. Jul 2007 A1
20070160310 Tanida et al. Jul 2007 A1
20070165931 Higaki Jul 2007 A1
20070166447 Ur-Rehman et al. Jul 2007 A1
20070171290 Kroger Jul 2007 A1
20070177004 Kolehmainen et al. Aug 2007 A1
20070182843 Shimamura et al. Aug 2007 A1
20070201859 Sarrat Aug 2007 A1
20070206241 Smith et al. Sep 2007 A1
20070211164 Olsen et al. Sep 2007 A1
20070216765 Wong et al. Sep 2007 A1
20070225600 Weibrecht et al. Sep 2007 A1
20070228256 Mentzer et al. Oct 2007 A1
20070236595 Pan et al. Oct 2007 A1
20070242141 Ciurea Oct 2007 A1
20070247517 Zhang et al. Oct 2007 A1
20070257184 Olsen et al. Nov 2007 A1
20070258006 Olsen et al. Nov 2007 A1
20070258706 Raskar et al. Nov 2007 A1
20070263113 Baek et al. Nov 2007 A1
20070263114 Gurevich et al. Nov 2007 A1
20070268374 Robinson Nov 2007 A1
20070291995 Rivera Dec 2007 A1
20070296721 Chang et al. Dec 2007 A1
20070296832 Ota et al. Dec 2007 A1
20070296835 Olsen et al. Dec 2007 A1
20070296846 Barman et al. Dec 2007 A1
20070296847 Chang et al. Dec 2007 A1
20070297696 Hamza et al. Dec 2007 A1
20080006859 Mionetto Jan 2008 A1
20080019611 Larkin et al. Jan 2008 A1
20080024683 Damera-Venkata et al. Jan 2008 A1
20080025649 Liu et al. Jan 2008 A1
20080030592 Border et al. Feb 2008 A1
20080030597 Olsen et al. Feb 2008 A1
20080043095 Vetro et al. Feb 2008 A1
20080043096 Vetro et al. Feb 2008 A1
20080044170 Yap et al. Feb 2008 A1
20080054518 Ra et al. Mar 2008 A1
20080056302 Erdal et al. Mar 2008 A1
20080062164 Bassi et al. Mar 2008 A1
20080079805 Takagi et al. Apr 2008 A1
20080080028 Bakin et al. Apr 2008 A1
20080084486 Enge et al. Apr 2008 A1
20080088793 Sverdrup et al. Apr 2008 A1
20080095523 Schilling-Benz et al. Apr 2008 A1
20080099804 Venezia et al. May 2008 A1
20080106620 Sawachi May 2008 A1
20080112059 Choi et al. May 2008 A1
20080112635 Kondo et al. May 2008 A1
20080117289 Schowengerdt et al. May 2008 A1
20080118241 TeKolste et al. May 2008 A1
20080131019 Ng Jun 2008 A1
20080131107 Ueno Jun 2008 A1
20080151097 Chen et al. Jun 2008 A1
20080152213 Medioni et al. Jun 2008 A1
20080152215 Horie et al. Jun 2008 A1
20080152296 Oh et al. Jun 2008 A1
20080156991 Hu et al. Jul 2008 A1
20080158259 Kempf et al. Jul 2008 A1
20080158375 Kakkori et al. Jul 2008 A1
20080158698 Chang et al. Jul 2008 A1
20080165257 Boettiger Jul 2008 A1
20080174670 Olsen et al. Jul 2008 A1
20080187305 Raskar et al. Aug 2008 A1
20080193026 Horie et al. Aug 2008 A1
20080208506 Kuwata Aug 2008 A1
20080211737 Kim et al. Sep 2008 A1
20080218610 Chapman et al. Sep 2008 A1
20080218611 Parulski et al. Sep 2008 A1
20080218612 Border et al. Sep 2008 A1
20080218613 Janson et al. Sep 2008 A1
20080219654 Border et al. Sep 2008 A1
20080239116 Smith Oct 2008 A1
20080240598 Hasegawa Oct 2008 A1
20080246866 Kinoshita et al. Oct 2008 A1
20080247638 Tanida et al. Oct 2008 A1
20080247653 Moussavi et al. Oct 2008 A1
20080272416 Yun Nov 2008 A1
20080273751 Yuan et al. Nov 2008 A1
20080278591 Barna et al. Nov 2008 A1
20080278610 Boettiger Nov 2008 A1
20080284880 Numata Nov 2008 A1
20080291295 Kato et al. Nov 2008 A1
20080298674 Baker et al. Dec 2008 A1
20080310501 Ward et al. Dec 2008 A1
20090027543 Kanehiro Jan 2009 A1
20090050946 Duparre et al. Feb 2009 A1
20090052743 Techmer Feb 2009 A1
20090060281 Tanida et al. Mar 2009 A1
20090066693 Carson Mar 2009 A1
20090079862 Subbotin Mar 2009 A1
20090086074 Li et al. Apr 2009 A1
20090091645 Trimeche et al. Apr 2009 A1
20090091806 Inuiya Apr 2009 A1
20090092363 Daum et al. Apr 2009 A1
20090096050 Park Apr 2009 A1
20090102956 Georgiev Apr 2009 A1
20090103792 Rahn et al. Apr 2009 A1
20090109306 Shan et al. Apr 2009 A1
20090127430 Hirasawa et al. May 2009 A1
20090128644 Camp, Jr. et al. May 2009 A1
20090128833 Yahav May 2009 A1
20090129667 Ho et al. May 2009 A1
20090140131 Utagawa Jun 2009 A1
20090141933 Wagg Jun 2009 A1
20090147919 Goto et al. Jun 2009 A1
20090152664 Klem et al. Jun 2009 A1
20090167922 Perlman et al. Jul 2009 A1
20090167923 Safaee-Rad et al. Jul 2009 A1
20090167934 Gupta Jul 2009 A1
20090175349 Ye et al. Jul 2009 A1
20090179142 Duparre et al. Jul 2009 A1
20090180021 Kikuchi et al. Jul 2009 A1
20090200622 Tai et al. Aug 2009 A1
20090201371 Matsuda et al. Aug 2009 A1
20090207235 Francini et al. Aug 2009 A1
20090219435 Yuan Sep 2009 A1
20090225203 Tanida et al. Sep 2009 A1
20090237520 Kaneko et al. Sep 2009 A1
20090245573 Saptharishi et al. Oct 2009 A1
20090245637 Barman et al. Oct 2009 A1
20090256947 Ciurea et al. Oct 2009 A1
20090263017 Tanbakuchi Oct 2009 A1
20090268192 Koenck et al. Oct 2009 A1
20090268970 Babacan et al. Oct 2009 A1
20090268983 Stone et al. Oct 2009 A1
20090273663 Yoshida Nov 2009 A1
20090274387 Jin Nov 2009 A1
20090279800 Uetani et al. Nov 2009 A1
20090284651 Srinivasan Nov 2009 A1
20090290811 Imai Nov 2009 A1
20090297056 Lelescu et al. Dec 2009 A1
20090302205 Olsen et al. Dec 2009 A9
20090317061 Jung et al. Dec 2009 A1
20090322876 Lee et al. Dec 2009 A1
20090323195 Hembree et al. Dec 2009 A1
20090323206 Oliver et al. Dec 2009 A1
20090324118 Maslov et al. Dec 2009 A1
20100002126 Wenstrand et al. Jan 2010 A1
20100002313 Duparre et al. Jan 2010 A1
20100002314 Duparre Jan 2010 A1
20100007714 Kim et al. Jan 2010 A1
20100013927 Nixon Jan 2010 A1
20100044815 Chang Feb 2010 A1
20100045809 Packard Feb 2010 A1
20100053342 Hwang et al. Mar 2010 A1
20100053347 Agarwala et al. Mar 2010 A1
20100053415 Yun Mar 2010 A1
20100053600 Tanida et al. Mar 2010 A1
20100060746 Olsen et al. Mar 2010 A9
20100073463 Momonoi et al. Mar 2010 A1
20100074532 Gordon et al. Mar 2010 A1
20100085351 Deb et al. Apr 2010 A1
20100085425 Tan Apr 2010 A1
20100086227 Sun et al. Apr 2010 A1
20100091389 Henriksen et al. Apr 2010 A1
20100097444 Lablans Apr 2010 A1
20100097491 Farina et al. Apr 2010 A1
20100103175 Okutomi et al. Apr 2010 A1
20100103259 Tanida et al. Apr 2010 A1
20100103308 Butterfield et al. Apr 2010 A1
20100111444 Coffman May 2010 A1
20100118127 Nam et al. May 2010 A1
20100128145 Pitts et al. May 2010 A1
20100129048 Pitts et al. May 2010 A1
20100133230 Henriksen et al. Jun 2010 A1
20100133418 Sargent et al. Jun 2010 A1
20100141802 Knight et al. Jun 2010 A1
20100142828 Chang et al. Jun 2010 A1
20100142839 Lakus-Becker Jun 2010 A1
20100157073 Kondo et al. Jun 2010 A1
20100165152 Lim Jul 2010 A1
20100166410 Chang Jul 2010 A1
20100171866 Brady et al. Jul 2010 A1
20100177411 Hegde et al. Jul 2010 A1
20100182406 Benitez Jul 2010 A1
20100194860 Mentz et al. Aug 2010 A1
20100194901 van Hoorebeke et al. Aug 2010 A1
20100195716 Klein Gunnewiek et al. Aug 2010 A1
20100201809 Oyama et al. Aug 2010 A1
20100201834 Maruyama et al. Aug 2010 A1
20100202054 Niederer Aug 2010 A1
20100202683 Robinson Aug 2010 A1
20100208100 Olsen et al. Aug 2010 A9
20100214423 Ogawa Aug 2010 A1
20100220212 Perlman et al. Sep 2010 A1
20100223237 Mishra et al. Sep 2010 A1
20100225740 Jung et al. Sep 2010 A1
20100231285 Boomer et al. Sep 2010 A1
20100238327 Griffith et al. Sep 2010 A1
20100244165 Lake et al. Sep 2010 A1
20100245684 Xiao et al. Sep 2010 A1
20100254627 Tehran et al. Oct 2010 A1
20100259610 Petersen Oct 2010 A1
20100265346 Iizuka Oct 2010 A1
20100265381 Yamamoto et al. Oct 2010 A1
20100265385 Knight et al. Oct 2010 A1
20100277629 Tanaka Nov 2010 A1
20100281070 Chan et al. Nov 2010 A1
20100289941 Ito et al. Nov 2010 A1
20100290483 Park et al. Nov 2010 A1
20100302423 Adams, Jr. et al. Dec 2010 A1
20100309292 Ho et al. Dec 2010 A1
20100309368 Choi et al. Dec 2010 A1
20100321595 Chiu Dec 2010 A1
20100321640 Yeh et al. Dec 2010 A1
20100329556 Mitarai et al. Dec 2010 A1
20100329582 Albu et al. Dec 2010 A1
20110001037 Tewinkle Jan 2011 A1
20110013006 Uzenbajakava et al. Jan 2011 A1
20110018973 Takayama Jan 2011 A1
20110019048 Raynor et al. Jan 2011 A1
20110019243 Constant, Jr. et al. Jan 2011 A1
20110031381 Tay et al. Feb 2011 A1
20110032341 Ignatov et al. Feb 2011 A1
20110032370 Ludwig Feb 2011 A1
20110033129 Robinson Feb 2011 A1
20110038536 Gong Feb 2011 A1
20110043604 Peleg et al. Feb 2011 A1
20110043613 Rohaly et al. Feb 2011 A1
20110043661 Podoleanu Feb 2011 A1
20110043665 Ogasahara Feb 2011 A1
20110043668 McKinnon et al. Feb 2011 A1
20110044502 Liu et al. Feb 2011 A1
20110051255 Lee et al. Mar 2011 A1
20110055729 Mason et al. Mar 2011 A1
20110064327 Dagher et al. Mar 2011 A1
20110069189 Venkataraman et al. Mar 2011 A1
20110080487 Venkataraman et al. Apr 2011 A1
20110084893 Lee et al. Apr 2011 A1
20110085028 Samadani et al. Apr 2011 A1
20110090217 Mashitani et al. Apr 2011 A1
20110102553 Corcoran et al. May 2011 A1
20110108708 Olsen et al. May 2011 A1
20110115886 Nguyen et al. May 2011 A1
20110121421 Charbon et al. May 2011 A1
20110122308 Duparre May 2011 A1
20110128393 Tavi et al. Jun 2011 A1
20110128412 Milnes et al. Jun 2011 A1
20110129165 Lim et al. Jun 2011 A1
20110141309 Nagashima et al. Jun 2011 A1
20110142138 Tian et al. Jun 2011 A1
20110149408 Hahgholt et al. Jun 2011 A1
20110149409 Haugholt et al. Jun 2011 A1
20110150321 Cheong et al. Jun 2011 A1
20110153248 Gu et al. Jun 2011 A1
20110157321 Nakajima et al. Jun 2011 A1
20110157451 Chang Jun 2011 A1
20110169994 DiFrancesco et al. Jul 2011 A1
20110176020 Chang Jul 2011 A1
20110181797 Galstian et al. Jul 2011 A1
20110193944 Lian et al. Aug 2011 A1
20110199458 Hayasaka et al. Aug 2011 A1
20110200319 Kravitz et al. Aug 2011 A1
20110206291 Kashani et al. Aug 2011 A1
20110207074 Hall-Holt et al. Aug 2011 A1
20110211068 Yokota Sep 2011 A1
20110211077 Nayar et al. Sep 2011 A1
20110211824 Georgiev et al. Sep 2011 A1
20110221599 Högasten Sep 2011 A1
20110221658 Haddick et al. Sep 2011 A1
20110221939 Jerdev Sep 2011 A1
20110221950 Oostra et al. Sep 2011 A1
20110222757 Yeatman, Jr. et al. Sep 2011 A1
20110227922 Shim Sep 2011 A1
20110228142 Brueckner et al. Sep 2011 A1
20110228144 Tian et al. Sep 2011 A1
20110234825 Liu et al. Sep 2011 A1
20110234841 Akeley et al. Sep 2011 A1
20110241234 Duparre Oct 2011 A1
20110242342 Goma et al. Oct 2011 A1
20110242355 Goma et al. Oct 2011 A1
20110242356 Aleksic et al. Oct 2011 A1
20110243428 Das Gupta et al. Oct 2011 A1
20110255592 Sung et al. Oct 2011 A1
20110255745 Hodder et al. Oct 2011 A1
20110255786 Hunter et al. Oct 2011 A1
20110261993 Weiming et al. Oct 2011 A1
20110267264 Mccarthy et al. Nov 2011 A1
20110267348 Lin et al. Nov 2011 A1
20110273531 Ito et al. Nov 2011 A1
20110274175 Sumitomo Nov 2011 A1
20110274366 Tardif Nov 2011 A1
20110279705 Kuang et al. Nov 2011 A1
20110279721 McMahon Nov 2011 A1
20110285701 Chen et al. Nov 2011 A1
20110285866 Bhrugumalla et al. Nov 2011 A1
20110285910 Bamji et al. Nov 2011 A1
20110292216 Fergus et al. Dec 2011 A1
20110298898 Jung et al. Dec 2011 A1
20110298917 Yanagita Dec 2011 A1
20110300929 Tardif et al. Dec 2011 A1
20110310980 Mathew Dec 2011 A1
20110316968 Taguchi et al. Dec 2011 A1
20110317766 Lim et al. Dec 2011 A1
20120012748 Pain Jan 2012 A1
20120013748 Stanwood et al. Jan 2012 A1
20120014456 Martinez Bauza et al. Jan 2012 A1
20120019530 Baker Jan 2012 A1
20120019700 Gaber Jan 2012 A1
20120023456 Sun et al. Jan 2012 A1
20120026297 Sato Feb 2012 A1
20120026342 Yu et al. Feb 2012 A1
20120026366 Golan et al. Feb 2012 A1
20120026451 Nystrom Feb 2012 A1
20120026478 Chen et al. Feb 2012 A1
20120038745 Yu et al. Feb 2012 A1
20120039525 Tian et al. Feb 2012 A1
20120044249 Mashitani et al. Feb 2012 A1
20120044372 Côté et al. Feb 2012 A1
20120051624 Ando Mar 2012 A1
20120056982 Katz et al. Mar 2012 A1
20120057040 Park et al. Mar 2012 A1
20120062697 Treado et al. Mar 2012 A1
20120062702 Jiang et al. Mar 2012 A1
20120062756 Tian et al. Mar 2012 A1
20120069235 Imai Mar 2012 A1
20120081519 Goma et al. Apr 2012 A1
20120086803 Malzbender et al. Apr 2012 A1
20120105590 Fukumoto et al. May 2012 A1
20120105654 Kwatra et al. May 2012 A1
20120105691 Waqas et al. May 2012 A1
20120113232 Joblove May 2012 A1
20120113318 Galstian et al. May 2012 A1
20120113413 Miahczylowicz-Wolski et al. May 2012 A1
20120114224 Xu et al. May 2012 A1
20120114260 Takahashi et al. May 2012 A1
20120120264 Lee et al. May 2012 A1
20120127275 Von Zitzewitz et al. May 2012 A1
20120127284 Bar-Zeev et al. May 2012 A1
20120147139 Li et al. Jun 2012 A1
20120147205 Lelescu et al. Jun 2012 A1
20120153153 Chang et al. Jun 2012 A1
20120154551 Inoue Jun 2012 A1
20120155830 Sasaki et al. Jun 2012 A1
20120162374 Markas et al. Jun 2012 A1
20120163672 McKinnon Jun 2012 A1
20120163725 Fukuhara Jun 2012 A1
20120169433 Mullins et al. Jul 2012 A1
20120170134 Bolis et al. Jul 2012 A1
20120176479 Mayhew et al. Jul 2012 A1
20120176481 Lukk et al. Jul 2012 A1
20120188235 Wu et al. Jul 2012 A1
20120188341 Klein Gunnewiek et al. Jul 2012 A1
20120188389 Lin et al. Jul 2012 A1
20120188420 Black et al. Jul 2012 A1
20120188634 Kubala et al. Jul 2012 A1
20120198677 Duparre Aug 2012 A1
20120200669 Lai et al. Aug 2012 A1
20120200726 Bugnariu Aug 2012 A1
20120200734 Tang Aug 2012 A1
20120206582 DiCarlo et al. Aug 2012 A1
20120218455 Imai et al. Aug 2012 A1
20120219236 Ali et al. Aug 2012 A1
20120224083 Jovanovski et al. Sep 2012 A1
20120229602 Chen et al. Sep 2012 A1
20120229628 Ishiyama et al. Sep 2012 A1
20120237114 Park et al. Sep 2012 A1
20120249550 Akeley et al. Oct 2012 A1
20120249750 Izzat et al. Oct 2012 A1
20120249836 Ali et al. Oct 2012 A1
20120249853 Krolczyk et al. Oct 2012 A1
20120250990 Bocirnea Oct 2012 A1
20120262601 Choi et al. Oct 2012 A1
20120262607 Shimura et al. Oct 2012 A1
20120268574 Gidon et al. Oct 2012 A1
20120274626 Hsieh Nov 2012 A1
20120287291 McMahon Nov 2012 A1
20120290257 Hodge et al. Nov 2012 A1
20120293489 Chen et al. Nov 2012 A1
20120293624 Chen et al. Nov 2012 A1
20120293695 Tanaka Nov 2012 A1
20120307084 Mantzel Dec 2012 A1
20120307093 Miyoshi Dec 2012 A1
20120307099 Yahata Dec 2012 A1
20120314033 Lee et al. Dec 2012 A1
20120314937 Kim et al. Dec 2012 A1
20120327222 Ng et al. Dec 2012 A1
20130002828 Ding et al. Jan 2013 A1
20130002953 Noguchi et al. Jan 2013 A1
20130003184 Duparre Jan 2013 A1
20130010073 Do et al. Jan 2013 A1
20130016245 Yuba Jan 2013 A1
20130016885 Tsujimoto Jan 2013 A1
20130022111 Chen et al. Jan 2013 A1
20130027580 Olsen et al. Jan 2013 A1
20130033579 Wajs Feb 2013 A1
20130033585 Li et al. Feb 2013 A1
20130038696 Ding et al. Feb 2013 A1
20130047396 Au et al. Feb 2013 A1
20130050504 Safaee-Rad et al. Feb 2013 A1
20130050526 Keelan Feb 2013 A1
20130057710 McMahon Mar 2013 A1
20130070060 Chatterjee et al. Mar 2013 A1
20130076967 Brunner et al. Mar 2013 A1
20130077859 Stauder et al. Mar 2013 A1
20130077880 Venkataraman et al. Mar 2013 A1
20130077882 Venkataraman et al. Mar 2013 A1
20130083172 Baba Apr 2013 A1
20130088489 Schmeitz et al. Apr 2013 A1
20130088637 Duparre Apr 2013 A1
20130093842 Yahata Apr 2013 A1
20130100254 Morioka et al. Apr 2013 A1
20130107061 Kumar et al. May 2013 A1
20130113888 Koguchi May 2013 A1
20130113899 Morohoshi et al. May 2013 A1
20130113939 Strandemar May 2013 A1
20130120536 Song et al. May 2013 A1
20130120605 Georgiev et al. May 2013 A1
20130121559 Hu et al. May 2013 A1
20130127988 Wang et al. May 2013 A1
20130128049 Schofield et al. May 2013 A1
20130128068 Georgiev et al. May 2013 A1
20130128069 Georgiev et al. May 2013 A1
20130128087 Georgiev et al. May 2013 A1
20130128121 Agarwala et al. May 2013 A1
20130135315 Bares et al. May 2013 A1
20130135448 Nagumo et al. May 2013 A1
20130147979 McMahon et al. Jun 2013 A1
20130155050 Rastogi et al. Jun 2013 A1
20130162641 Zhang et al. Jun 2013 A1
20130169754 Aronsson et al. Jul 2013 A1
20130176394 Tian et al. Jul 2013 A1
20130208138 Li et al. Aug 2013 A1
20130215108 McMahon et al. Aug 2013 A1
20130215231 Hiramoto et al. Aug 2013 A1
20130216144 Robinson et al. Aug 2013 A1
20130222556 Shimada Aug 2013 A1
20130222656 Kaneko Aug 2013 A1
20130223759 Nishiyama Aug 2013 A1
20130229540 Farina et al. Sep 2013 A1
20130230237 Schlosser et al. Sep 2013 A1
20130250123 Zhang et al. Sep 2013 A1
20130250150 Malone et al. Sep 2013 A1
20130258067 Zhang et al. Oct 2013 A1
20130259317 Gaddy Oct 2013 A1
20130265459 Duparre et al. Oct 2013 A1
20130274596 Azizian et al. Oct 2013 A1
20130274923 By Oct 2013 A1
20130278631 Border et al. Oct 2013 A1
20130286236 Mankowski Oct 2013 A1
20130293760 Nisenzon et al. Nov 2013 A1
20130308197 Duparre Nov 2013 A1
20130321581 El-Ghoroury et al. Dec 2013 A1
20130321589 Kirk et al. Dec 2013 A1
20130335598 Gustavsson et al. Dec 2013 A1
20130342641 Morioka et al. Dec 2013 A1
20140002674 Duparre et al. Jan 2014 A1
20140002675 Duparre et al. Jan 2014 A1
20140009586 McNamer et al. Jan 2014 A1
20140013273 Ng Jan 2014 A1
20140037137 Broaddus et al. Feb 2014 A1
20140037140 Benhimane et al. Feb 2014 A1
20140043507 Wang et al. Feb 2014 A1
20140050355 Cobb Feb 2014 A1
20140059462 Wernersson Feb 2014 A1
20140076336 Clayton et al. Mar 2014 A1
20140078333 Miao Mar 2014 A1
20140079336 Venkataraman et al. Mar 2014 A1
20140081454 Nuyujukian et al. Mar 2014 A1
20140085502 Lin et al. Mar 2014 A1
20140092281 Nisenzon et al. Apr 2014 A1
20140098266 Nayar et al. Apr 2014 A1
20140098267 Tian et al. Apr 2014 A1
20140104490 Hsieh et al. Apr 2014 A1
20140118493 Sali et al. May 2014 A1
20140118584 Lee et al. May 2014 A1
20140125760 Au et al. May 2014 A1
20140125771 Grossmann et al. May 2014 A1
20140132810 McMahon May 2014 A1
20140139642 Ni et al. May 2014 A1
20140139643 Hogasten et al. May 2014 A1
20140140626 Cho et al. May 2014 A1
20140146132 Bagnato et al. May 2014 A1
20140146201 Knight et al. May 2014 A1
20140176592 Wilburn et al. Jun 2014 A1
20140183258 DiMuro Jul 2014 A1
20140183334 Wang et al. Jul 2014 A1
20140186045 Poddar et al. Jul 2014 A1
20140192154 Jeong et al. Jul 2014 A1
20140192253 Laroia Jul 2014 A1
20140198188 Izawa Jul 2014 A1
20140204183 Lee et al. Jul 2014 A1
20140218546 McMahon Aug 2014 A1
20140232822 Venkataraman et al. Aug 2014 A1
20140240528 Venkataraman et al. Aug 2014 A1
20140240529 Venkataraman et al. Aug 2014 A1
20140253738 Mullis Sep 2014 A1
20140267243 Venkataraman et al. Sep 2014 A1
20140267286 Duparre Sep 2014 A1
20140267633 Venkataraman et al. Sep 2014 A1
20140267762 Mullis et al. Sep 2014 A1
20140267829 McMahon et al. Sep 2014 A1
20140267890 Lelescu et al. Sep 2014 A1
20140285675 Mullis Sep 2014 A1
20140300706 Song Oct 2014 A1
20140307058 Kirk et al. Oct 2014 A1
20140307063 Lee Oct 2014 A1
20140313315 Shoham et al. Oct 2014 A1
20140321712 Ciurea et al. Oct 2014 A1
20140333731 Venkataraman et al. Nov 2014 A1
20140333764 Venkataraman et al. Nov 2014 A1
20140333787 Venkataraman et al. Nov 2014 A1
20140340539 Venkataraman et al. Nov 2014 A1
20140347509 Venkataraman et al. Nov 2014 A1
20140347748 Duparre Nov 2014 A1
20140354773 Venkataraman et al. Dec 2014 A1
20140354843 Venkataraman et al. Dec 2014 A1
20140354844 Venkataraman et al. Dec 2014 A1
20140354853 Venkataraman et al. Dec 2014 A1
20140354854 Venkataraman et al. Dec 2014 A1
20140354855 Venkataraman et al. Dec 2014 A1
20140355870 Venkataraman et al. Dec 2014 A1
20140368662 Venkataraman et al. Dec 2014 A1
20140368683 Venkataraman et al. Dec 2014 A1
20140368684 Venkataraman et al. Dec 2014 A1
20140368685 Venkataraman et al. Dec 2014 A1
20140368686 Duparre Dec 2014 A1
20140369612 Venkataraman et al. Dec 2014 A1
20140369615 Venkataraman et al. Dec 2014 A1
20140376825 Venkataraman et al. Dec 2014 A1
20140376826 Venkataraman et al. Dec 2014 A1
20150002734 Lee Jan 2015 A1
20150003752 Venkataraman et al. Jan 2015 A1
20150003753 Venkataraman et al. Jan 2015 A1
20150009353 Venkataraman et al. Jan 2015 A1
20150009354 Venkataraman et al. Jan 2015 A1
20150009362 Venkataraman et al. Jan 2015 A1
20150015669 Venkataraman et al. Jan 2015 A1
20150035992 Mullis Feb 2015 A1
20150036014 Lelescu et al. Feb 2015 A1
20150036015 Lelescu et al. Feb 2015 A1
20150042766 Ciurea et al. Feb 2015 A1
20150042767 Ciurea et al. Feb 2015 A1
20150042814 Vaziri Feb 2015 A1
20150042833 Lelescu et al. Feb 2015 A1
20150043806 Karsch et al. Feb 2015 A1
20150049915 Ciurea et al. Feb 2015 A1
20150049916 Ciurea et al. Feb 2015 A1
20150049917 Ciurea et al. Feb 2015 A1
20150055884 Venkataraman et al. Feb 2015 A1
20150085073 Bruls et al. Mar 2015 A1
20150085174 Shabtay et al. Mar 2015 A1
20150091900 Yang et al. Apr 2015 A1
20150095235 Dua Apr 2015 A1
20150098079 Montgomery et al. Apr 2015 A1
20150104076 Hayasaka Apr 2015 A1
20150104101 Bryant et al. Apr 2015 A1
20150122411 Rodda et al. May 2015 A1
20150124059 Georgiev et al. May 2015 A1
20150124113 Rodda et al. May 2015 A1
20150124151 Rodda et al. May 2015 A1
20150138346 Venkataraman et al. May 2015 A1
20150146029 Venkataraman et al. May 2015 A1
20150146030 Venkataraman et al. May 2015 A1
20150161798 Venkataraman et al. Jun 2015 A1
20150199793 Venkataraman et al. Jul 2015 A1
20150199841 Venkataraman et al. Jul 2015 A1
20150207990 Ford et al. Jul 2015 A1
20150228081 Kim et al. Aug 2015 A1
20150235476 McMahon et al. Aug 2015 A1
20150237329 Venkataraman et al. Aug 2015 A1
20150243480 Yamada Aug 2015 A1
20150244927 Laroia et al. Aug 2015 A1
20150245013 Venkataraman et al. Aug 2015 A1
20150248744 Hayasaka et al. Sep 2015 A1
20150254868 Srikanth et al. Sep 2015 A1
20150264337 Venkataraman et al. Sep 2015 A1
20150288861 Duparre Oct 2015 A1
20150296137 Duparre et al. Oct 2015 A1
20150312455 Venkataraman et al. Oct 2015 A1
20150317638 Donaldson Nov 2015 A1
20150325048 Engle et al. Nov 2015 A1
20150326852 Duparre et al. Nov 2015 A1
20150332468 Hayasaka et al. Nov 2015 A1
20150373261 Rodda et al. Dec 2015 A1
20160037097 Duparre Feb 2016 A1
20160042548 Du et al. Feb 2016 A1
20160044252 Molina Feb 2016 A1
20160044257 Venkataraman et al. Feb 2016 A1
20160057332 Ciurea et al. Feb 2016 A1
20160065934 Kaza et al. Mar 2016 A1
20160163051 Mullis Jun 2016 A1
20160165106 Duparre Jun 2016 A1
20160165134 Lelescu et al. Jun 2016 A1
20160165147 Nisenzon et al. Jun 2016 A1
20160165212 Mullis Jun 2016 A1
20160182786 Anderson et al. Jun 2016 A1
20160191768 Shin et al. Jun 2016 A1
20160195733 Lelescu et al. Jul 2016 A1
20160198096 McMahon et al. Jul 2016 A1
20160209654 Riccomini et al. Jul 2016 A1
20160210785 Balachandreswaran et al. Jul 2016 A1
20160227195 Venkataraman et al. Aug 2016 A1
20160249001 McMahon Aug 2016 A1
20160255333 Nisenzon et al. Sep 2016 A1
20160266284 Duparre et al. Sep 2016 A1
20160267486 Mitra et al. Sep 2016 A1
20160267665 Venkataraman et al. Sep 2016 A1
20160267672 Ciurea et al. Sep 2016 A1
20160269626 McMahon Sep 2016 A1
20160269627 McMahon Sep 2016 A1
20160269650 Venkataraman et al. Sep 2016 A1
20160269651 Venkataraman et al. Sep 2016 A1
20160269664 Duparre Sep 2016 A1
20160309084 Venkataraman et al. Oct 2016 A1
20160309134 Venkataraman et al. Oct 2016 A1
20160316140 Nayar et al. Oct 2016 A1
20160323578 Kaneko et al. Nov 2016 A1
20170004791 Aubineau et al. Jan 2017 A1
20170006233 Venkataraman et al. Jan 2017 A1
20170011405 Pandey Jan 2017 A1
20170048468 Pain et al. Feb 2017 A1
20170053382 Lelescu et al. Feb 2017 A1
20170054901 Venkataraman et al. Feb 2017 A1
20170070672 Rodda et al. Mar 2017 A1
20170070673 Lelescu et al. Mar 2017 A1
20170070753 Kaneko Mar 2017 A1
20170078568 Venkataraman et al. Mar 2017 A1
20170085845 Venkataraman et al. Mar 2017 A1
20170094243 Venkataraman et al. Mar 2017 A1
20170099465 Mullis et al. Apr 2017 A1
20170109742 Varadarajan Apr 2017 A1
20170142405 Shors et al. May 2017 A1
20170163862 Molina Jun 2017 A1
20170178363 Venkataraman et al. Jun 2017 A1
20170187933 Duparre Jun 2017 A1
20170188011 Panescu et al. Jun 2017 A1
20170244960 Ciurea et al. Aug 2017 A1
20170257562 Venkataraman et al. Sep 2017 A1
20170365104 McMahon et al. Dec 2017 A1
20180005244 Govindarajan et al. Jan 2018 A1
20180007284 Venkataraman et al. Jan 2018 A1
20180013945 Ciurea et al. Jan 2018 A1
20180024330 Laroia Jan 2018 A1
20180035057 McMahon et al. Feb 2018 A1
20180040135 Mullis Feb 2018 A1
20180048830 Venkataraman et al. Feb 2018 A1
20180048879 Venkataraman et al. Feb 2018 A1
20180081090 Duparre et al. Mar 2018 A1
20180097993 Nayar et al. Apr 2018 A1
20180109782 Duparre et al. Apr 2018 A1
20180124311 Lelescu et al. May 2018 A1
20180131852 McMahon May 2018 A1
20180139382 Venkataraman et al. May 2018 A1
20180189767 Bigioi Jul 2018 A1
20180197035 Venkataraman et al. Jul 2018 A1
20180211402 Ciurea et al. Jul 2018 A1
20180227511 McMahon Aug 2018 A1
20180240265 Yang et al. Aug 2018 A1
20180270473 Mullis Sep 2018 A1
20180286120 Fleishman et al. Oct 2018 A1
20180302554 Lelescu et al. Oct 2018 A1
20180308281 Okoyama Oct 2018 A1
20180330182 Venkataraman et al. Nov 2018 A1
20180376122 Park et al. Dec 2018 A1
20190012768 Tafazoli Bilandi et al. Jan 2019 A1
20190037116 Molina Jan 2019 A1
20190037150 Srikanth et al. Jan 2019 A1
20190043253 Lucas et al. Feb 2019 A1
20190057513 Jain et al. Feb 2019 A1
20190063905 Venkataraman et al. Feb 2019 A1
20190089947 Venkataraman et al. Mar 2019 A1
20190098209 Venkataraman et al. Mar 2019 A1
20190109998 Venkataraman et al. Apr 2019 A1
20190164341 Venkataraman May 2019 A1
20190174040 Mcmahon Jun 2019 A1
20190197735 Xiong et al. Jun 2019 A1
20190215496 Mullis et al. Jul 2019 A1
20190230348 Ciurea et al. Jul 2019 A1
20190235138 Duparre et al. Aug 2019 A1
20190243086 Rodda et al. Aug 2019 A1
20190244379 Venkataraman Aug 2019 A1
20190268586 Mullis Aug 2019 A1
20190289176 Duparre Sep 2019 A1
20190347768 Lelescu et al. Nov 2019 A1
20190356863 Venkataraman et al. Nov 2019 A1
20190362515 Ciurea et al. Nov 2019 A1
20190364263 Jannard et al. Nov 2019 A1
20200026948 Venkataraman et al. Jan 2020 A1
20200151894 Jain et al. May 2020 A1
20200252597 Mullis Aug 2020 A1
20200334905 Venkataraman Oct 2020 A1
20200389604 Venkataraman et al. Dec 2020 A1
20210042952 Jain et al. Feb 2021 A1
20210044790 Venkataraman et al. Feb 2021 A1
20210063141 Venkataraman et al. Mar 2021 A1
20210084206 McEldowney Mar 2021 A1
20210133927 Lelescu et al. May 2021 A1
20210150748 Ciurea et al. May 2021 A1
20210264147 Kadambi Aug 2021 A1
20210264607 Kalra Aug 2021 A1
20210356572 Kadambi Nov 2021 A1
20230048725 Barbour Feb 2023 A1
Foreign Referenced Citations (279)
Number Date Country
2488005 Apr 2002 CN
1619358 May 2005 CN
1669332 Sep 2005 CN
1727991 Feb 2006 CN
1839394 Sep 2006 CN
1985524 Jun 2007 CN
1992499 Jul 2007 CN
101010619 Aug 2007 CN
101046882 Oct 2007 CN
101064780 Oct 2007 CN
101102388 Jan 2008 CN
101147392 Mar 2008 CN
201043890 Apr 2008 CN
101212566 Jul 2008 CN
101312540 Nov 2008 CN
101427372 May 2009 CN
101551586 Oct 2009 CN
101593350 Dec 2009 CN
101606086 Dec 2009 CN
101785025 Jul 2010 CN
101883291 Nov 2010 CN
102037717 Apr 2011 CN
102164298 Aug 2011 CN
102184720 Sep 2011 CN
102375199 Mar 2012 CN
103004180 Mar 2013 CN
103765864 Apr 2014 CN
104081414 Oct 2014 CN
104508681 Apr 2015 CN
104662589 May 2015 CN
104685513 Jun 2015 CN
104685860 Jun 2015 CN
105409212 Mar 2016 CN
103765864 Jul 2017 CN
104081414 Aug 2017 CN
104662589 Aug 2017 CN
107077743 Aug 2017 CN
107230236 Oct 2017 CN
107346061 Nov 2017 CN
107404609 Nov 2017 CN
104685513 Apr 2018 CN
107924572 Apr 2018 CN
108307675 Jul 2018 CN
104335246 Sep 2018 CN
107404609 Feb 2020 CN
107346061 Apr 2020 CN
107230236 Dec 2020 CN
108307675 Dec 2020 CN
107077743 Mar 2021 CN
602011041799.1 Sep 2017 DE
0677821 Oct 1995 EP
0840502 May 1998 EP
1201407 May 2002 EP
1355274 Oct 2003 EP
1734766 Dec 2006 EP
1991145 Nov 2008 EP
1243945 Jan 2009 EP
2026563 Feb 2009 EP
2031592 Mar 2009 EP
2041454 Apr 2009 EP
2072785 Jun 2009 EP
2104334 Sep 2009 EP
2136345 Dec 2009 EP
2156244 Feb 2010 EP
2244484 Oct 2010 EP
0957642 Apr 2011 EP
2336816 Jun 2011 EP
2339532 Jun 2011 EP
2381418 Oct 2011 EP
2386554 Nov 2011 EP
2462477 Jun 2012 EP
2502115 Sep 2012 EP
2569935 Mar 2013 EP
2652678 Oct 2013 EP
2677066 Dec 2013 EP
2708019 Mar 2014 EP
2761534 Aug 2014 EP
2777245 Sep 2014 EP
2867718 May 2015 EP
2873028 May 2015 EP
2888698 Jul 2015 EP
2888720 Jul 2015 EP
2901671 Aug 2015 EP
2973476 Jan 2016 EP
3066690 Sep 2016 EP
2569935 Dec 2016 EP
3201877 Aug 2017 EP
2652678 Sep 2017 EP
3284061 Feb 2018 EP
3286914 Feb 2018 EP
3201877 Mar 2018 EP
2817955 Apr 2018 EP
3328048 May 2018 EP
3075140 Jun 2018 EP
3201877 Dec 2018 EP
3467776 Apr 2019 EP
2708019 Oct 2019 EP
3286914 Dec 2019 EP
2761534 Nov 2020 EP
2888720 Mar 2021 EP
3328048 Apr 2021 EP
2482022 Jan 2012 GB
2708CHENP2014 Aug 2015 IN
361194 Mar 2021 IN
59-025483 Feb 1984 JP
64-037177 Feb 1989 JP
02-285772 Nov 1990 JP
06129851 May 1994 JP
07-015457 Jan 1995 JP
H0756112 Mar 1995 JP
09171075 Jun 1997 JP
09181913 Jul 1997 JP
10253351 Sep 1998 JP
11142609 May 1999 JP
11223708 Aug 1999 JP
11325889 Nov 1999 JP
2000209503 Jul 2000 JP
2001008235 Jan 2001 JP
2001194114 Jul 2001 JP
2001264033 Sep 2001 JP
2001277260 Oct 2001 JP
2001337263 Dec 2001 JP
2002195910 Jul 2002 JP
2002205310 Jul 2002 JP
2002209226 Jul 2002 JP
2002250607 Sep 2002 JP
2002252338 Sep 2002 JP
2003094445 Apr 2003 JP
2003139910 May 2003 JP
2003163938 Jun 2003 JP
2003298920 Oct 2003 JP
2004221585 Aug 2004 JP
2005116022 Apr 2005 JP
2005181460 Jul 2005 JP
2005295381 Oct 2005 JP
2005303694 Oct 2005 JP
2005341569 Dec 2005 JP
2005354124 Dec 2005 JP
2006033228 Feb 2006 JP
2006033493 Feb 2006 JP
2006047944 Feb 2006 JP
2006258930 Sep 2006 JP
2007520107 Jul 2007 JP
2007259136 Oct 2007 JP
2008039852 Feb 2008 JP
2008055908 Mar 2008 JP
2008507874 Mar 2008 JP
2008172735 Jul 2008 JP
2008258885 Oct 2008 JP
2009064421 Mar 2009 JP
2009132010 Jun 2009 JP
2009300268 Dec 2009 JP
2010139288 Jun 2010 JP
2011017764 Jan 2011 JP
2011030184 Feb 2011 JP
2011109484 Jun 2011 JP
2011523538 Aug 2011 JP
2011203238 Oct 2011 JP
2012504805 Feb 2012 JP
2011052064 Mar 2013 JP
2013509022 Mar 2013 JP
2013526801 Jun 2013 JP
2014519741 Aug 2014 JP
2014521117 Aug 2014 JP
2014535191 Dec 2014 JP
2015022510 Feb 2015 JP
2015522178 Aug 2015 JP
2015534734 Dec 2015 JP
5848754 Jan 2016 JP
2016524125 Aug 2016 JP
6140709 May 2017 JP
2017163550 Sep 2017 JP
2017163587 Sep 2017 JP
2017531976 Oct 2017 JP
6546613 Jul 2019 JP
2019-220957 Dec 2019 JP
6630891 Dec 2019 JP
2020017999 Jan 2020 JP
6767543 Sep 2020 JP
6767558 Sep 2020 JP
1020050004239 Jan 2005 KR
100496875 Jun 2005 KR
1020110097647 Aug 2011 KR
20140045373 Apr 2014 KR
20170063827 Jun 2017 KR
101824672 Feb 2018 KR
101843994 Mar 2018 KR
101973822 Apr 2019 KR
10-2002165 Jul 2019 KR
10-2111181 May 2020 KR
191151 Jul 2013 SG
11201500910 Oct 2015 SG
200828994 Jul 2008 TW
200939739 Sep 2009 TW
201228382 Jul 2012 TW
I535292 May 2016 TW
1994020875 Sep 1994 WO
2005057922 Jun 2005 WO
2006039906 Apr 2006 WO
2006039906 Apr 2006 WO
2007013250 Feb 2007 WO
2007083579 Jul 2007 WO
2007134137 Nov 2007 WO
2008045198 Apr 2008 WO
2008050904 May 2008 WO
2008108271 Sep 2008 WO
2008108926 Sep 2008 WO
2008150817 Dec 2008 WO
2009073950 Jun 2009 WO
2009151903 Dec 2009 WO
2009157273 Dec 2009 WO
2010037512 Apr 2010 WO
2011008443 Jan 2011 WO
2011026527 Mar 2011 WO
2011046607 Apr 2011 WO
2011055655 May 2011 WO
2011063347 May 2011 WO
2011105814 Sep 2011 WO
2011116203 Sep 2011 WO
2011063347 Oct 2011 WO
2011121117 Oct 2011 WO
2011143501 Nov 2011 WO
2012057619 May 2012 WO
2012057620 May 2012 WO
2012057621 May 2012 WO
2012057622 May 2012 WO
2012057623 May 2012 WO
2012057620 Jun 2012 WO
2012074361 Jun 2012 WO
2012078126 Jun 2012 WO
2012082904 Jun 2012 WO
2012155119 Nov 2012 WO
2013003276 Jan 2013 WO
2013043751 Mar 2013 WO
2013043761 Mar 2013 WO
2013049699 Apr 2013 WO
2013055960 Apr 2013 WO
2013119706 Aug 2013 WO
2013126578 Aug 2013 WO
2013166215 Nov 2013 WO
2014004134 Jan 2014 WO
2014005123 Jan 2014 WO
2014031795 Feb 2014 WO
2014052974 Apr 2014 WO
2014032020 May 2014 WO
2014078443 May 2014 WO
2014130849 Aug 2014 WO
2014131038 Aug 2014 WO
2014133974 Sep 2014 WO
2014138695 Sep 2014 WO
2014138697 Sep 2014 WO
2014144157 Sep 2014 WO
2014145856 Sep 2014 WO
2014149403 Sep 2014 WO
2014149902 Sep 2014 WO
2014150856 Sep 2014 WO
2014153098 Sep 2014 WO
2014159721 Oct 2014 WO
2014159779 Oct 2014 WO
2014160142 Oct 2014 WO
2014164550 Oct 2014 WO
2014164909 Oct 2014 WO
2014165244 Oct 2014 WO
2014133974 Apr 2015 WO
2015048694 Apr 2015 WO
2015048906 Apr 2015 WO
2015070105 May 2015 WO
2015074078 May 2015 WO
2015081279 Jun 2015 WO
2015134996 Sep 2015 WO
2015183824 Dec 2015 WO
2016054089 Apr 2016 WO
2016172125 Oct 2016 WO
2016167814 Oct 2016 WO
2016172125 Apr 2017 WO
2018053181 Mar 2018 WO
2019038193 Feb 2019 WO
WO 2021055585 Mar 2021 WO
WO 2021108002 Jun 2021 WO
Non-Patent Literature Citations (263)
Entry
US 8,957,977 B2, 02/2015, Venkataraman et al. (withdrawn)
Zhang et al., “Deep Multimodal Fusion for Semantic Image Segmentation: A Survey”, Oct. 2020, pp. 1-58 (Year: 2020).
Gan et al., “ThreeDWorld: A Platform for Interactive Multi-Modal Physical Simulation”, Jul. 9, 2020, arXiV.org (Year: 2020).
Kondo, Yuhi, et al. “Accurate Polarimetric BRDF for Real Polarization Scene Rendering.” European Conference on Computer Vision. Springer, Cham, 2020, 17 pages.
Baek, Seung-Hwan, et al. “Image-based acquisition and modeling of polarimetric reflectance.” ACM Transactions on Graphics(Proc. SIGGRAPH 2020) 39.4 (2020), 14 pages.
Written Opinion and International Search Report for International Application No. PCT/US21/12073, dated Apr. 29, 2021, 10 pages.
Ansari et al., “3-D Face Modeling Using Two Views and a Generic Face Model with Application to 3-D Face Recognition”, Proceedings of the IEEE Conference on Advanced Video and Signal Based Surveillance, Jul. 22, 2003, 9 pgs.
Aufderheide et al., “A MEMS-based Smart Sensor System for Estimation of Camera Pose for Computer Vision Applications”, Research and Innovation Conference 2011, Jul. 29, 2011, pp. 1-10.
Baker et al., “Limits on Super-Resolution and How to Break Them”, IEEE Transactions on Pattern Analysis and Machine Intelligence, Sep. 2002, vol. 24, No. 9, pp. 1167-1183.
Banz et al., “Real-Time Semi-Global Matching Disparity Estimation on the GPU”, IEEE Transactions on Pattern Analysis and Machine Intelligence, Sep. 2002, vol. 24, No. 9, pp. 1167-1183.
Barron et al., “Intrinsic Scene Properties from a Single RGB-D Image”, 2013 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 23-28, 2013, Portland, OR, USA, pp. 17-24.
Bennett et al., “Multispectral Bilateral Video Fusion”, Computer Graphics (ACM SIGGRAPH Proceedings), Jul. 25, 2006, published Jul. 30, 2006, 1 pg.
Bennett et al., “Multispectral Video Fusion”, Computer Graphics (ACM SIGGRAPH Proceedings), Jul. 25, 2006, published Jul. 30, 2006, 1 pg.
Berretti et al., “Face Recognition by Super-Resolved 3D Models from Consumer Depth Cameras”, IEEE Transactions on Information Forensics and Security, vol. 9, No. 9, Sep. 2014, pp. 1436-1448.
Bertalmio et al., “Image Inpainting”, Proceedings of the 27th Annual Conference on Computer Graphics and Interactive Techniques, 2000, ACM Pres/Addison-Wesley Publishing Co., pp. 417-424.
Bertero et al., “Super-resolution in computational imaging”, Micron, Jan. 1, 2003, vol. 34, Issues 6-7, 17 pgs.
Bishop et al., “Full-Resolution Depth Map Estimation from an Aliased Plenoptic Light Field”, ACCV Nov. 8, 2010, Part II, LNCS 6493, pp. 186-200.
Bishop et al., “Light Field Superresolution”, Computational Photography (ICCP), 2009 IEEE International Conference, Conference Date April 16-17, published Jan. 26, 2009, 9 pgs.
Bishop et al., “The Light Field Camera: Extended Depth of Field, Aliasing, and Superresolution”, IEEE Transactions on Pattern Analysis and Machine Intelligence, May 2012, vol. 34, No. 5, published Aug. 18, 2011, pp. 972-986.
Blanz et al., “A Morphable Model for The Synthesis of 3D Faces”, In Proceedings of ACM SIGGRAPH 1999, Jul. 1, 1999, pp. 187-194.
Borman, “Topics in Multiframe Superresolution Restoration”, Thesis of Sean Borman, Apr. 2004, 282 pgs.
Borman et al., “Image Sequence Processing”, Dekker Encyclopedia of Optical Engineering, Oct. 14, 2002, 81 pgs.
Borman et al., “Linear models for multi-frame super-resolution restoration under non-affine registration and spatially varying PSF”, Proc. SPIE, May 21, 2004, vol. 5299, 12 pgs.
Borman et al., “Simultaneous Multi-Frame MAP Super-Resolution Video Enhancement Using Spatio-Temporal Priors”, Image Processing, 1999, ICIP 99 Proceedings, vol. 3, pp. 469-473.
Borman et al., “Super-Resolution from Image Sequences—A Review”, Circuits & Systems, 1998, pp. 374-378.
Borman et al., “Nonlinear Prediction Methods for Estimation of Clique Weighting Parameters in NonGaussian Image Models”, Proc. SPIE, Sep. 22, 1998, vol. 3459, 9 pgs.
Borman et al., “Block-Matching Sub-Pixel Motion Estimation from Noisy, Under-Sampled Frames—An Empirical Performance Evaluation”, Proc SPIE, Dec. 28, 1998, vol. 3653, 10 pgs.
Borman et al., “Image Resampling and Constraint Formulation for Multi-Frame Super-Resolution Restoration”, Proc SPIE, Dec. 28, 1998, vol. 3653, 10 pgs.
Bose et al., “Superresolution and Noise Filtering Using Moving Least Squares”, IEEE Transactions on Image Processing, Aug. 2006, vol. 15, Issue 8, published Jul. 17, 2006, pp. 2239-2248.
Boye et al., “Comparison of Subpixel Image Registration Algorithms”, Proc, of SPIE—IS&T Electronic Imaging, Feb. 3, 2009, vol. 7246, pp. 72460X-1-72460X-9; doi: 10.1117/12.810369.
Bruckner et al., “Thin wafer-level camera lenses inspired by insect compound eyes”, Optics Express, Nov. 22, 2010, vol. 18, No. 24, pp. 24379-24394.
Bruckner et al., “Artificial compound eye applying hyperacuity”, Optics Express, Dec. 11, 2006, vol. 14, No. 25, pp. 12076-12084.
Bruckner et al., “Driving microoptical imaging systems towards miniature camera applications”, Proc. SPIE, Micro-Optics, May 13, 2010, 11 pgs.
Bryan et al., “Perspective Distortion from Interpersonal Distance Is an Implicit Visual Cue for Social Judgments of Faces”, PLOS One, vol. 7, Issue 9, Sep. 26, 2012, e45301, doi:10.1371/journal.pone.0045301, 9 pgs.
Bulat et al., “How far are we from solving the 2D & 3D Face Alignment problem? (and a dataset of 230,000 3D facial landmarks)”, ARXIV.ORG, Cornell University Library, 201 Olin Library Cornell University Ithaca, NY 14853, Mar. 21, 2017.
Cai et al., “3D Deformable Face Tracking with a Commodity Depth Camera”, Proceedings of the European Conference on Computer Vision: Part III, Sep. 5-11, 2010, 14pgs.
Capel, “Image Mosaicing and Super-resolution”, Retrieved on Nov. 10, 2012, Retrieved from the Internet at URL:<http://citeseerx.ist.psu.edu/viewdoc/download?doi=10.1.1.226.2643&rep=rep1 &type=pdf>, 2001, 269 pgs.
Caron et al., “Multiple camera types simultaneous stereo calibration, Robotics and Automation (ICRA)”, 2011 IEEE International Conference on, May 1, 2011 (May 1, 2011), pp. 2933-2938.
Carroll et al., “Image Warps for Artistic Perspective Manipulation”, ACM Transactions on Graphics (TOG), vol. 29, No. 4, Jul. 26, 2010, Article No. 127, 9 pgs.
Chan et al., “Investigation of Computational Compound-Eye Imaging System with Super-Resolution Reconstruction”, IEEE, ISASSP, Jun. 19, 2006, pp. 1177-1180.
Chan et al., “Extending the Depth of Field in a Compound-Eye Imaging System with Super-Resolution Reconstruction”, Proceedings—International Conference on Pattern Recognition, Jan. 1, 2006, vol. 3, pp. 623-626.
Chan et al., “Super-resolution reconstruction in a computational compound-eye imaging system”, Multidim. Syst. Sign. Process, published online Feb. 23, 2007, vol. 18, pp. 83-101.
Chen et al., “Interactive deformation of light fields”, Symposium on Interactive 3D Graphics, 2005, pp. 139-146.
Chen et al., “KNN Matting”, IEEE Transactions on Pattern Analysis and Machine Intelligence, Sep. 2013, vol. 35, No. 9, pp. 2175-2188.
Chen et al., “KNN matting”, 2012 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 16-21, 2012, Providence, RI, USA, pp. 869-876.
Chen et al., “Image Matting with Local and Nonlocal Smooth Priors”, CVPR '13 Proceedings of the 2013 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 23, 2013, pp. 1902-1907.
Chen et al., “Human Face Modeling and Recognition Through Multi-View High Resolution Stereopsis”, IEEE Conference on Computer Vision and Pattern Recognition Workshop, Jun. 17-22, 2006, 6 pgs.
Collins et al., “An Active Camera System for Acquiring Multi-View Video”, IEEE 2002 International Conference on Image Processing, Date of Conference: Sep. 22-25, 2002, Rochester, NY, 4 pgs.
Cooper et al., “The perceptual basis of common photographic practice”, Journal of Vision, vol. 12, No. 5, Article 8, May 25, 2012, pp. 1-14.
Crabb et al., “Real-time foreground segmentation via range and color imaging”, 2008 IEEE Computer Society Conference on Computer Vision and Pattern Recognition Workshops, Anchorage, AK, USA, Jun. 23-28, 2008, pp. 1-5.
Dainese et al., “Accurate Depth-Map Estimation for 3D Face Modeling”, IEEE European Signal Processing Conference, Sep. 4-8, 2005, 4 pgs.
Debevec et al., “Recovering High Dynamic Range Radiance Maps from Photographs”, Computer Graphics (ACM SIGGRAPH Proceedings), Aug. 16, 1997, 10 pgs.
Do, Minh N. “Immersive Visual Communication with Depth”, Presented at Microsoft Research, Jun. 15, 2011, Retrieved from: http://minhdo.ece.illinois.edu/talks/ImmersiveComm.pdf, 42 pgs.
Do et al., Immersive Visual Communication, IEEE Signal Processing Magazine, vol. 28, Issue 1, Jan. 2011, DOI: 10.1109/MSP.2010.939075, Retrieved from: http://minhdo.ece.illinois.edu/publications/ImmerComm_SPM.pdf, pp. 58-66.
Dou et al., “End-to-end 3D face reconstruction with deep neural networks”, arXiv:1704.05020v1, Apr. 17, 2017, 10 pgs.
Drouin et al., “Improving Border Localization of Multi-Baseline Stereo Using Border-Cut”, International Journal of Computer Vision, Jul. 5, 2006, vol. 83, Issue 3, 8 pgs.
Drouin et al., “Fast Multiple-Baseline Stereo with Occlusion”, Fifth International Conference on 3-D Digital Imaging and Modeling (3DIM'05), Ottawa, Ontario, Canada, Jun. 13-16, 2005, pp. 540-547.
Drouin et al., “Geo-Consistency for Wide Multi-Camera Stereo”, 2005 IEEE Computer Society Conference on Computer Vision and Pattern Recognition (CVPR'05), vol. 1, Jun. 20-25, 2005, pp. 351-358.
Drulea et al., “Motion Estimation Using the Correlation Transform”, IEEE Transactions on Image Processing, August 2013, vol. 22, No. 8, pp. 3260-3270, first published May 14, 2013.
Duparre et al., “Microoptical artificial compound eyes—from design to experimental verification of two different concepts”, Proc. of SPIE, Optical Design and Engineering II, vol. 5962, Oct. 17, 2005, pp. 59622A-1-59622A-12.
Duparre et al., Novel Optics/Micro-Optics for Miniature Imaging Systems, Proc. of SPIE, Apr. 21, 2006, vol. 6196, pp. 619607-1-619607-15.
Duparre et al., “Micro-optical artificial compound eyes”, Bioinspiration & Biomimetics, Apr. 6, 2006, vol. 1, pp. R1-R16.
Duparre et al., “Artificial compound eye zoom camera”, Bioinspiration & Biomimetics, Nov. 21, 2008, vol. 3, pp. 1-6.
Duparre et al., “Artificial apposition compound eye fabricated by micro-optics technology”, Applied Optics, Aug. 1, 2004, vol. 43, No. 22, pp. 4303-4310.
Duparre et al., “Micro-optically fabricated artificial apposition compound eye”, Electronic Imaging—Science and Technology, Prod. SPIE 5301, Jan. 2004, pp. 25-33.
Duparre et al., “Chirped arrays of refractive ellipsoidal microlenses for aberration correction under oblique incidence”, Optics Express, Dec. 26, 2005, vol. 13, No. 26, pp. 10539-10551.
Duparre et al., “Artificial compound eyes—different concepts and their application to ultra flat image acquisition sensors”, MOEMS and Miniaturized Systems IV, Proc. SPIE 5346, Jan. 24, 2004, pp. 89-100.
Duparre et al., “Ultra-Thin Camera Based on Artificial Apposition Compound Eyes”, 10th Microoptics Conference, Sep. 1-3, 2004, 2 pgs.
Duparre et al., “Microoptical telescope compound eye”, Optics Express, Feb. 7, 2005, vol. 13, No. 3, pp. 889-903.
Duparre et al., “Theoretical analysis of an artificial superposition compound eye for application in ultra flat digital image acquisition devices”, Optical Systems Design, Proc. SPIE 5249, Sep. 2003, pp. 408-418.
Duparre et al., “Thin compound-eye camera”, Applied Optics, May 20, 2005, vol. 44, No. 15, pp. 2949-2956.
Duparre et al., “Microoptical Artificial Compound Eyes—Two Different Concepts for Compact Imaging Systems”, 11th Microoptics Conference, Oct. 30-Nov. 2, 2005, 2 pgs.
Eng et al., “Gaze correction for 3D tele-immersive communication system”, IVMSP Workshop, 2013 IEEE 11th. IEEE, Jun. 10, 2013.
Fanaswala, “Regularized Super-Resolution of Multi-View Images”, Retrieved on Nov. 10, 2012 (Nov. 11, 2012). Retrieved from the Internet at URL:<http://www.site.uottawa.ca/-edubois/theses/Fanaswala_thesis.pdf>, 2009, 163 pgs.
Fang et al., “Volume Morphing Methods for Landmark Based 3D Image Deformation”, SPIE vol. 2710, Proc. 1996 SPIE Intl Symposium on Medical Imaging, Newport Beach, CA, Feb. 10, 1996, pp. 404-415.
Fangmin et al., “3D Face Reconstruction Based on Convolutional Neural Network”, 2017 10th International Conference on Intelligent Computation Technology and Automation, Oct. 9-10, 2017, Changsha, China.
Farrell et al., “Resolution and Light Sensitivity Tradeoff with Pixel Size”, Proceedings of the SPIE Electronic Imaging 2006 Conference, Feb. 2, 2006, vol. 6069, 8 pgs.
Farsiu et al., “Advances and Challenges in Super-Resolution”, International Journal of Imaging Systems and Technology, Aug. 12, 2004, vol. 14, pp. 47-57.
Farsiu et al., “Fast and Robust Multiframe Super Resolution”, IEEE Transactions on Image Processing, Oct. 2004, published Sep. 3, 2004, vol. 13, No. 10, pp. 1327-1344.
Farsiu et al., “Multiframe Demosaicing and Super-Resolution of Color Images”, IEEE Transactions on Image Processing, Jan. 2006, vol. 15, No. 1, date of publication Dec. 12, 2005, pp. 141-159.
Fechteler et al., Fast and High Resolution 3D Face Scanning, IEEE International Conference on Image Processing, Sep. 16-Oct. 19, 2007, 4 pgs.
Fecker et al., “Depth Map Compression for Unstructured Lumigraph Rendering”, Proc. SPIE 6077, Proceedings Visual Communications and Image Processing 2006, Jan. 18, 2006, pp. 60770B-1-60770B-8.
Feris et al., “Multi-Flash Stereopsis: Depth Edge Preserving Stereo with Small Baseline Illumination”, IEEE Trans on PAMI, 2006, 31 pgs.
Fife et al., “A 3D Multi-Aperture Image Sensor Architecture”, Custom Integrated Circuits Conference, 2006, CICC '06, IEEE, pp. 281-284.
Fife et al., “A 3MPixel Multi-Aperture Image Sensor with 0.7Mu Pixels in 0.11Mu CMOS”, ISSCC 2008, Session 2, Image Sensors & Technology, 2008, pp. 48-50.
Fischer et al., “Optical System Design”, 2nd Edition, SPIE Press, Feb. 14, 2008, pp. 49-58.
Fischer et al., “Optical System Design”, 2nd Edition, SPIE Press, Feb. 14, 2008, pp. 191-198.
Garg et al., “Unsupervised CNN for Single View Depth Estimation: Geometry to the Rescue”, In European Conference on Computer Vision, Springer, Cham, Jul. 2016, 16 pgs.
Gastal et al., “Shared Sampling for Real-Time Alpha Matting”, Computer Graphics Forum, EUROGRAPHICS 2010, vol. 29, Issue 2, May 2010, pp. 575-584.
Georgeiv et al., “Light Field Camera Design for Integral View Photography”, Adobe Systems Incorporated, Adobe Technical Report, 2003, 13 pgs.
Georgiev et al., “Light-Field Capture by Multiplexing in the Frequency Domain”, Adobe Systems Incorporated, Adobe Technical Report, 2003, 13 pgs.
Godard et al., “Unsupervised Monocular Depth Estimation with Left-Right Consistency”, In Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition, 2017, 14 pgs.
Goldman et al., “Video Object Annotation, Navigation, and Composition”, In Proceedings of UIST 2008, Oct. 19-22, 2008, Monterey CA, USA, pp. 3-12.
Goodfellow et al., “Generative Adversarial Nets, 2014. Generative adversarial nets”, In Advances in Neural Information Processing Systems (pp. 2672-2680).
Gortler et al., “The Lumigraph”, In Proceedings of SIGGRAPH 1996, published Aug. 1, 1996, pp. 43-54.
Gupta et al., “Perceptual Organization and Recognition of Indoor Scenes from RGB-D Images”, 2013 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 23-28, 2013, Portland, OR, USA, pp. 564-571.
Hacohen et al., “Non-Rigid Dense Correspondence with Applications for Image Enhancement”, ACM Transactions on Graphics, vol. 30, No. 4, Aug. 7, 2011, 9 pgs.
Hamilton, “JPEG File Interchange Format, Version 1.02”, Sep. 1, 1992, 9 pgs.
Hardie, “A Fast Image Super-Algorithm Using an Adaptive Wiener Filter”, IEEE Transactions on Image Processing, Dec. 2007, published Nov. 19, 2007, vol. 16, No. 12, pp. 2953-2964.
Hasinoff et al., “Search-and-Replace Editing for Personal Photo Collections”, 2010 International Conference: Computational Photography (ICCP) Mar. 2010, pp. 1-8.
Hernandez et al., “Laser Scan Quality 3-D Face Modeling Using a Low-Cost Depth Camera”, 20th European Signal Processing Conference, Aug. 27-31, 2012, Bucharest, Romania, pp. 1995-1999.
Hernandez-Lopez et al., “Detecting objects using color and depth segmentation with Kinect sensor”, Procedia Technology, vol. 3, Jan. 1, 2012, pp. 196-204, XP055307680, ISSN: 2212-0173, DOI: 10.1016/j.protcy.2012.03.021.
Higo et al., “A Hand-held Photometric Stereo Camera for 3-D Modeling”, IEEE International Conference on Computer Vision, 2009, pp. 1234-1241.
Hirschmuller, “Accurate and Efficient Stereo Processing by Semi-Global Matching and Mutual Information”, IEEE Conference on Computer Vision and Pattern Recognition (CVPR), San Diego, CA, USA, Jun. 20-26, 2005, 8 pgs.
Hirschmuller et al., “Memory Efficient Semi-Global Matching, ISPRS Annals of the Photogrammetry”, Remote Sensing and Spatial Information Sciences, vol. I-3, 2012, XXII ISPRS Congress, Aug. 25-Sep. 1, 2012, Melbourne, Australia, 6 pgs.
Holoeye Photonics AG, “Spatial Light Modulators”, Oct. 2, 2013, Brochure retrieved from https://web.archive.org/web/20131002061028/http://holoeye.com/wp-content/uploads/Spatial_Light_Modulators.pdf on Oct. 13, 2017, 4 pgs.
Holoeye Photonics AG, “Spatial Light Modulators”, Sep. 18, 2013, retrieved from https://web.archive.org/web/20130918113140/http://holoeye.com/spatial-light-modulators/ on Oct. 13, 2017, 4 pgs.
Holoeye Photonics AG, “LC 2012 Spatial Light Modulator (transmissive)”, Sep. 18, 2013, retrieved from https://web.archive.org/web/20130918151716/http://holoeye.com/spatial-light-modulators/lc-2012-spatial-light-modulator/ on Oct. 20, 2017, 3 pgs.
Horisaki et al., “Superposition Imaging for Three-Dimensionally Space-Invariant Point Spread Functions”, Applied Physics Express, Oct. 13, 2011, vol. 4, pp. 112501-1-112501-3.
Horisaki et al., “Irregular Lens Arrangement Design to Improve Imaging Performance of Compound-Eye Imaging Systems”, Applied Physics Express, Jan. 29, 2010, vol. 3, pp. 022501-1-022501-3.
Horn et al., “LightShop: Interactive Light Field Manipulation and Rendering”, In Proceedings of I3D, Jan. 1, 2007, pp. 121-128.
Hossain et al., “Inexpensive Construction of a 3D Face Model from Stereo Images”, IEEE International Conference on Computerand Information Technology, Dec. 27-29, 2007, 6 pgs.
Hu et al., “A Quantitative Evaluation of Confidence Measures for Stereo Vision”, IEEE Transactions on Pattern Analysis and Machine Intelligence, vol. 34, Issue 11, Nov. 2012, pp. 2121-2133.
Humenberger er al., “A Census-Based Stereo Vision Algorithm Using Modified Semi-Global Matching and Plane Fitting to Improve Matching Quality”, IEEE Computer Society Conference on Computer Vision and Pattern Recognition Workshops (CVPRW), IEEE, Jun. 13-18, 2010, San Francisco, CA, 8 pgs.
Isaksen et al., “Dynamically Reparameterized Light Fields”, In Proceedings of SIGGRAPH 2000, 2000, pp. 297-306.
Izadi et al., “KinectFusion: Real-time 3D Reconstruction and Interaction Using a Moving Depth Camera”, UIST'11, Oct. 16-19, 2011, Santa Barbara, CA, pp. 559-568.
Jackson et al., “Large Post 3D Face Reconstruction from a Single Image via Direct Volumetric CNN Regression”, arXiv: 1703.07834v2, Sep. 8, 2017, 9 pgs.
Janoch et al., “A category-level 3-D object dataset: Putting the Kinect to work”, 2011 IEEE International Conference on Computer Vision Workshops (ICCV Workshops), Nov. 6-13, 2011, Barcelona, Spain, pp. 1168-1174.
Jarabo et al., “Efficient Propagation of Light Field Edits”, In Proceedings of SIACG 2011, 2011, pp. 75-80.
Jiang et al., “Panoramic 3D Reconstruction Using Rotational Stereo Camera with Simple Epipolar Constraints”, 2006 IEEE Computer Society Conference on Computer Vision and Pattern Recognition (CVPR'06), vol. 1, Jun. 17-22, 2006, New York, NY, USA, pp. 371-378.
Joshi, Color Calibration for Arrays of Inexpensive Image Sensors, Mitsubishi Electric Research Laboratories, Inc., TR2004-137, Dec. 2004, 6 pgs.
Joshi et al., “Synthetic Aperture Tracking: Tracking Through Occlusions”, I CCV IEEE 11th International Conference on Computer Vision; Publication [online], Oct. 2007 [retrieved Jul. 28, 2014], Retrieved from the Internet <URL: http:l/ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=4409032&isnumber=4408819>, pp. 1-8.
Jourabloo, “Large-Pose Face Alignment via CNN-Based Dense 3D Model Fitting”, I CCV IEEE 11th International Conference on Computer Vision; Publication [online], Oct. 2007 [retrieved Jul. 28, 2014], Retrieved from the Internet: <URL http:l/ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=4409032&isnumber=4408819>; pp. 1-8.
Kang et al., “Handling Occlusions in Dense Multi-view Stereo”, Computer Vision and Pattern Recognition, 2001, vol. 1, pp. 1-103-1-110.
Keeton, “Memory-Driven Computing”, Hewlett Packard Enterprise Company, Oct. 20, 2016, 45 pgs.
Kim, “Scene Reconstruction from a Light Field”, Master Thesis, Sep. 1, 2010 (Sep. 1, 2010), pp. 1-72.
Kim et al., “Scene reconstruction from high spatio-angular resolution light fields”, ACM Transactions on Graphics (TOG)—SIGGRAPH 2013 Conference Proceedings, vol. 32 Issue 4, Article 73, Jul. 21, 2013, 11 pages.
Kitamura et al., “Reconstruction of a high-resolution image on a compound-eye image-capturing system”, Applied Optics, Mar. 10, 2004, vol. 43, No. 8, pp. 1719-1727.
Kittler et al., “3D Assisted Face Recognition: A Survey of 3D Imaging, Modelling, and Recognition Approaches”, Proceedings of the IEEE Computer Society Conference on Computer Vision and Pattern Recognition, Jul. 2005, 7 pgs.
Konolige, Kurt “Projected Texture Stereo”, 2010 IEEE International Conference on Robotics and Automation, May 3-7, 2010, pp. 148-155.
Kotsia et al., “Facial Expression Recognition in Image Sequences Using Geometric Deformation Features and Support Vector Machines”, IEEE Transactions on Image Processing, Jan. 2007, vol. 16, No. 1, pp. 172-187.
Krishnamurthy et al., “Compression and Transmission of Depth Maps for Image-Based Rendering”, Image Processing, 2001, pp. 828-831.
Kubota et al., “Reconstructing Dense Light Field From Array of Multifocus Images for Novel View Synthesis”, IEEE Transactions on Image Processing, vol. 16, No. 1, Jan. 2007, pp. 269-279.
Kutulakos et al., “Occluding Contour Detection Using Affine Invariants and Purposive Viewpoint Control”, Computer Vision and Pattern Recognition, Proceedings CVPR 94, Seattle, Washington, Jun. 21-23, 1994, 8 pgs.
Lai et al., “A Large-Scale Hierarchical Multi-View RGB-D Object Dataset”, Proceedings—IEEE International Conference on Robotics and Automation, Conference Date May 9-13, 2011, 8 pgs., DOI:10.1109/ICRA.201135980382.
Lane et al., “A Survey of Mobile Phone Sensing”, IEEE Communications Magazine, vol. 48, Issue 9, Sep. 2010, pp. 140-150.
Lao et al., “3D template matching for pose invariant face recognition using 3D facial model built with isoluminance line based stereo vision”, Proceedings 15th International Conference on Pattern Recognition, Sep. 3-7, 2000, Barcelona, Spain, pp. 911-916.
Lee, “NFC Hacking: The Easy Way”, Defcon Hacking Conference, 2012, 24 pgs.
Lee et al., “Electroactive Polymer Actuator for Lens-Drive Unit in Auto-Focus Compact Camera Module”, ETRI Journal, vol. 31, No. 6, Dec. 2009, pp. 695-702.
Lee et al., “Nonlocal matting”, CVPR 2011, Jun. 20-25, 2011, pp. 2193-2200.
Lee et al., “Automatic Upright Adjustment of Photographs”, IEEE Conference on Computer Vision and Pattern Recognition (CVPR), 2012, pp. 877-884.
Lensvector, “How LensVector Autofocus Works”, 2010, printed Nov. 2, 2012 from http://www.lensvector.com/overview.html, 1 pg.
Levin et al., “A Closed Form Solution to Natural Image Matting”, IEEE Conference on Computer Vision and Pattern Recognition (CVPR), 2006, vol. 1, pp. 61-68.
Levin et al., “Spectral Matting”, 2007 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 17-22, 2007, Minneapolis, MN, USA, pp. 1-8.
Levoy, “Light Fields and Computational Imaging”, IEEE Computer Society, Sep. 1, 2006, vol. 39, Issue No. 8, pp. 46-55.
Levoy et al., “Light Field Rendering”, Proc. ADM SIGGRAPH '96, 1996, pp. 1-12.
Li et al., “A Hybrid Camera for Motion Deblurring and Depth Map Super-Resolution”, Jun. 23-28, 2008, IEEE Conference on Computer Vision and Pattern Recognition, 8 pgs. Retrieved from www.eecis.udel.edu/˜jye/lab_research/08/deblur-feng.pdf on Feb. 5, 2014.
Li et al., “Fusing Images with Different Focuses Using Support Vector Machines”, IEEE Transactions on Neural Networks, vol. 15, No. 6, Nov. 8, 2004, pp. 1555-1561.
Lim, “Optimized Projection Pattern Supplementing Stereo Systems”, 2009 IEEE International Conference on Robotics and Automation, May 12-17, 2009, pp. 2823-2829.
Liu et al., “Virtual View Reconstruction Using Temporal Information”, 2012 IEEE International Conference on Multimedia and Expo, 2012, pp. 115-120.
Lo et al., “Stereoscopic 3D Copy & Paste”, ACM Transactions on Graphics, vol. 29, No. 6, Article 147, Dec. 2010, pp. 147:1-147:10.
Ma et al., “Constant Time Weighted Median Filtering for Stereo Matching and Beyond”, ICCV'13 Proceedings of the 2013 IEEE International Conference on Computer Vision, IEEE Computer Society, Washington DC, USA, Dec. 1-8, 2013, 8 pgs.
Martinez et al., “Simple Telemedicine for Developing Regions: Camera Phones and Paper-Based Microfluidic Devices for Real-Time, Off-Site Diagnosis”, Analytical Chemistry (American Chemical Society), vol. 80, No. 10, May 15, 2008, pp. 3699-3707.
McGuire et al., “Defocus video matting”, ACM Transactions on Graphics (TOG)—Proceedings of ACM SIGGRAPH 2005, vol. 24, Issue 3, Jul. 2005, pp. 567-576.
Medioni et al., “Face Modeling and Recognition in 3-D”, Proceedings of the IEEE International Workshop on Analysis and Modeling of Faces and Gestures, 2013, 2 pgs.
Merkle et al., “Adaptation and optimization of coding algorithms for mobile 3DTV”, Mobile3DTV Project No. 216503, Nov. 2008, 55 pgs.
Michael et al., “Real-time Stereo Vision: Optimizing Semi-Global Matching”, 2013 IEEE Intelligent Vehicles Symposium (IV), IEEE, Jun. 23-26, 2013, Australia, 6 pgs.
Milella et al., “3D reconstruction and classification of natural environments by an autonomous vehicle using multi-baseline stereo”, Intelligent Service Robotics, vol. 7, No. 2, Mar. 2, 2014, pp. 79-92.
Min et al., “Real-Time 3D Face Identification from a Depth Camera”, Proceedings of the IEEE International Conference on Pattern Recognition, Nov. 11-15, 2012, 4 pgs.
Mitra et al., “Light Field Denoising, Light Field Superresolution and Stereo Camera Based Refocussing using a GMM Light Field Patch Prior”, Computer Vision and Pattern Recognition Workshops (CVPRW), 2012 IEEE Computer Society Conference on Jun. 16-21, 2012, pp. 22-28.
Moreno-Noguer et al., “Active Refocusing of Images and Videos”, ACM Transactions on Graphics (TOG)—Proceedings of ACM SIGGRAPH 2007, vol. 26, Issue 3, Jul. 2007, 10 pgs.
Muehlebach, “Camera Auto Exposure Control for VSLAM Applications”, Studies on Mechatronics, Swiss Federal Institute of Technology Zurich, Autumn Term 2010 course, 67 pgs.
Nayar, “Computational Cameras: Redefining the Image”, IEEE Computer Society, Aug. 14, 2006, pp. 30-38.
Ng, “Digital Light Field Photography”, Thesis, Jul. 2006, 203 pgs.
Ng et al., “Super-Resolution Image Restoration from Blurred Low-Resolution Images”, Journal of Mathematical Imaging and Vision, 2005, vol. 23, pp. 367-378.
Ng et al., “Light Field Photography with a Hand-held Plenoptic Camera”, Stanford Tech Report CTSR 2005-02, Apr. 20, 2005, pp. 1-11.
Nguyen et al., “Image-Based Rendering with Depth Information Using the Propagation Algorithm”, Proceedings. (ICASSP '05). IEEE International Conference on Acoustics, Speech, and Signal Processing, 2005, vol. 5, Mar. 23-23, 2005, pp. II-589-II-592.
Nguyen et al., “Error Analysis for Image-Based Rendering with Depth Information”, IEEE Transactions on Image Processing, vol. 18, Issue 4, Apr. 2009, pp. 703-716.
Nishihara, H.K. “PRISM: A Practical Real-Time Imaging Stereo Matcher”, Massachusetts Institute of Technology, A.I. Memo 780, May 1984, 32 pgs.
Nitta et al., “Image reconstruction for thin observation module by bound optics by using the iterative backprojection method”, Applied Optics, May 1, 2006, vol. 45, No. 13, pp. 2893-2900.
Nomura et al., “Scene Collages and Flexible Camera Arrays”, Proceedings of Eurographics Symposium on Rendering, Jun. 2007, 12 pgs.
Park et al., “Super-Resolution Image Reconstruction”, IEEE Signal Processing Magazine, May 2003, pp. 21-36.
Park et al., “Multispectral Imaging Using Multiplexed Illumination”, 2007 IEEE 11th International Conference on Computer Vision, Oct. 14-21, 2007, Rio de Janeiro, Brazil, pp. 1-8.
Park et al., “3D Face Reconstruction from Stereo Video”, First International Workshop on Video Processing for Security, Jun. 7-9, 2006, Quebec City, Canada, 2006, 8 pgs.
Parkkinen et al., “Characteristic Spectra of Munsell Colors”, Journal of the Optical Society of America A, vol. 6, Issue 2, Feb. 1989, pp. 318-322.
Perwass et al., “Single Lens 3D-Camera with Extended Depth-of-Field”, printed from www.raytrix.de, Jan. 22, 2012, 15 pgs.
Pham et al., “Robust Super-Resolution without Regularization”, Journal of Physics: Conference Series 124, Jul. 2008, pp. 1-19.
Philips 3D Solutions, “3D Interface Specifications, White Paper”, Feb. 15, 2008, 2005-2008 Philips Electronics Nederland B.V., Philips 3D Solutions retrieved from www.philips.com/3dsolutions, 29 pgs.
Polight, “Designing Imaging Products Using Reflowable Autofocus Lenses”, printed Nov. 2, 2012 from http://www.polight.no/tunable-polymer-autofocus-lens-html--11.html, 1 pg.
Pouydebasque et al., “Varifocal liquid lenses with integrated actuator, high focusing power and low operating voltage fabricated on 200 mm wafers”, Sensors and Actuators A: Physical, vol. 172, Issue 1, Dec. 2011, pp. 280-286.
Protter et al., “Generalizing the Nonlocal-Means to Super-Resolution Reconstruction”, IEEE Transactions on Image Processing, Dec. 2, 2008, vol. 18, No. 1, pp. 36-51.
Radtke et al., “Laser lithographic fabrication and characterization of a spherical artificial compound eye”, Optics Express, Mar. 19, 2007, vol. 15, No. 6, pp. 3067-3077.
Rajan et al., “Simultaneous Estimation of Super Resolved Scene and Depth Map from Low Resolution Defocused Observations”, IEEE Transactions on Pattern Analysis and Machine Intelligence, vol. 25, No. 9, Sep. 8, 2003, pp. 1-16.
Rander et al., “Virtualized Reality: Constructing Time-Varying Virtual Worlds from Real World Events”, Proc. of IEEE Visualization '97, Phoenix, Arizona, Oct. 19-24, 1997, pp. 277-283, 552.
Ranjan et al., “HyperFace: A Deep Multi-Task Learning Framework for Face Detection, Landmark Localization, Pose Estimation, and Gender Recognition”, May 11, 2016 (May 11, 2016), pp. 1-16.
Rhemann et al., “Fast Cost-Volume Filtering for Visual Correspondence and Beyond”, IEEE Trans. Pattern Anal. Mach. Intell, 2013, vol. 35, No. 2, pp. 504-511.
Rhemann et al., “A perceptually motivated online benchmark for image matting”, 2009 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 20-25, 2009, Miami, FL, USA, pp. 1826-1833.
Robert et al., “Dense Depth Map Reconstruction: A Minimization and Regularization Approach which Preserves Discontinuities”, European Conference on Computer Vision (ECCV), pp. 439-451, (1996).
Robertson et al., “Dynamic Range Improvement Through Multiple Exposures”, In Proc. of the Int. Conf. on Image Processing, 1999, 5 pgs.
Robertson et al., “Estimation-theoretic approach to dynamic range enhancement using multiple exposures”, Journal of Electronic Imaging, Apr. 2003, vol. 12, No. 2, pp. 219-228.
Roy et al., “Non-Uniform Hierarchical Pyramid Stereo for Large Images”, Computer and Robot Vision, 2002, pp. 208-215.
Rusinkiewicz et al., “Real-Time 3D Model Acquisition”, ACM Transactions on Graphics (TOG), vol. 21, No. 3, Jul. 2002, pp. 438-446.
Saatci et al., “Cascaded Classification of Gender and Facial Expression using Active Appearance Models”, IEEE, FGR'06, 2006, 6 pgs.
Sauer et al., “Parallel Computation of Sequential Pixel Updates in Statistical Tomographic Reconstruction”, ICIP 1995 Proceedings of the 1995 International Conference on Image Processing, Date of Conference: Oct. 23-26, 1995, pp. 93-96.
Scharstein et al., “High-Accuracy Stereo Depth Maps Using Structured Light”, IEEE Computer Society Conference on Computer Vision and Pattern Recognition (CVPR 2003), Jun. 2003, vol. 1, pp. 195-202.
Seitz et al., “Plenoptic Image Editing”, International Journal of Computer Vision 48, Conference Date Jan. 7, 1998, 29 pgs., DOI: 10.1109/ICCV.1998.710696 ⋅ Source: DBLP Conference: Computer Vision, Sixth International Conference.
Shechtman et al., “Increasing Space-Time Resolution in Video”, European Conference on Computer Vision, LNCS 2350, May 28-31, 2002, pp. 753-768.
Shotton et al., “Real-time human pose recognition in parts from single depth images”, CVPR 2011, Jun. 20-25, 2011, Colorado Springs, CO, USA, pp. 1297-1304.
Shum et al., “Pop-Up Light Field: An Interactive Image-Based Modeling and Rendering System”, Apr. 2004, ACM Transactions on Graphics, vol. 23, No. 2, pp. 143-162, Retrieved from http://131.107.65.14/en-us/um/people/jiansun/papers/PopupLightField_TOG.pdf on Feb. 5, 2014.
Shum et al., “A Review of Image-based Rendering Techniques”, Visual Communications and Image Processing 2000, May 2000, 12 pgs.
Sibbing et al., “Markerless reconstruction of dynamic facial expressions”, 2009 IEEE 12th International Conference on Computer Vision Workshops, ICCV Workshop: Kyoto, Japan, Sep. 27-Oct. 4, 2009, Institute of Electrical and Electronics Engineers, Piscataway, NJ, Sep. 27, 2009 (Sep. 27, 2009), pp. 1778-1785.
Silberman et al., “Indoor segmentation and support inference from RGBD images”, ECCV'12 Proceedings of the 12th European conference on Computer Vision, vol. Part V, Oct. 7-13, 2012, Florence, Italy, pp. 746-760.
Stober, “Stanford researchers developing 3-D camera with 12,616 lenses”, Stanford Report, Mar. 19, 2008, Retrieved from: http://news.stanford.edu/news/2008/march19/camera-031908.html, 5 pgs.
Stollberg et al., “The Gabor superlens as an alternative wafer-level camera approach inspired by superposition compound eyes of nocturnal insects”, Optics Express, Aug. 31, 2009, vol. 17, No. 18, pp. 15747-15759.
Sun et al., “Image Super-Resolution Using Gradient Profile Prior”, 2008 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 23-28, 2008, 8 pgs.; DOI: 10.1109/CVPR.2008.4587659.
Taguchi et al., “Rendering-Oriented Decoding fora Distributed Multiview Coding System Using a Coset Code”, Hindawi Publishing Corporation, EURASIP Journal on Image and Video Processing, vol. 2009, Article ID 251081, Online: Apr. 22, 2009, 12 pgs.
Takeda et al., “Super-resolution Without Explicit Subpixel Motion Estimation”, IEEE Transaction on Image Processing, Sep. 2009, vol. 18, No. 9, pp. 1958-1975.
Tallon et al., “Upsampling and Denoising of Depth Maps Via Joint-Segmentation”, 20th European Signal Processing Conference, Aug. 27-31, 2012, 5 pgs.
Tanida et al., “Thin observation module by bound optics (TOMBO): concept and experimental verification”, Applied Optics, Apr. 10, 2001, vol. 40, No. 11, pp. 1806-1813.
Tanida et al., “Color imaging with an integrated compound imaging system”, Optics Express, Sep. 8, 2003, vol. 11, No. 18, pp. 2109-2117.
Tao et al., “Depth from Combining Defocus and Correspondence Using Light-Field Cameras”, ICCV '13 Proceedings of the 2013 IEEE International Conference on Computer Vision, Dec. 1, 2013, pp. 673-680.
Taylor, “Virtual camera movement: The way of the future?”, American Cinematographer, vol. 77, No. 9, Sep. 1996, pp. 93-100.
Tseng et al., “Automatic 3-D depth recovery from a single urban-scene image”, 2012 Visual Communications and Image Processing, Nov. 27-30, 2012, San Diego, CA, USA, pp. 1-6.
Uchida et al., 3D Face Recognition Using Passive Stereo Vision, IEEE International Conference on Image Processing 2005, Sep. 14, 2005, 4 pgs.
Vaish et al., “Reconstructing Occluded Surfaces Using Synthetic Apertures: Stereo, Focus and Robust Measures”, 2006 IEEE Computer Society Conference on Computer Vision and Pattern Recognition (CVPR'06), vol. 2, Jun. 17-22, 2006, pp. 2331-2338.
Vaish et al., “Using Plane + Parallax for Calibrating Dense Camera Arrays”, IEEE Conference on Computer Vision and Pattern Recognition (CVPR), 2004, 8 pgs.
Vaish et al., “Synthetic Aperture Focusing Using a Shear-Warp Factorization of the Viewing Transform”, IEEE Workshop on A3DISS, CVPR, 2005, 8 pgs.
Van Der Wal et al., “The Acadia Vision Processor”, Proceedings Fifth IEEE International Workshop on Computer Architectures for Machine Perception, Sep. 13, 2000, Padova, Italy, pp. 31-40.
Veilleux, “CCD Gain Lab: The Theory”, University of Maryland, College Park-Observational Astronomy (ASTR 310), Oct. 19, 2006, pp. 1-5 (online], [retrieved on May 13, 2014], Retrieved from the Internet <URL: http://www.astro.umd.edu/˜veilleux/ASTR310/fall06/ccd_theory.pdf, 5 pgs.
Venkataraman et al., “PiCam: An Ultra-Thin High Performance Monolithic Camera Array”, ACM Transactions on Graphics (TOG), ACM, US, vol. 32, No. 6, 1 Nov. 1, 2013, pp. 1-13.
Vetro et al., “Coding Approaches for End-To-End 3D TV Systems”, Mitsubishi Electric Research Laboratories, Inc., TR2004-137, Dec. 2004, 6 pgs.
Viola et al., “Robust Real-time Object Detection”, Cambridge Research Laboratory, Technical Report Series, Compaq, CRL 2001/01, Feb. 2001, Printed from: http://www.hpl.hp.com/techreports/Compaq-DEC/CRL-2001-1.pdf, 30 pgs.
Vuong et al., “A New Auto Exposure and Auto White-Balance Algorithm to Detect High Dynamic Range Conditions Using CMOS Technology”, Proceedings of the World Congress on Engineering and Computer Science 2008, WCECS 2008, Oct. 22-24, 2008, 5 pgs.
Wang, “Calculation of Image Position, Size and Orientation Using First Order Properties”, Dec. 29, 2010, OPTI521 Tutorial, 10 pgs.
Wang et al., “Soft scissors: an interactive tool for realtime high quality matting”, ACM Transactions on Graphics (TOG)—Proceedings of ACM SIGGRAPH 2007, vol. 26, Issue 3, Article 9, Jul. 2007, 6 pg., published Aug. 5, 2007.
Wang et al., “Automatic Natural Video Matting with Depth”, 15th Pacific Conference on Computer Graphics and Applications, PG '07, Oct. 29-Nov. 2, 2007, Maui, HI, USA, pp. 469-472.
Wang et al., “Image and Video Matting: A Survey”, Foundations and Trends, Computer Graphics and Vision, vol. 3, No. 2, 2007, pp. 91-175.
Wang et al., “Facial Feature Point Detection: A Comprehensive Survey”, arXiv: 1410.1037v1, Oct. 4, 2014, 32 pgs.
Wetzstein et al., “Computational Plenoptic Imaging”, Computer Graphics Forum, 2011, vol. 30, No. 8, pp. 2397-2426.
Wheeler et al., “Super-Resolution Image Synthesis Using Projections Onto Convex Sets in the Frequency Domain”, Proc. SPIE, Mar. 11, 2005, vol. 5674, 12 pgs.
Widanagamaachchi et al., “3D Face Recognition from 2D Images: A Survey”, Proceedings of the International Conference on Digital Image Computing: Techniques and Applications, Dec. 1-3, 2008, 7 pgs.
Wieringa et al., “Remote Non-invasive Stereoscopic Imaging of Blood Vessels: First In-vivo Results of a New Multispectral Contrast Enhancement Technology”, Annals of Biomedical Engineering, vol. 34, No. 12, Dec. 2006, pp. 1870-1878, Published online Oct. 12, 2006.
Wikipedia, “Polarizing Filter (Photography)”, retrieved from http://en.wikipedia.org/wiki/Polarizing_filter_(photography) on Dec. 12, 2012, last modified on Sep. 26, 2012, 5 pgs.
Wilburn, “High Performance Imaging Using Arrays of Inexpensive Cameras”, Thesis of Bennett Wilburn, Dec. 2004, 128 pgs.
Wilburn et al., “High Performance Imaging Using Large Camera Arrays”, ACM Transactions on Graphics, Jul. 2005, vol. 24, No. 3, pp. 1-12.
Wilburn et al., “High-Speed Videography Using a Dense Camera Array”, Proceedings of the 2004 IEEE Computer Society Conference on Computer Vision and Pattern Recognition, 2004. CVPR 2004., vol. 2, Jun. 27-Jul. 2, 2004, pp. 294-301.
Wilburn et al., “The Light Field Video Camera”, Proceedings of Media Processors 2002, SPIE Electronic Imaging, 2002, 8 pgs.
Wippermann et al., “Design and fabrication of a chirped array of refractive ellipsoidal micro-lenses for an apposition eye camera objective”, Proceedings of SPIE, Optical Design and Engineering II, Oct. 15, 2005, pp. 59622C-1-59622C-11.
Wu et al., “A virtual view synthesis algorithm based on image inpainting”, 2012 Third International Conference on Networking and Distributed Computing, Hangzhou, China, Oct. 21-24, 2012, pp. 153-156.
Xu, “Real-Time Realistic Rendering and High Dynamic Range Image Display and Compression”, Dissertation, School of Computer Science in the College of Engineering and Computer Science at the University of Central Florida, Orlando, Florida, Fall Term 2005, 192 pgs.
Yang et al., “Superresolution Using Preconditioned Conjugate Gradient Method”, Proceedings of SPIE—The International Society for Optical Engineering, Jul. 2002, 8 pgs.
Yang et al., “A Real-Time Distributed Light Field Camera”, Eurographics Workshop on Rendering (2002), published Jul. 26, 2002, pp. 1-10.
Yang et al., Model-based Head Pose Tracking with Stereovision, Microsoft Research, Technical Report, MSR-TR-2001-102, Oct. 2001, 12 pgs.
Yokochi et al., “Extrinsic Camera Parameter Estimation Based-on Feature Tracking and GPS Data”, 2006, Nara Institute of Science and Technology, Graduate School of Information Science, LNCS 3851, pp. 369-378.
Zbontar et al., Computing the Stereo Matching Cost with a Convolutional Neural Network, CVPR, 2015, pp. 1592-1599.
Zhang et al., “A Self-Reconfigurable Camera Array”, Eurographics Symposium on Rendering, published Aug. 8, 2004, 12 pgs.
Zhang et al., “Depth estimation, spatially variant image registration, and super-resolution using a multi-lenslet camera”, proceedings of SPIE, vol. 7705, Apr. 23, 2010, pp. 770505-770505-8, XP055113797 ISSN: 0277-786X, DOI: 10.1117/12.852171.
Zhang et al., “Spacetime Faces: High Resolution Capture for Modeling and Animation”, ACM Transactions on Graphics, 2004, 11pgs.
Zheng et al., “Balloon Motion Estimation Using Two Frames”, Proceedings of the Asilomar Conference on Signals, Systems and Computers, IEEE, Comp. Soc. Press, US, vol. 2 of 2, Nov. 4, 1991, pp. 1057-1061.
Zhu et al., “Fusion of Time-of-Flight Depth and Stereo for High Accuracy Depth Maps”, 2008 IEEE Conference on Computer Vision and Pattern Recognition, Jun. 23-28, 2008, Anchorage, AK, USA, pp. 1-8.
Zomet et al., “Robust Super-Resolution”, IEEE, 2001, pp. 1-6.
“File Formats Version 6”, Alias Systems, 2004, 40 pgs.
“Light fields and computational photography”, Stanford Computer Graphics Laboratory, Retrieved from: http://graphics.stanford.edu/projects/lightfield/, Earliest publication online: Feb. 10, 1997, 3 pgs.
“Exchangeable image file format for digital still cameras: Exif Version 2.2”_, Japan Electronics and Information Technology Industries Association, Prepared by Technical Standardization Committee on AV & IT Storage Systems and Equipment, JEITA CP-3451, Apr. 2002, Retrieved from: http://www.exif.org/Exif2-2.PDF, 154 pgs.
International Preliminary Report on Patentability International Application No. PCT/US21/12073, dated Aug. 11, 2022, 7 pages.
Chen et al., “Fast patch-based style transfer of arbitrary style,” CoRR, Dec. 13, 2016, arXiv:1612.04337, 10 pages.
Deng et al., “ImageNet: A Large-Scale Hierarchical Image Database,” IEEE Computer Vision and Pattern Recognition (CVPR), Jun. 20-25, 2009, 8 pages.
Dundar et al., “Domain stylization: A strong, simple baseline for synthetic to real image domain adaptation,” CoRR, Jul. 24, 2018, arXiv:1807.09384, 10 pages.
Karras et al., “Analyzing and improving the image quality of stylegan,” Proceedings of the IEEE/CVF Conference on Computer Vision and Pattern Recognition (CVPR), 2020, pp. 8110-8119.
Liu et al., “Somewhere over the rainbow: An empirical assessment of quantitative colormaps,” Proceedings of the 2018 CHI Conference on Human Factors in Computing Systems, Apr. 2018, 598:1-12.
Ramamoorthi et al., “A Signal-Processing Framework for Inverse Rendering,” Proceedings of the 28th Annual Conference on Computer Graphics and Interactive Techniques, Aug. 2001, pp. 117-128.
Ramamoorthi, “A Signal-Processing Framework for Forward and Inverse Rendering,” Dissertation for the degree of Doctor of Philosophy, Stanford University, Department of Computer Science, Aug. 2002, 207 pages.
Smirnov et al., “Hard example mining with auxiliary embeddings,” Proceedings of the IEEE Conference on Computer Vision and Pattern Recognition Workshops (CVPR), 2018, pp. 37-46.
Related Publications (1)
Number Date Country
20220215266 A1 Jul 2022 US
Provisional Applications (1)
Number Date Country
62968038 Jan 2020 US