The present invention relates generally to the field of sensing and, more specifically, to Light Detection and Ranging (LIDAR) sensing arrangements.
LIDAR systems use light for detecting a distance between a light source and a target. A collimated beam (e.g., a laser) is directed towards the target. LIDAR systems typically identify the time it takes for light to reach the target, be deflected off the target, and return to a detector. Based on this time and the speed of light, a distance to the target is determined.
The present technology provides improved LIDAR systems that are capable of capturing more extensive areas of an external environment.
In one implementation of the present technology, a LIDAR sensing system is disclosed. The LIDAR sensing system includes a light source arranged to project a collimated beam along a path. The light source is configured to adjust a wavelength of the projected collimated beam. The LIDAR sensing system includes an interferometer that splits the collimated beam into 1) a reference beam and 2) an object beam that is directed into an external environment of the LIDAR sensing system. The LIDAR sensing system includes diffraction grating arranged along the path of the object beam. The light source projects the collimated beam onto the diffraction grating at an incident angle via the interferometer, and the diffraction grating diffracts the collimated beam into the external environment at one of multiple diffraction angles according to the wavelength of the collimated beam. The LIDAR sensing system includes a detector that detects interference patterns generated by the interferometer and corresponding to 1) light reflected off objects located in the external environment and 2) the reference beam. The LIDAR sensing system includes a computing system including a processing circuit. The processing circuit includes a processor and memory. The memory is structured to store instructions that, when executed by the processor, cause the processor to generate a scan along an axis of the external environment. The instructions to generate the scan along the axis of the external environment include instructions to control the light source to project the collimated beam at a first wavelength at a first time and at a second wavelength at a second time. The object beam is diffracted from the diffraction grating at a first diffraction angle when the collimated beam is projected at the first wavelength. The object beam is diffracted from the diffraction grating at a second diffraction angle when the collimated beam is projected at the second wavelength. The first diffraction angle and the second diffraction angle define a field of view along the axis. The instructions to generate the scan along the axis of the external environment include instructions to calculate distances associated with objects located within the field of view based on the interference patterns detected by the detector.
In another implementation of the present technology, a LIDAR sensing system is disclosed. The LIDAR sensing system includes a light source arranged to project a collimated beam along a path. The light source is configured to adjust a wavelength of the projected collimated beam. The LIDAR sensing system includes an interferometer that splits the collimated beam into 1) a reference beam and 2) an object beam that is directed into an external environment of the LIDAR sensing system. The LIDAR sensing system includes a detector that detects interference patterns generated by the interferometer and corresponding to 1) light reflected off objects located in the external environment and 2) the reference beam. The LIDAR sensing system includes a computing system including a processing circuit. The processing circuit includes a processor and memory. The memory is structured to store instructions that, when executed by the processor, cause the processor to generate a scan along an axis of the external environment. The instructions to generate the scan along the axis of the external environment include instructions to control the light source to sweep a wavelength of the collimated beam through a plurality of incremental wavelengths between a first wavelength and a second wavelength. The instructions to generate the scan along the axis of the external environment include instructions to calculate distances associated with objects located within the field of view based on the interference patterns detected by the detector as the light source is controlled to sweep the wavelength of the collimated beam. The distances are calculated at each incremental wavelength as the light source is swept between the first wavelength and the second wavelength.
In another implementation of the present technology, a method of LIDAR sensing is described. The method includes controlling a light source to project a collimated beam at a first wavelength at a first time and at a second wavelength at a second time. The collimated beam is projected towards diffraction grating via an interferometer that splits the collimated beam into a reference beam and an object beam. The diffraction grating diffracts the object beam into the external environment at one of multiple diffraction angles according to the wavelength of the object beam. The object beam is diffracted from the diffraction grating at a first diffraction angle when the collimated beam is projected at the first wavelength. The object beam is diffracted from the diffraction grating at a second diffraction angle when the collimated beam is projected at the second wavelength. The first diffraction angle and the second diffraction angle define a field of view along an axis. The method includes calculating distances associated with objects located within the field of view based on interference patterns generated by the interferometer and detected by a detector. The interference patterns are generated based on 1) light corresponding to the object beam being reflected off objects in the external environment and 2) the reference beam reflected off a reference mirror.
In another implementation of the present technology, a method of LIDAR sensing is described. The method includes controlling a light source to project the collimated beam at a first wavelength at a first time, wherein an object beam corresponding to the collimated beam is diffracted from diffraction grating at a first diffraction angle. The method includes performing frequency analysis on a signal from a detector and corresponding to an interference pattern to identify one or more frequency characteristics of the signal, the interference pattern being generated based on 1) light corresponding to the object beam being reflected off an object in an external environment and 2) a reference beam reflected off a reference mirror. The method includes calculating distances based on the one or more frequency characteristics of the signal. The method includes controlling the light source to project the collimated beam at a second wavelength, the object beam being diffracted from the diffraction grating at a second diffraction angle different from the first diffraction angle, whereby the first diffraction angle and the second diffraction angle define a field of view along an axis.
The foregoing summary is illustrative only and is not intended to be in any way limiting. In addition to the illustrative aspects and features described above, further aspects and features will become apparent by reference to the following drawings and the detailed description.
The foregoing and other features of the present disclosure will become more fully apparent from the following description and appended claims, taken in conjunction with the accompanying drawings. Understanding that these drawings depict only several implementations in accordance with the disclosure and are, therefore, not to be considered limiting of its scope, the disclosure will be described with additional specificity and detail through use of the accompanying drawings.
In the following detailed description, reference is made to the accompanying drawings, which form a part hereof. In the drawings, similar symbols typically identify similar components, unless context dictates otherwise. The illustrative implementations described in the detailed description, drawings, and claims are not meant to be limiting. Other implementations may be utilized, and other changes may be made, without departing from the spirit or scope of the subject matter presented here. It will be readily understood that the aspects of the present disclosure, as generally described herein, and illustrated in the figures, may be arranged, substituted, combined, and designed in a wide variety of different configurations, all of which are explicitly contemplated and make part of this disclosure.
Described herein are systems and methods for LIDAR sensing.
As will be discussed in further detail below, a LIDAR sensing system includes a light source that is controlled to project a collimated beam at various wavelengths. An interferometer receives the collimated beam and projects an object beam corresponding to the collimated beam at a diffraction grating. The object beam is diffracted from the diffraction grating at different angles corresponding to the wavelength of the collimated beam. As a result, the LIDAR sensing system generates a vertical scan (e.g., a two-dimensional scan) of the external environment. Various components of the LIDAR sensing system are then configured to rotate to produce multiple vertical scans, thus generating a three-dimensional scan.
Referring to
In
The light source 102 may be arranged to project components of the collimated beam onto the diffraction grating 104. For instance, the diffraction grating 104 may be arranged along a path of an object beam corresponding to the collimated beam projected from the light source 102. As will be discussed in greater detail below with respect to
In some examples, light from the object beam reflects off a surface of an object located in an external environment 106 of the LIDAR sensing system 100. The light reflected off the surface of the object may then be detected by the LIDAR sensing system 100 and used for determining a distance to the object.
Referring now to
The LIDAR sensing system 100 may include an interferometer 110. The interferometer 110 may be or include components arranged to receive the collimated beam from the light source 102, and split the collimated beam into one or more component beams. For instance, the interferometer 110 may split the collimated beam into an object beam and a reference beam. The object beam may be projected towards the diffraction grating 104, and the reference beam may be projected towards a reference mirror 206. The interferometer 110 may generate an interference pattern based on a difference between light reflected off surfaces of objects in the external environment 106 and light reflected off the reference mirror 206. The LIDAR sensing system 100 may determine a distance to the objects based on the interference pattern.
For instance, the object beam reflected off the object 200 may return to the diffraction grating 104, diffract from the diffraction grating 104 to the interferometer 110, and the detector 202 may detect an interference pattern from the interferometer 110. The detector 202 may generate signals based on the interference pattern. The signals from the detector 202 may be used for determining the distance to the corresponding objects located in the external environment 106.
The LIDAR sensing system 100 may include a computing system 112. The computing system 112 may include a processor 114 and memory 116. The processor 114 may include any component or group of components that are configured to execute, implement, and/or perform any of the processes or functions described herein or any form of instructions to carry out such processes or cause such processes to be performed. In one or more arrangements, the processor 114 may be a main processor of the LIDAR sensing system 100. Examples of suitable processors include microprocessors, microcontrollers, DSP processors, and other circuitry that may execute software. Further examples of suitable processors include, but are not limited to, a central processing unit (CPU), an array processor, a vector processor, a digital signal processor (DSP), a field-programmable gate array (FPGA), a programmable logic array (PLA), an application specific integrated circuit (ASIC), programmable logic circuitry, and a controller. The processor 114 may include at least one hardware circuit (e.g., an integrated circuit) configured to carry out instructions contained in program code. In arrangements in which there is a plurality of processors, such processors may work independently from each other or one or more processors may work in combination with each other.
The memory 116 may be structured for storing one or more types of data. The memory 116 store may include volatile and/or non-volatile memory. Examples of suitable memory 116 include RAM (Random Access Memory), flash memory, ROM (Read Only Memory), PROM (Programmable Read-Only Memory), EPROM (Erasable Programmable Read-Only Memory), EEPROM (Electrically Erasable Programmable Read-Only Memory), registers, magnetic disks, optical disks, hard drives, or any other suitable storage medium, or any combination thereof. The memory 116 may be a component of the processor 114, or the memory 116 may be operatively connected to the processor 114 for use thereby. In some arrangements, the memory 116 may be located remotely and accessible by the processor 114, such as via a suitable communications device.
The LIDAR sensing system 100 may include a light source controller 118. The light source controller 118 may be or include computer-readable instructions to control one or more aspects of the light source 102. The light source controller 118 may be stored on memory 116 as shown. In other implementations, the light source controller 118 may be stored remotely and accessible by various components of the LIDAR sensing system 100. The processor 114 may control the light source 102 in accordance with the instructions from the light source controller 118.
The light source controller 118 may include instructions to generate a pattern for the collimated beam projected from the light source 102. For instance, in some implementations, the collimated beam may be projected from the light source 102 in a pattern 204 having a frequency (e.g., pulsed, saw tooth, etc.). The light source controller 118 may include instructions to generate, for example, a saw tooth signal 204 that corresponds to the frequency pattern of the collimated beam projected from the light source 102. As will be discussed in further detail below, the frequency pattern may be used for determining a distance between the object and the LIDAR sensing system 100.
Referring now to
The signal generated by the detector 202 may correspond to the signal generated by the light source controller 118 and projected via the light source 102 onto the object 102. In some implementations, the light source 102 may be arranged to project the collimated beam both onto the object 200 and the reference mirror 206 (e.g., through the interferometer 110). The reference mirror 206 may be located at a fixed distance D from a point (e.g., from the interferometer 110, for example). The object 200 may be located a distance away that is equal to the sum of the fixed distance D and the range R to the object 200.
When light from the light source 102 is projected in a pattern (e.g., the saw tooth pattern 204 shown in
Referring now to
The reference signal 300 and object signal 302 are shown in
where c is the speed of light, ƒbeat is the beat frequency, Δƒ is the range of frequencies, and tm is the ramp period (e.g., the time between t1 and t2). Where the fixed distance D between the reference mirror 206 and a point in the LIDAR sensing system 100 (e.g., interferometer 110) is known, the distance between the object and the same point is the sum of the fixed distance D and R (as shown in
In some implementations, the LIDAR sensing system 100 may calculate the distance instantaneously (or substantially instantaneously). In implementations such as these, the LIDAR sensing system 100 may calculate the distance according to equation (2):
is the instantaneous slope of the frequency ramp, and dtm is the ramp increment. Implementation such as these can compensate for any nonlinearity of frequency ramp of tunable light source 102, which may increase reliability of the distance calculations.
In some implementations, the LIDAR sensing system 100 may include the interferometer 110 (e.g., a main interferometer) and an auxiliary interferometer. The auxiliary interferometer may be substantially the same as the main interferometer. Additionally, the LIDAR sensing system 100 may include the detector 202 (e.g., a main detector) and an auxiliary detector. The auxiliary detector may be substantially the same as the main detector. The auxiliary interferometer may be arranged to receive the collimated beam from the light source 102. The auxiliary interferometer may split the collimated beam from the light source 102 into two beams, each of which is located at a fixed path length (e.g., a fixed range or distance from the auxiliary interferometer). The auxiliary detector may detect interference patterns from the auxiliary interferometer. In implementations such as these, the interferometer 110 may generate the same interference patterns described above, and the auxiliary interferometer may generate interference patterns corresponding to the fixed path length. The signal analyzer 122 can include instructions for analyzing signals from both the detector 202 and auxiliary detector. The signal analyzer 122 can calculate distances according to equation (3):
where Ro is the fixed path length associated with the auxiliary interferometer, ƒref beat is the beat frequency from the auxiliary interferometer, and ƒbeat is the beat frequency from the main interferometer (described above). In implementations such as these, the LIDAR sensing system 100 may compensate for any nonlinearity of the light source 102, which may increase accuracy of the distance calculations.
In each of these implementations described above, distances may be calculated on a “rolling” basis as the wavelength of the light source 102 is swept across a range. Further, various arrangements and calculations described above may further increase accuracy of the distance calculations (e.g., through different mathematical calculations, additional interferometers, etc.).
In some embodiments, the LIDAR sensing system 100 may calculate distances at each interval as the wavelength (and therefore frequency) is changed. In these embodiments, the wavelength (and frequency) can be incrementally changed. For instance, the range of wavelengths can be subdivided into a number of increments. At each incremental wavelength, the distance can be calculated (e.g., according to any of the implementations described above, according to time shift or a time difference between receiving an indication of detection of the object beam and reference beam, etc.).
The computing system 112 may include a point cloud generator 124. The point cloud generator 124 may be or include instructions to generate a point cloud from various distance measurements. Point cloud, as used herein, refers to a two or three dimensional representation of an external environment 106 of the LIDAR sensing system 100 based on measured distances to various surfaces detected in the external environment 106. The point cloud generator 124 may include instructions to store each calculated distance and, for instance, an associated coordinate in a coordinate system. Additionally, where the object beam is moved (e.g., mechanically or electromechanically), further distance measurements may be obtained and thereby producing a two-dimensional scan or three-dimensional scan of the external environment 106. At least some of these measurements may be used for forming the point cloud. In some implementations, such as those where at least some components of the LIDAR sensing system 100 are rotated a number of degrees about an axis (e.g., axis 138 of
Referring now to
The collimated beam may be projected from the light source 102 at a variable wavelength. For instance, the light source controller 118 may include instructions for changing the wavelength of the collimated beam from the light source 102. As stated above, in some examples, the range of wavelengths λ at which the collimated beam from the light source 102 may be swept may be between 1.25 μm and 1.35 μm. As the wavelength λ of the collimated beam projected from the light source 102 is swept, the diffraction angle β changes. The diffraction angle β changes according to equation (4) below:
λ=d(sin α0−sin β) (4)
where the groove frequency d of grating in the diffraction grating 104 is 1200/mm (as one non-limiting example). According to equation (4), as the wavelength A increases, the diffraction angle β increases. Continuing the previous example, where the wavelength λ is swept from 1.25 μm and 1.35 μm, the diffraction angle β changes from 61.3 degrees to 85.9 degrees, or a 24.6 degree field of view along the vertical axis.
In some implementations, the collimated beam projected from the light source 102 may have a linewidth of 1 MHz. In implementations such as these, the coherence length may be 300 m (or a single path range of 150 m). Additionally, the collimated beam projected from the light source 102 may have a tuning range of 1.6 GHz. In these implementations, the resolution may be 9 cm. In each of these implementations, the LIDAR sensing system 100 may satisfy, at least, current standard requirements for LIDAR in many autonomous driving applications (e.g., ranging of 100 m and a resolution of less than 10 cm).
Referring now to
In some embodiments, the rotational element 502 may rotate the mirror 504 a number of degrees along the vertical axis. In so doing, the object beam diffracted from the diffraction grating 104 may be reflected off the mirror 504 at an angular range 508 corresponding to the rotation of the mirror 504. As a result, the field of view 510 of the LIDAR sensing system 100 may be defined by the degree of rotation of the mirror 504 and the change in wavelength of the collimated beam from the light source 102.
As the wavelength of the collimated beam is swept across the range, the LIDAR sensing system 100 may acquire data corresponding to various distances to objects in the external environment 106 (e.g., along the axis). In this regard, the LIDAR sensing system 100 may execute a scan (e.g., a two-dimensional scan) of the external environment 106 along an axis (e.g., the vertical axis of the external environment 106). As will be discussed in greater detail below, where various components of the LIDAR sensing system 100 are rotated, the LIDAR sensing system 100 may generate additional vertical scans. These additional vertical scans may be combined to generate a three-dimensional scan of the external environment 106 (e.g., via the point cloud generator 124). Such a three-dimensional scan may have several practical applications including, but not limited to, object detection and tracking, advanced driving assistance systems, autonomous driving, etc. Additionally, such a three-dimensional scan may be used in other fields outside of vehicle applications including, for instance, generation of three-dimensional maps.
Referring now to
As shown in
The motor 128 may be configured to rotate about an axis 136 as shown. When the motor 128 rotates about the axis 136, the motor 128 may rotate the rotational driver 130 about another axis. In the example shown, the motor 128 causes the rotational driver 130 to rotate about the same axis 136. However, the motor 128 may cause the rotational driver 130 to rotate along an axis that is different from axis 136. Accordingly, the present disclosure is not limited to the particular arrangement shown in
When the rotational driver 130 rotates about an axis (for instance, axis 136), the rotational driver 130 may cause the rotary stage 132 to rotate about another axis 138. In some implementations, the rotational driver 130 may cause the rotary stage 132 to rotate a full 360° about the axis 138. In other implementations, the rotation driver 130 may cause the rotary stage 132 to rotate less than (or greater than) the full 360° about the axis 138. As the rotary stage 132 rotates about axis 138, LIDAR sensing system 100 may generate additional scans along the vertical axis (e.g., through controlling the light source 102). Each of these scans may generate distance data associated with various objects located along the vertical axis. The point cloud generator 124 may include instructions to generate a three-dimensional point cloud based on each of these vertical scans.
As shown in
Where the rotational system 126 includes the rotational element 502 and mirror 504, the rotational element 502 may be arranged to rotate the mirror 504 about axis 602 (e.g., an axis 602 parallel to the vertical axis). The mirror 504 may be rotated about the axis 602, and subsequent vertical scans may be generated of the external environment 106 (e.g., shown by box 604). Each of these vertical scans may be used to generate a point cloud, as described above.
Now that various aspects of the disclosed systems and components have been described, a method of LIDAR scanning will be described with reference to
Referring now to
At operation 702, the method 700 may begin. For example, the method 700 may begin when an initialization signal (e.g., from a user) is received by the various components/systems described herein. As another example, the method 700 may begin when a vehicle is started (e.g., when the LIDAR sensing system 100 is a component of the vehicle). The method 700 may proceed to operation 704.
At operation 704, the method 700 may include controlling the light source 102 to project the collimated beam at a first wavelength at a first time. The collimated beam may be split by interferometer 110 into the object beam and reference beam. The object beam may be projected onto the diffraction grating 104. In some implementations, the processor 114 may control the light source 102 in accordance with the instructions from the light source controller 118. The object beam may be diffracted from the diffraction grating 104 at a first diffraction angle β. The object beam may be diffracted from the diffraction grating 104 at the first diffraction angle β in accordance with the wavelength of the collimated beam. The method 700 may proceed to operation 706.
In some implementations, while the light source 102 projects the collimated beam at the first wavelength, the method 700 may further include generating one or more control signals FOV expansion system 500 to control the rotational element 502 to rotate the mirror 504 in a first direction. In implementations such as these, the collimated beam may be reflected off the mirror 504 into the external environment 106 at a first angular range 508 corresponding to a degree of rotation of the mirror 504. In implementations where the mirror 504 is rotated in the first direction, the field of view for the LIDAR sensing system 100 may be defined by the first and second diffraction angle and the first angular range 508.
At operation 706, the method 700 may include receiving a signal corresponding to a first interference pattern from the detector 202. The interferometer 110 may generate the first interference pattern based on light reflected off objects in the external environment 106 and the reference mirror 206. The detector 202 may detect the interference pattern, and may generate a signal corresponding to the interference pattern. The first interference pattern may be associated with the collimated beam projected at operation 704. The method 700 may proceed to operation 708.
At operation 708, the method 700 may include calculating a first distance associated with the first interference pattern from operation 706. The signal analyzer 122 can include instructions for calculating the first distance (e.g., via any of equations 1-3). The signal analyzer 122 can include instructions for analyzing the signal from function block 706 to determine various signal characteristics (e.g., frequency, temporal, or other characteristics). The signal analyzer 122 can include instructions for calculating the first distance based on various characteristics of the analyzed signal. The method 700 may proceed to operation 710.
At operation 710, the method 700 may include controlling the light source 102 to project the collimated beam at a second wavelength at a second time. Operation 710 may be similar to operation 704. However, the second wavelength may be different from the first wavelength. Accordingly, the object beam may be diffracted from the diffraction grating 104 at a second diffraction angle β different from the first diffraction angle β. The object beam may be diffracted from the diffraction grating 104 at the second diffraction angle β in accordance with the wavelength of the collimated beam.
The method 700 may include calculating additional distances in substantially the same manner as described above with reference to operation 708. In this regard, the method 700 may include calculating distances associated with various objects located along the axis in the external environment 106. The distances may be calculated based on interference patterns generated by the interferometer 110 and detected by the detector 202. The distances may be calculated on a “rolling” basis. For instance, as the light source 102 is controlled to sweep the collimated beam across a range of wavelengths, the method 700 may include calculating distances as the collimated beam is swept across the range of wavelengths.
In some implementations, while the light source 102 projects the collimated beam at the second wavelength, the method 700 may further include generating one or more control signals for the FOV expansion system 500 to control the rotational element 502 to rotate the mirror 504 in a second direction. In implementations such as these, the object beam may be reflected off the mirror 504 into the external environment 106 at a second angular range 508 corresponding to a degree of rotation of the mirror 504. In implementations where the mirror 504 is rotated in the second direction, the field of view for the LIDAR sensing system 100 may be defined by the first and second diffraction angle and the second angular range 508. Additionally, where the mirror 504 is rotated in both the first direction while the light source 102 projects the collimated beam at the first wavelength the second direction while the light source 102 projects the collimated beam at the second wavelength, the field of view for the LIDAR sensing system 100 may be defined by the first and second diffraction angle and the first and second angular range 508.
In some implementations, following execution of the operations 702 through 710 to generate a first scan along an axis (e.g., a vertical axis) at a first position, the method 700 may further include generating one or more control signals for the rotational system 126 to one or more components of the LIDAR sensing system 100 about another axis to a second position. In implementations such as these, the method 700 may further include generating a second scan (and additional scans) of adjacent portions of the external environment 106 (e.g., through executing operations 702 through 710 when the rotary stage 132 is located at the second position).
In some implementations, the method 700 may include generating a point cloud map based on distances (including the first distance calculated at operation 708). The point cloud map may be a 360° point cloud map. For instance, the point cloud map may be a 360° point cloud map when the rotary stage is rotated 360° about the second axis.
The foregoing description of illustrative embodiments has been presented for purposes of illustration and of description. It is not intended to be exhaustive or limiting with respect to the precise form disclosed, and modifications and variations are possible in light of the above teachings or may be acquired from practice of the disclosed embodiments.
While certain embodiments have been illustrated and described, it should be understood that changes and modifications may be made therein in accordance with ordinary skill in the art without departing from the technology in its broader aspects as defined in the following claims.
The embodiments, illustratively described herein may suitably be practiced in the absence of any element or elements, limitation or limitations, not specifically disclosed herein. Thus, for example, the terms “comprising,” “including,” “containing,” etc. shall be read expansively and without limitation. Additionally, the terms and expressions employed herein have been used as terms of description and not of limitation, and there is no intention in the use of such terms and expressions of excluding any equivalents of the features shown and described or portions thereof, but it is recognized that various modifications are possible within the scope of the claimed technology. Additionally, the phrase “consisting essentially of” will be understood to include those elements specifically recited and those additional elements that do not materially affect the basic and novel characteristics of the claimed technology. The phrase “consisting of” excludes any element not specified.
The present disclosure is not to be limited in terms of the particular embodiments described in this application. Many modifications and variations may be made without departing from its spirit and scope, as will be apparent to those skilled in the art. Functionally equivalent methods and compositions within the scope of the disclosure, in addition to those enumerated herein, will be apparent to those skilled in the art from the foregoing descriptions.
Such modifications and variations are intended to fall within the scope of the appended claims. The present disclosure is to be limited only by the terms of the appended claims, along with the full scope of equivalents to which such claims are entitled. It is to be understood that this disclosure is not limited to particular methods, reagents, compounds compositions or biological systems, which may of course vary.
It is also to be understood that the terminology used herein is for the purpose of describing particular embodiments only, and is not intended to be limiting.
As will be understood by one skilled in the art, for any and all purposes, particularly in terms of providing a written description, all ranges disclosed herein also encompass any and all possible subranges and combinations of subranges thereof. Any listed range may be easily recognized as sufficiently describing and enabling the same range being broken down into at least equal halves, thirds, quarters, fifths, tenths, etc. As a non-limiting example, each range discussed herein may be readily broken down into a lower third, middle third and upper third, etc. As will also be understood by one skilled in the art all language such as “up to,” “at least,” “greater than,” “less than,” and the like, include the number recited and refer to ranges which may be subsequently broken down into subranges as discussed above. Finally, as will be understood by one skilled in the art, a range includes each individual member.
All publications, patent applications, issued patents, and other documents referred to in this specification are herein incorporated by reference as if each individual publication, patent application, issued patent, or other document was specifically and individually indicated to be incorporated by reference in its entirety.
Definitions that are contained in text incorporated by reference are excluded to the extent that they contradict definitions in this disclosure.
Other embodiments are set forth in the following claims.
Number | Name | Date | Kind |
---|---|---|---|
4466699 | Droessler et al. | Aug 1984 | A |
5022745 | Zayhowski et al. | Jun 1991 | A |
5319668 | Luecke | Jun 1994 | A |
5372135 | Mendelson et al. | Dec 1994 | A |
5430574 | Tehrani | Jul 1995 | A |
5537162 | Hellmuth et al. | Jul 1996 | A |
5561523 | Blomberg et al. | Oct 1996 | A |
5979760 | Freyman et al. | Nov 1999 | A |
5982963 | Feng et al. | Nov 1999 | A |
6070093 | Oosta et al. | May 2000 | A |
6111645 | Tearney et al. | Aug 2000 | A |
6134003 | Tearney et al. | Oct 2000 | A |
6160826 | Swanson et al. | Dec 2000 | A |
6275718 | Lempert | Aug 2001 | B1 |
6282011 | Tearney et al. | Aug 2001 | B1 |
6373632 | Flanders | Apr 2002 | B1 |
6421164 | Tearney et al. | Jul 2002 | B2 |
6485413 | Boppart et al. | Nov 2002 | B1 |
6501551 | Tearney et al. | Dec 2002 | B1 |
6556853 | Cabib et al. | Apr 2003 | B1 |
6564087 | Pitris et al. | May 2003 | B1 |
6725073 | Motamedi et al. | Apr 2004 | B1 |
7099358 | Chong | Aug 2006 | B1 |
7231243 | Tearney et al. | Jun 2007 | B2 |
7323680 | Chong | Jan 2008 | B2 |
7324214 | De Groot et al. | Jan 2008 | B2 |
7352783 | Chong | Apr 2008 | B2 |
7382809 | Chong et al. | Jun 2008 | B2 |
7388891 | Uehara et al. | Jun 2008 | B2 |
7400410 | Baker et al. | Jul 2008 | B2 |
7414779 | Huber et al. | Aug 2008 | B2 |
7428057 | De Lega et al. | Sep 2008 | B2 |
7489713 | Chong et al. | Feb 2009 | B2 |
7701588 | Chong | Apr 2010 | B2 |
7725169 | Boppart et al. | May 2010 | B2 |
7835010 | Morosawa et al. | Nov 2010 | B2 |
7865231 | Tearney et al. | Jan 2011 | B2 |
7869057 | De Groot | Jan 2011 | B2 |
7884945 | Srinivasan et al. | Feb 2011 | B2 |
7961312 | Lipson et al. | Jun 2011 | B2 |
8036727 | Schurman et al. | Oct 2011 | B2 |
8115934 | Boppart et al. | Feb 2012 | B2 |
8315282 | Huber et al. | Nov 2012 | B2 |
8405834 | Srinivasan et al. | Mar 2013 | B2 |
8427649 | Hays | Apr 2013 | B2 |
8500279 | Everett et al. | Aug 2013 | B2 |
8625104 | Izatt et al. | Jan 2014 | B2 |
8690328 | Chong | Apr 2014 | B1 |
8690330 | Hacker et al. | Apr 2014 | B2 |
9163930 | Buckland et al. | Oct 2015 | B2 |
9295391 | Tearney et al. | Mar 2016 | B1 |
9335154 | Wax et al. | May 2016 | B2 |
9851433 | Sebastian | Dec 2017 | B2 |
20020163948 | Yoshida et al. | Nov 2002 | A1 |
20030089778 | Tsikos et al. | May 2003 | A1 |
20040036838 | Podoleanu et al. | Feb 2004 | A1 |
20050171438 | Chen et al. | Aug 2005 | A1 |
20050201432 | Uehara et al. | Sep 2005 | A1 |
20050213103 | Everett et al. | Sep 2005 | A1 |
20060105209 | Thyroff et al. | May 2006 | A1 |
20060109872 | Sanders | May 2006 | A1 |
20060215713 | Flanders et al. | Sep 2006 | A1 |
20070040033 | Rosenberg | Feb 2007 | A1 |
20070076217 | Baker et al. | Apr 2007 | A1 |
20070081166 | Brown et al. | Apr 2007 | A1 |
20070133647 | Daiber | Jun 2007 | A1 |
20070141418 | Ota et al. | Jun 2007 | A1 |
20070233396 | Tearney et al. | Oct 2007 | A1 |
20070263226 | Kurtz et al. | Nov 2007 | A1 |
20070291277 | Everett et al. | Dec 2007 | A1 |
20080097194 | Milner | Apr 2008 | A1 |
20080269575 | Iddan | Oct 2008 | A1 |
20090022181 | Atkins et al. | Jan 2009 | A1 |
20090079993 | Yatagai et al. | Mar 2009 | A1 |
20090103050 | Michaels et al. | Apr 2009 | A1 |
20090169928 | Nishimura et al. | Jul 2009 | A1 |
20090247853 | Debreczeny | Oct 2009 | A1 |
20090268020 | Buckland et al. | Oct 2009 | A1 |
20090290613 | Zheng et al. | Nov 2009 | A1 |
20100110171 | Satake | May 2010 | A1 |
20100157308 | Xie | Jun 2010 | A1 |
20100246612 | Shimizu | Sep 2010 | A1 |
20100253908 | Hammer et al. | Oct 2010 | A1 |
20100284021 | Hacker | Nov 2010 | A1 |
20110112385 | Aalders | May 2011 | A1 |
20110228218 | Hauger et al. | Sep 2011 | A1 |
20110235045 | Koerner | Sep 2011 | A1 |
20110255054 | Hacker et al. | Oct 2011 | A1 |
20110299034 | Walsh et al. | Dec 2011 | A1 |
20120013849 | Podoleanu et al. | Jan 2012 | A1 |
20120026466 | Zhou et al. | Feb 2012 | A1 |
20120133950 | Suehira et al. | May 2012 | A1 |
20120136259 | Milner et al. | May 2012 | A1 |
20120188555 | Izatt et al. | Jul 2012 | A1 |
20130265545 | Buckland et al. | Oct 2013 | A1 |
20140051952 | Reichgott et al. | Feb 2014 | A1 |
20140111774 | Komine | Apr 2014 | A1 |
20140228681 | Jia et al. | Aug 2014 | A1 |
20140268163 | Milner et al. | Sep 2014 | A1 |
20140293290 | Kulkarni | Oct 2014 | A1 |
20140336479 | Ando | Nov 2014 | A1 |
20150177380 | Satyan | Jun 2015 | A1 |
20150223681 | Kuranov et al. | Aug 2015 | A1 |
20150348287 | Yi et al. | Dec 2015 | A1 |
20160178346 | Kulkarni | Jun 2016 | A1 |
20160259038 | Retterath et al. | Sep 2016 | A1 |
20160356881 | Retterath et al. | Dec 2016 | A1 |
20170090031 | Bondy et al. | Mar 2017 | A1 |
20180088236 | Eichenholz et al. | Mar 2018 | A1 |
20180128594 | Lee et al. | May 2018 | A1 |
20190257927 | Yao | Aug 2019 | A1 |
20200292673 | Galloway et al. | Sep 2020 | A1 |
20200292674 | Angus et al. | Sep 2020 | A1 |
Number | Date | Country |
---|---|---|
10 2011 114 797 | Apr 2013 | DE |
2006-202543 | Aug 2006 | JP |
2008-188047 | Aug 2008 | JP |
2010-172538 | Aug 2010 | JP |
2010-540914 | Dec 2010 | JP |
WO-2012075126 | Jun 2012 | WO |
WO-2013168149 | Nov 2013 | WO |
WO-2015121756 | Aug 2015 | WO |
WO-2017176901 | Oct 2017 | WO |
WO-2019204301 | Oct 2019 | WO |
Entry |
---|
Aflatouni, et al., “Nanophotonic coherent imager,” Optics Express 5118, vol. 23, No. 4, Feb. 23, 2015, DOI:10.1364/OE.23.005117 (9 pages). |
Hulme, et al., “Fully integrated hybrid silicon free-space beam steering source with 32 channel phased array,” Proc. of SPIE vol. 8989 898907-1, 2014 (15 pages). |
Poulton, et al., “Coherent solid-state LIDAR with silicon photonic optical phased arrays,” vol. 42, No. 20, Oct. 15, 2017, Optics Letters 4091 (6 pages). |
Chong, et al. “Large Coherence Length Swept Source for Axial Length Measurement of the Eye,” Applied Optics, 2009, pp. D145-D150, vol. 48, Issue 10. |
Chopra et al., Topographical Thickness of the Skin in the Human Face, Aesthetic Surgery Journal, vol. 35(8), 2015, pp. 1007-1013. |
Chowdhury, et al., “Challenges & Countermeasures in Optical Noninvasive Blood Glucose Detection,” International Journal of Innovative Research in Science, Engineering and Technology, Jan. 2013, pp. 329-334, vol. 2, Issue 1. |
Dai, et al., “Optical coherence tomography for whole eye segment imaging,” Optics Express, Mar. 2012, pp. 6109-6115, vol. 20, Issue 6. |
Dhalla, et al., “Simultaneous swept source optical coherence tomography of the anterior segment and retina using coherence revival,” Optics Letters, 2012, pp. 1883-1885, vol. 37, No. 11. |
Fainman, et al., “Nanophotonics for Information Systems,” Information Optics and Photonics, Oct. 1, 2010, pp. 13-37, T. Fournel and B. Javidi eds., Springer New York. |
Final Office Action on U.S. Appl. No. 14/723,325 dated Jul. 26, 2018. |
Final Rejection Office Action on U.S. Appl. No. 14/641,200 dated Dec. 7, 2015 (13 pages). |
Final Rejection Office Action on U.S. Appl. No. 14/723,325 dated Apr. 24, 2017 (8 pages). |
International Preliminary Report on Patentability on International Application No. PCT/IB2015/000808 dated Aug. 4, 2016 (7 pages). |
International Preliminary Report on Patentability on International Application No. PCT/US2015/019299 dated Sep. 13, 2016 (8 pages). |
International Preliminary Report on Patentability on International Application No. PCT/US2015/032727 dated Dec. 8, 2016 (7 pages). |
International Preliminary Report on Patentability on International Application No. PCT/US2016/035012 dated Dec. 14, 2017 (11 pages). |
International Search Report and Written Opinion dated Aug. 26, 2015 for PCT/US15/32727 (8 pages). |
International Search Report and Written Opinion on International Application No. PCT/EP2009/009189 dated Apr. 6, 2010 (12 pages). |
International Search Report and Written Opinion on International Application No. PCT/IB2015/000808 dated Oct. 20, 2015 (12 pages). |
International Search Report and Written Opinion on International Application No. PCT/US2015/19299 dated Nov. 2, 2015(10 pages). |
International Search Report and Written Opinion on International application No. PCT/US2016/035012 dated Aug. 18, 2016 (13 pages). |
Jeong, et al., “Spectral-domain OCT with dual illumination and interlaced detection for simultaneous anterior segment and retina imaging,” Optics Express, Aug. 2012, pp. 19148-19159, vol. 20, Issue 17. |
Jia, et al., “Split-Spectrum Amplitude-Decorrelation Angiography with Optical Coherence Tomography,” Optics Express, Feb. 2012, pp. 4710-4725, vol. 20 No. 4. |
Lexer, et al., “Wavelength-tuning interferometry of intraocular distances,” Applied Optics, 1997, pp. 6548-6553, vol. 36, Issue 25. |
Mariampillai, et al., “Speckle Variance Detection of Microvasculature Using Swept-Source Optical Coherence Tomography,” Optics Letters, Jul. 2008, pp. 1530-1532, vol. 33 No. 13. |
Nankivil, et al., “Handheld, rapidly switchable, anterior/posterior segment swept source optical coherence tomography probe,” Biomedical Optics Express, Nov. 2015, pp. 4516-4528, vol. 6, Issue 11. |
Non-Final Office Action on U.S. Appl. No. 15/086,520 dated Aug. 6, 2018. |
Non-Final Office Action on U.S. Appl. No. 15/139,579 dated Jul. 17, 2018. |
Non-Final Office Action on U.S. Appl. No. 15/648,239 dated Jun. 6, 2018. |
Non-Final Office Action on U.S. Appl. No. 14/641,200 dated Aug. 19, 2015 (12 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 13/892,997 dated Sep. 12, 2013 (15 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 14/601,945 dated Mar. 2, 2016 (13 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 14/613,644 dated Jun. 8, 2016 (8 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 14/641,200 dated Mar. 14, 2016 (13 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 14/723,325 dated Nov. 18, 2016 (8 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 14/723,325 dated Dec. 7, 2017 (11 pages). |
Non-Final Rejection Office Action on U.S. Appl. No. 15/202,925 dated Jul. 27, 2017 (8 pages). |
Notice of Allowance on U.S. Appl. No. 13/892,997 dated Dec. 6, 2013 (9 pages). |
Notice of Allowance on U.S. Appl. No. 14/601,945 dated Sep. 13, 2016 (10 pages). |
Notice of Allowance on U.S. Appl. No. 14/613,644 dated Nov. 7, 2016 7 pages). |
Notice of Allowance on U.S. Appl. No. 14/613,644 dated Nov. 18, 2016 (4 pages). |
Notice of Allowance on U.S. Appl. No. 14/641,200 dated Jul. 12, 2016 (10 pages). |
Notice of Allowance on U.S. Appl. No. 15/202,925 dated Feb. 13, 2018 (9 pages). |
Ortiz, et al., “Corneal Topography From Spectral Optical Coherence Tomography (sOCT),” Biomedical Optics Express, Dec. 2011, pp. 3232-3247, vol. 2, No. 12. |
Poddar, et al., “Non-Invasive Glucose Monitoring Techniques: A Review and Current Trends,” Oct. 2008, pp. 1-47. |
Sarlet, et al., “Wavelength and Mode Stabilization of Widely Tunable SG-DBR and SSG-DBR Lasers,” IEEE Photonics Technology Letters, Nov. 1999, pp. 1351-1353, vol. 11, Issue 11. |
Segawa, et al., “Semiconductor Double-Ring-Resonator-Coupled Tunable Laser for Wavelength Routing,” IEEE Journal of Quantum Electronics, Jul. 2009, pp. 892-899, vol. 45, Issue 7. |
Tayebati, et al., “Microelectromechanical tunable filter with stable half symmetric cavity,” Electronics Letters, Oct. 1998, pp. 1967-1968, vol. 34, Issue 20. |
U.S. Notice of Allowance on U.S. Appl. No. 15/202,925 dated May 17, 2018. |
U.S. Office Action on U.S. Appl. No. 15/630,654 dated Apr. 4, 2018. |
Pierrottet, D. et al., “Linear FMCW Laser Radar for Precision Range and Vector Velocity Measurements,” MRS Proceedings, 1076-K04-06; doi:10.1557/PROC-1076-K04-06. |
White et al., “In Vivo Dynamic Human Retinal Blood Flow Imaging Using Ultra-High-Speed Spectral Domain Optical Doppler Tomography,” Opt. Express 11, 3490-3497 (2003). |
Zhao, Y. et al., “Doppler Standard Deviation Imaging for Clinical Monitoring of In Vivo Human Skin Blood Flow,” Opt. Lett. 25, 1358-1360 (2000). |
Final Office Action on U.S. Appl. No. 15/139,579 dated May 15, 2019. |
International Search Report and Written Opinion in PCT/US2019/027671 dated Jul. 1, 2019. |
Notice of Allowance on U.S. Appl. No. 15/086,520 dated Jul. 9, 2019. |
Notice of Allowance on U.S. Appl. No. 15/578,421 dated May 1, 2019. |
Notice of Allowance on U.S. Appl. No. 15/611,515 dated May 21, 2019. |
Notice of Allowance on U.S. Appl. No. 15/630,654 dated Apr. 22, 2019. |
U.S. Office Action on U.S. Appl. No. 14/723,325 dated Apr. 19, 2019. |
Zhou, et al., “Space-division multiplexing optical coherence tomography,” Opt. Exp., Aug. 12, 2013, vol. 21, No. 16, pp. 19219-19227. |
International Search Report and Written Opinion for International Application No. PCT/US2021/019341 dated May 3, 2021, 10 pages. |
Number | Date | Country | |
---|---|---|---|
20190317194 A1 | Oct 2019 | US |