The present disclosure is in the technical field of solid-state LIDAR.
Generally, LIDAR, which stands for Light Detection and Ranging, is a remote sensing method that uses a laser to measure ranges or distances to a target object. The method typically measures distance to a target by illuminating the target with the laser and measuring the reflected signals with a sensor. Differences in laser return time and frequency may be gathered to generate precise, three-dimensional representations regarding the shape and surface characteristics of the target.
Typically, LIDAR uses ultraviolet, visible, or near infrared light to image objects. It may target a wide range of materials, including metal or non-metal objects, rocks, rain, chemical compounds, aerosols, clouds, etc. Further, a laser beam may be capable of mapping physical features with very high resolutions.
The present disclosure provides new and innovative methods and systems for a wide-angle high resolution solid-state LIDAR system using grating lobes. An example method includes a laser driver providing a current to a laser, and the laser producing laser energy. A splitter receiving the laser energy, and dividing the laser energy. The divided laser energy is provided to an optical antenna, where the optical antenna is connected to an optical phase shifters. The optical phase shifter controls the phase of the beams to be emitted from the antennas. The optical antenna emits beams, and the emitted beams include a first lobe and a second lobe. A photoreceiver having an optical receiver receives reflected optical signals, where the reflected optical signals are reflections of the first lobe and second lobe. Then, the reflected optical signals are converted into electronic signals in parallel.
An example system includes a control circuit, and a LIDAR signal processor, the LIDAR signal processor is located within the control circuit. Further, the example system includes a transmitter and a receiver. The transmitter includes an optical phased array circuit, and an optical phased array driver. The optical phased array driver is in communication with the control circuit and controls the optical phased array circuit. The transmitter further includes a laser and a laser driver. The laser driver is in communication with the LIDAR signal processor and drives the laser. The receiver includes a photoreceiver and a receiver front end circuit. The receiver front end circuit is in communication with the LIDAR signal processor and is connected to the photoreceiver.
Additional features and advantages of the disclosed methods and system are described in, and will be apparent from, the following Detailed Description and the Figures.
Generally, conventional LIDAR systems employ mechanical moving parts to steer a laser beam. They are generally considered bulky, incredibly costly and unreliable for many applications. These mechanical moving parts typically are the largest and most expensive part of a laser-scanning system. Generally, Solid-state LIDAR systems can overcome these issues by eliminating moving and mechanical parts. For example, by using the same manufacturing technology as silicon microchips, LIDAR systems can be incredibly small and inexpensive, without sacrificing loss in performance.
An optical phased array (OPA) is typically used to realize low-cost solid-state LIDARs. Generally, a phased array is an array of unmoving antennas creating light beams which can be steered to point in different directions. The beams produced by the antennas include a main lobe and other ancillary side lobes. The main lobe is the lobe containing the maximum power, and exhibits the greatest field strength. Side lobes, or grating lobes, are ancillary lobes produced by the antennas.
Traditionally, the OPA in a solid-state LIDAR uses the main lobe to scan the field-of-view (FOV) and collect the depth information of a target. In such a case, the grating lobes usually limit the steerable range of the main lobe and thus the total FOV angle. The main lobe and grating lobes may be generated by constructive interference of optical radiation from the antennas. Therefore, generally the side lobes are covered up or cut out of view in order for the main lobe to have the widest FOV. Typically, reducing the pitch of phased array antennas (or distance between the phased array antennas) increases the steerable range. However, optical crosstalk may limit the minimum feasible pitch. Moreover, reducing the pitch widens the beam divergence of main lobe when the total number of antennas is fixed. Therefore, the actual resolution of the LIDAR is not improved. Further, not utilizing the grating lobes produced by an optical phased array wastes energy.
In an example, the present disclosure remedies the above noted deficiencies by utilizing a solid-state LIDAR system that incorporates an optical phased array and/or an optical receiver array having photodetectors, pixels, photodiodes, or integrated photonic circuits. The system may be constructed to utilize grating lobes produced by an OPA in addition to the main lobe for scanning and ranging. In an example of the present disclosure, output of the antennas is optimized so that the steering windows of the main lobes and grating lobes may be stitched together to from a wide field-of-view by having optical receivers in a receiver chip/circuit that will capture reflections from the main lobes and the grating lobes. Aspects of the present disclosure can efficiently improve the scanning angle and resolution for solid-state LIDAR.
In exemplary
The power splitter 11 divides optical power from the laser source 12. This division of power between antennas may be equal or unequal. From the system perspective, the use of photodetector array or optical receiver array in a reception module to receive reflected signals enables the use of more than one lobe for ranging and imaging. From the transmitter perspective, grating lobes can be directly generated and optimized by increasing the pitch between antennas.
A laser 12 is connected to the transmitter chip 20. Generally, a laser generates an intense beam of coherent monochromatic light, or other electromagnetic radiation, by stimulating the emission of photons from excited atoms or molecules. Laser 12 can be an external module connecting to the transmitter chip 20 with a fiber-to-chip coupler. Alternatively, the laser 12 can be a semiconductor device, such as a laser diode, that is directly mounted on the transmitter chip. A laser diode creates a laser beam at the diode's junction. The transmitter chip may optionally also include an on-chip waveguide. Generally, a waveguide structure may guide waves, such as optical waves, and may enable a signal to propagate with minimal loss of energy by restricting expansion to one or two dimensions. If a laser diode is used as the laser 12, the laser diode may be coupled to the on-chip waveguide.
The receiver chip 21, or photoreceiver 21, contains an array of optical receivers 24. These optical receivers 24 may include photodiodes, pixels, photodetectors, or integrated photonic circuits. The optical receivers 24 can be one-dimensional or two-dimensional. The number of optical receivers 24 may be equivalent to the number of lobes 17 and 19. Alternatively, the number of optical receivers 24 may not be the same as the number of lobes created by the OPA. Using a plurality of optical receivers 24, multiple reflection points in the field of view can be imaged. Therefore, unlike the conventional method of using only the main lobe for imaging, when the grating lobes and main lobes are reflected there is more than one optical receiver 24 able to receive the reflected signal. The received signals can be separated and processed in parallel. This way, a wider steering angle and higher resolution can be achieved by breaking the limitations imposed by the conventional OPAs using only the main lobe. In addition, laser power is utilized in a more efficient way by preserving grating lobes.
Within the control module 35 is a LIDAR digital signal processing (DSP) module 34, or a LIDAR signal processor, used to process information received from any reflected optical signals. The LIDAR DSP module 34 can function in a variety of ways depending on the type of ranging method employed. For example, the LIDAR DSP module 34 may be a time of flight (“TOF”) processing module. For example, a TOF processing module calculates the depth for each laser beams at each steering angle based on the received signals from a photodetector array. Alternatively, the LIDAR DSP module 34 may be capable of processing information from frequency modulated continuous waves (FMCW) or amplitude modulated continuous waves (AMCW).
The system 300 includes a transmitter portion and a receiver portion. The transmitter portion includes an OPA circuit, such as a transmitter chip/circuit 20, a laser 30, an OPA driver 31 and a laser driver 32. Transmitter chip 20 includes an optical phased array 25 that produces main lobe 17 and grating lobes 19. These lobes can be steered/adjusted within window 16. The steering angle of the laser beams are set by the optical phase shifters, which are driven by the OPA driver frontend 31. The digital control module 35 controls the OPA driver 31. The laser driver 32 is used to drive the laser 30 and generate a similar or identical optical signal for the laser beams simultaneously. The laser driver 32 may be connected directly to LIDAR DSP module 34. In an alternative example, laser driver 32 may not be connected directly to LIDAR DSP module 34, and may alternatively be connected to control module 35. The transmitter portion of the system 300 may include more or less functionality, modules, or features than provided herein.
The receiver portion includes the receiver chip 21 and the receiver frontend 33. The receiver chip 21 includes an array of optical receivers with photodiodes 24. The array in
The method 400 begins by a current being provided to a laser (block 402). For example, in
Next, the laser produces laser energy (block 404), the laser energy is received by a splitter (block 406), and the laser energy is divided by the splitter (block 408). For example, laser 30 in
Next, the divided laser energy is provided to an optical antenna (block 410). For example, the energy split at splitter 11 is provided to each optical antenna 14. In an alternative example, the energy split at splitter 11 is provided to only some of the optical antennas 14. For example, an optical antenna 14 may be broken, damaged, or not desired to emit a beam.
Next, the phase of the beams to be emitted by the antennas is controlled by an optical phase shifter (block 412). For example, in order to direct the beams in a particular direction, phase shifters 13 may change or modify the phase of beams to be emitted from optical antennas 14. Each antenna 14 may connected to an optical phase shifter 13. This phase shifter 13 may be used for controlling the phase of the beams before or while the beams are being emitted from the antennas 14. Changing the phase of the emitted pulses or waves allows for the control of the beam's direction. In an alternate example, each antenna 14 may not be connected to an optical phase shifter 13.
Next, laser beams are emitted from the antennas (block 414). For example, main lobe 17 and grating lobes 19 are formed through the constructive interference of the pulses or waves produced from the various antennas 14. These main lobes 17 and grating lobes 19 are transmitted towards a desired target object, and once they hit the target object, some of the wave bounces off the object and are reflected back to the system.
Next, reflected optical signals are received at the receiver chip (block 416). For example, the reflections of grating lobes 19 and main lobes 17 are received at receiver chip 21 by optical receivers 24. In an example, all reflected optical signals are received at the receiver chip. In an alternative example, not all reflected signals are received at the receiver chip as some signals may be deflected, blocked, etc. Further, although a number grating lobes may be produced, not all grating lobes may be used depending on the target being imaged. A small target may require fewer grating lobes being used than all grating lobes produced. Alternatively, a closer or farther target may also require fewer/greater grating lobes. There are a number of reasons why less than all grating lobes would be used or processed by the receiver chip. A chip as used herein refers to a circuit such as, for example, an electronic circuit, an integrated circuit, a microchip, a semiconductor fabricated device, etc.
Last, the received reflected optical signals are converted into electronic signals in parallel (block 418). For example, the received optical signals are converted into electrical signals by the plurality of optical receivers 24 and/or the receiver chip 21. The receiver front end circuit 33 then amplifies the converted electronic signals. Following the receiver front end 33, an Analog to Digital Converter may be used to convert analog electronic signals into digital electronic signal, and a DSP/microprocessors may used to process the digital signals. These electrical signals may be used to create 3D, 2D, or 1D graphical images, or these data points may be stored in a memory or storage device for later use. For example, a 1D line scheme or a point cloud may be created. A memory device refers to a volatile or non-volatile memory device, such as RAM, ROM, EEPROM, or any other device capable of storing data.
It should be understood that various changes and modifications to the examples described herein will be apparent to those skilled in the art. Such changes and modifications can be made without departing from the spirit and scope of the present subject matter and without diminishing its intended advantages. It is therefore intended that such changes and modifications be covered by the appended claims.
This application claims priority to and the benefit of U.S. Provisional Application Ser. No. 62/490,514, entitled, “Wide-Angle High-Resolution Solid-State LIDAR System Based on Optical Phased Array and Photodetector Array Using Multiple Grating Lobes”, filed Apr. 26, 2017; U.S. Provisional Application Ser. No. 62/490,501, entitled, “Two-Dimensional Scanning High-Resolution Solid-State LIDAR System Based on Optical Phased Array and Photodetector Array Using Multiple Grating Lobes”, filed Apr. 26, 2017; U.S. Provisional Application Ser. No. 62/500,812, entitled, “Line-Scan High-Resolution Solid-State Light Detection And Ranging (LIDAR) System Based on Optical Phased Array and Photodetector Array”, filed May 3, 2017; U.S. Provisional Application Ser. No. 62/511,287, entitled, “Solid-State Light Detection and Ranging (LIDAR) System with Real-Time Self-Calibration”, filed May 25, 2017; U.S. Provisional Application Ser. No. 62/511,285, entitled, “Microprocessor-Assisted Solid-State Light Detection and Ranging (LIDAR) Calibration”, filed May 25, 2017; U.S. Provisional Application Ser. No. 62/511,288, entitled, “Adaptive Zooming in Solid-State Light Detection and Ranging (LIDAR) System Using Optical Phased Array”, filed May 25, 2017; and U.S. Provisional Application Ser. No. 62/532,814, entitled, “Solid-State Light Detection and Ranging System Based on an Optical Phased Array with an Optical Power Distribution Network”, filed Jul. 14, 2017, the entire contents of each of which are incorporated herein by reference and relied upon.
Number | Date | Country | |
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62490514 | Apr 2017 | US | |
62490501 | Apr 2017 | US | |
62500812 | May 2017 | US | |
62511287 | May 2017 | US | |
62511285 | May 2017 | US | |
62511288 | May 2017 | US | |
62532814 | Jul 2017 | US |