High-resolution frequency-modulated continuous-wave LiDAR with solid-state beam steering

Abstract

A focal plane array (FPA) system for a solid-state frequency-modulated continuous wave (FMCW) light detection and ranging (LiDAR) system is disclosed. The FPA system includes a switchable coherent pixel array (SCPA) and a lens system. The SCPA is located on a LiDAR chip and includes coherent pixels (CPs). Each CP is configured to emit coherent light. The lens system is positioned to direct the coherent light emitted from the SCPA into an environment as one or more light beams. Each of the one or more light beams is emitted at a specific angle, based in part on the location of the coherent pixel on the LiDAR chip that generated the coherent light forming the one or more light beams.

Description

[Technical field]

[0001] CROSS-REFERENCE TO RELATED APPLICATIONS This application claims priority under 35 U.S.C. §119(e) to U.S. Provisional Application No. 62 / 957,050, filed January 3, 2020, and U.S. Provisional Application No. 62 / 960,686, filed January 13, 2020, the entire disclosures of which are incorporated herein by reference.

[0002] The subject matter of this disclosure relates generally to Frequency Modulated Continous Wave (FMCW) Light Detecting and Range (LiDAR), and more specifically to Solid State FMCW LiDAR systems. [Background technology]

[0003] Conventional LiDAR systems use mechanical moving parts and bulk optical lens elements (i.e., refractive lens systems) to steer the laser beam and are too bulky, expensive and unreliable for many applications (e.g., automotive). Summary of the Invention

[0004] A solid-state Frequency Modulated Continuous Wave (FMCW) Light Detection and Ranging (LiDAR) system is configured to determine depth information of one or more objects in an environment. The solid-state FMCW LiDAR system includes a Focal Plane Array (FPA) system and one or more laser sources. The one or more laser sources (e.g., tunable laser arrays) provide light to the FPA system such that the FPA system generates one or more beams and scans the one or more beams (e.g., in two dimensions) across the environment. The FPA system includes a Switchable Coherent Pixel Array (SCPA) and a lens system. The SCPA is located on the LiDAR chip and includes coherent pixels (CPs). Each CP is configured to emit coherent light. The lens system is positioned to direct the coherent light emitted from the SCPA into the environment as one or more light beams. The one or more light beams are then each emitted at a particular angle, the particular angle being based in part on the position of the CP on the LiDAR chip that generated the coherent light forming the one or more light beams. [Brief description of the drawings]

[0005] Other advantages and features of the embodiments of the present disclosure will become more clearly apparent from the following detailed description and appended claims taken in conjunction with the accompanying drawing examples.

[0006] [Figure 1] 1 illustrates an implementation of a switchable coherent pixel array on an Integrated Photonic LiDAR Chip in accordance with one or more embodiments.

[0007] [Figure 2a] 1 illustrates four versions of a coherent pixel (CP) in accordance with one or more embodiments. [Figure 2b] 1 illustrates four versions of a coherent pixel (CP) in accordance with one or more embodiments. [Figure 2c] 1 illustrates four versions of a coherent pixel (CP) in accordance with one or more embodiments. [Figure 2d] 1 illustrates four versions of a coherent pixel (CP) in accordance with one or more embodiments.

[0008] [Diagram 3] 1 illustrates a light beam steering structure in a solid-state FMCW LiDAR system in accordance with one or more embodiments.

[0009] [Figure 4a] 1 illustrates an optical beam steering structure for a solid-state FMCW LiDAR system including a transmission grating in accordance with one or more embodiments.

[0010] [Figure 4b] 1 illustrates an optical beam steering structure for a solid-state FMCW LiDAR system including a reflective grating in accordance with one or more embodiments.

[0011] [Diagram 5] 4a and 4b show examples of scanning and acquisition patterns generated by the solid-state LiDAR system.

[0012] [Figure 6] 1 illustrates two synchronization methods between the CP and the laser source of a solid-state FMCW LiDAR system in accordance with one or more embodiments.

[0013] [Figure 7] 1 illustrates a solid-state LiDAR system including an FPA system according to one or more embodiments. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0014] LiDAR systems determine depth information (e.g., range, velocity, acceleration for one or more objects) for the system's field of view. The LiDAR system is a Frequency Modulated Continuous Wave (FMCW) LiDAR. FMCW LiDARs measure the distance and velocity of objects directly by directing a frequency modulated collimated light beam at a target. The signal, which is the light reflected from the object, is mixed with a Tapped Version of said beam, called the Local Oscillator (LO). The frequency of the resulting Radio Frequency (RF) beat signal, when corrected for Doppler shift, which requires an additional measurement, is proportional to the distance of the object from the LiDAR system. The two measurements, either made simultaneously or not, provide the range and velocity information of the target.

[0015] A solid state FMCW LiDAR system is described herein. The solid state LiDAR system includes a Focal Plane Array (FPA) system and a laser source. The laser source provides coherent light to the FPA system. The FPA system can be a reciprocal system. The FPA system can include a lens system, a LiDAR chip, and further a diffraction grating. The LiDAR chip includes a solid state two-dimensional Switchable Coherent Pixels Array (SCPA) located at a focal distance from an optical lens. The SCPA includes a plurality of Coherent Pixels (CPs). The FPA system can selectively activate the CPs to emit light (received from the laser source). Each CP includes an optical antenna and a coherent optical receiver. The optical lens maps the direction of the incoming beam to a Focused Spot location in the Focal Plane and maps the light emitted from the CP to different angles in the environment (e.g., the surrounding area in a solid-state FMCW LiDAR system) depending on the location of the CP on the chip. The on-chip switch routes the light to the selected CP and steers the beam to an individual angular position through the optical lens. The vertical and horizontal angles of the outgoing light are determined by the location of the optical antenna on the chip with respect to the principal axis of the optical lens. Multi-channel individual beam steering is achieved by simultaneously switching multiple optical antennas with multiple switch networks.

[0016] In some embodiments, a diffraction grating (transmissive or reflective) is used to provide precision scanning capabilities. The diffraction grating is arranged to diffract one or more beams emitted from the lens system into the environment. The diffraction grating is a periodic structure that splits, refracts, or reflects light into multiple directions or diffraction orders. The angle of the emitted light depends on the period of the grating, the wavelength of the light beam, and the angle of incidence. One of ordinary skill in the art can design the diffraction grating and the angle of incidence so that the light is directed primarily in one direction (e.g., blazed grating), i.e., generally only in the first order. In some embodiments, the solid-state FMCW LiDAR system includes a laser source, which is a tunable light source such that the FPA system can output a light beam over a wavelength range. Thus, by varying the wavelength of the light source, the solid-state FMCW LiDAR system can steer the emitted light between two discrete steering positions set by the SCPA. This can provide a finer scanning resolution than that associated with selectively activating different CPs.

[0017] Conventional FMCW LiDAR systems using optical fibers and discrete optical components, such as optical interferometers, optical delay lines, and optical circulators, are bulky, expensive, and unreliable for use in many application fields such as automotive and robotics. In contrast, the aforementioned solid-state LiDAR system overcomes these issues by integrating the aforementioned optical components as well as optoelectronic components such as photodiodes and optical phase shifters on one semiconductor chip. In addition, solid-state LiDAR systems can further reduce cost and form factor and improve reliability by realizing beam steering function on the chip and eliminating mechanically moving parts in the system.

[0018] FIG. 1 illustrates an implementation of a Switchable Coherent Pixel Array (SCPA) on an optically integrated LiDAR chip 111 according to one or more embodiments. The LiDAR chip is a Photonic Integrated Circuit. The chip may include multiple basic functional subarrays 100. Each subarray 100 includes an optical input / output (I / O) port 102, a selective 1-K optical splitter 103, and one or more SCPAs 101, where K is an integer. The 1-K optical splitters 103 may be passive or active. Each optical I / O is supplied by a frequency modulated light source provided by an off-chip or on-chip laser (e.g., a laser source). To reduce the number of optical I / Os, optical power may be distributed on-chip via selective 1-K optical splitters. In the illustrated embodiment, each output of the 1-K optical splitters 103 is supplied to a corresponding SPCA 101. In the illustrated embodiment, each SCPA 101 includes M coherent pixels 105 and an optical switch network 104, where M is an integer. Note that in some cases, one or more of the optical switch networks 104, the optional 1-K optical splitters 103, or some combination thereof may simply be referred to as an optical switch. The optical switch is configured to switchably couple the input port 102 to an optical antenna in the coherent pixel, thereby forming an optical path between the input port and the optical antenna. The optical switch may include multiple active optical splitters. In some embodiments, the optical switch optically couples a frequency modulated laser signal to each of the optical antennas one at a time during a scanning period of the FMCW transceiver.

[0019] The optical switch network 104 selects one or more of the M coherent pixels to transmit and receive frequency modulated light (FM Light) for distance measurement and detection. The coherent pixels may be physically arranged on the chip in a one-dimensional array (e.g., a linear array) or a two-dimensional array (e.g., a rectangular or regular array (e.g., a non-random arrangement such as a grid)). In some embodiments, the selected coherent pixels may transmit light into free space, receive the returned optical signal, perform coherent detection, and directly convert the optical signal to an electrical signal for digital signal processing. It is noted that the received optical signal is not propagated again through the switch network so that it can be detected, but instead the output is routed separately (although not shown in the illustrated embodiment), which reduces losses and accordingly improves signal quality.

[0020] 2a-2d show four versions of a coherent pixel (CP) according to one or more embodiments. In FIG. 2a and FIG. 2b, light from an optical switch network is provided to an optical input port 203 of the CP. An optical splitter 212 splits the light into two output ports called TX signal 205 and local oscillator 214 (LO, Local Oscillator). The TX signal 215 is directly transmitted from the chip to the environment using a polarization-splitting optical antenna 210 with one polarization (e.g., TM). The polarization-splitting optical antenna 210 collects the beam reflected from the object to be measured and couples the orthogonal polarization (e.g., TE) into a waveguide 213, which transmits it directly to the optical mixer 201. In this case, the optical signal received by the polarization-splitting optical antenna 210 is not further split by an additional splitter or "pseudo circulator". The signals received from port 213 and LO 214 are mixed for coherent detection by the optical mixer 201, which can be a balanced 2×2 optical combiner 201 as in FIG. 2a or an optical hybrid 209 as in FIG. 2b. Finally, a pair of photodiodes 207 (PD) in FIG. 2a and four PDs in FIG. 2b convert the optical signals to electrical signals for beat-tone detection. This design implements a highly efficient integrated circulator for every single coherent pixel, enabling an ultra-sensitive on-chip monostatic FMCW LiDAR. As shown in Figures 2c and 2d, the TX signal 215 and the LO 214 can be fed to the CP separately to provide additional flexibility, for example, the TX signal or the local oscillator can be routed to the CP through two individual switch networks.

[0021] FIG. 3 illustrates an optical beam steering structure in a solid-state FMCW LiDAR system according to one or more embodiments. The solid-state FMCW LiDAR system includes a LiDAR chip 111 and a lens system 300. In the illustrated embodiment, the CP 105 of the SCPA on the LiDAR chip 111 is located at the focal length of the lens system 300. The lens system 300 includes one or more optical elements (e.g., positive lenses, freeform lenses, Fresnel lenses, etc.) that map the physical location of each CP 105 to a unique direction. The lens system 300 is configured to project a transmission signal emitted from each antenna of the multiple antennas to a corresponding portion of a field of view (e.g., an area of ​​the environment) and provide a reflection of the transmission signal to the antenna. Each optical antenna transmits and receives light at a different angle from each other. Thus, through the conversion to the different antennas, discrete optical beam scanning is achieved. The horizontal angle θ of the laser beam 301 h and the vertical angle θ v is set by the position of the CP including the optical antenna relative to the Principal Axis of the lens system 300. The SCPA may have the same or different step sizes when scanning in different directions. For example, SCPA-Enabled Discrete Beam Scanning, limited by the total number of CPs on the LiDAR chip 111, may have a fine angular step size in one dimension and a coarse angular step size in the other dimension.

[0022] FIG. 4a illustrates an optical beam steering structure for a solid-state FMCW LiDAR system including a transmission grating 400 according to one or more embodiments. The solid-state FMCW LiDAR system includes a LiDAR chip 111, a lens system 300, and a transmission grating 400. The LiDAR chip 111 and the lens system 300 operate as described with reference to FIG. 3 to generate beams 400, 401 that are emitted into the environment. The transmission grating 400 changes the direction of the beams 400, 401 emitted from the lens system 300. The diffraction angle is changed by adjusting the optical wavelength of the input light source relative to the LiDAR chip 111, thereby allowing continuous steering between coarse discrete steering positions (e.g., based on the position of the CP emission light) of the output from the lens system 300. For example, λ1, λ2, and λ3 represent three different optical wavelengths, and as shown, the transmission grating diffracts light of different wavelengths to different positions. Therefore, solid-state FMCW LiDAR systems emit light from different CPs to position the beam in a specific region of the environment (i.e., coarse optical steering) and adjust the wavelength of the emitted beam (e.g., λ) for finer optical steering of the beam. min From λ max The grating can be a 1D grating or a 2D grating. In some embodiments, the grating is a blazed grating designed to concentrate most of the power in a single order. In some embodiments, the grating is a custom 2D grating designed, for example, to suppress energy leaking into undesired higher orders and to compensate for the angular distortion of chromatic linear scanning that can occur with 1D gratings or some combination of these.

[0023] 4b illustrates an optical beam steering structure for a solid-state FMCW LiDAR system including a reflective grating 410 according to one or more embodiments. The solid-state FMCW LiDAR system of FIG. 4b operates in substantially the same manner as the solid-state FMCW LiDAR system of FIG. 4a.

[0024] 4a and 4b are positioned to diffract one or more beams emitted from lens system 300 into the environment, with the amount of diffraction based in part on the wavelength of the one or more beams. By tuning the wavelength of one or more beams over a range of wavelengths (i.e. based in part on the selective activation of different CPs of the SCPA), the solid-state FMCW LiDAR system can be altered to provide a second scanning resolution (i.e., the resolution of the grating) that is finer than the first scanning resolution.

[0025] FIG. 5 shows an example of a scanning and acquisition pattern generated by the solid-state LiDAR system of FIGS. 4a and 4b. min From λ max By chromatic scanning up to , each coherent pixel can generate a continuous section of a line (hereafter referred to as a scan line) in free space, and different coherent pixels (e.g., CP1, CP2) can be generated that are mapped to different scan lines projected onto the environment.

[0026] FMCW LiDAR receives a continuous signal for each scan line, which is typically much (e.g., 10-100 times) longer than the time window (e.g., several milliseconds) required to make a complete range and velocity measurement and generate individual LiDAR points. The range and velocity measurements of FMCW LiDAR are based on information extracted from a Fourier transform, primarily in the form of a Fast Fourier Transform (FFT). For each scan line, an FFT may be performed on successive and non-overlapping divisions of the continuous time-domain signal. For example, if the required time window is 10 μs and the scan line is 1 ms, typically 100 FFTs are performed, generating ~100 LiDAR points. The Sliding Discrete Fourier Transform (SDFT) can achieve much higher resolution compared to the typical Fast Fourier Transform (FFT) by interpolating the angular positions of successive scans within each pixel group. With the SDFT, the measurement interval (angle step size) can be set to a fraction of the required time window. For example, if the time window is 10 μs and the scan line is 1 ms, if the measurement interval is set to 5 μs, then ~200 LiDAR points can be generated through 200 SDFT runs. The number of LiDAR points is doubled compared to the case of non-overlapping FFT. The smaller the measurement interval, the more points per fixed scan line can be. The selective spatial overlap between the scan lines of two adjacent subframes ensures enough headroom for the SDFT window to slide. In this way, the solid-state FMCW LiDAR system can project one or more beams into the environment. The solid-state FMCW LiDAR system includes an SCPA that includes multiple CP groups. Each CP group corresponds to a different region of the environment. A portion of the one or more beams is reflected by an object in the environment and sensed by at least two groups of CPs. The solid-state FMCW LiDAR system can interpolate the angular position of the object from the detected portions of the one or more beams using SDFT.

[0027] The FMCW laser source generates a frequency chirp that is synchronized to the LiDAR pixels in the time domain: for each pixel, one upward ramp and one downward ramp of the FMCW LiDAR's frequency response can be used to simultaneously calculate velocity and distance based on the Doppler effect.

[0028] FIG. 6 illustrates two synchronization methods between the CP and the laser source of a solid-state FMCW LiDAR system according to one or more embodiments. The solid-state FMCW LiDAR system can be any of the embodiments described herein. FIG. 6 illustrates two methods (A and B) of chirping the laser source of a solid-state FMCW LiDAR system. The horizontal axis is time and the vertical axis is frequency. In method A, the light is chirped so that the frequency response is a triangular waveform with a period equal to the pixel time of the SDFT. The solid-state FMCW LiDAR system scans the beam into the environment and measures the frequency of the light reflected from objects in the environment during the scan. Each measurement takes a finite amount of time. Two measurements are used for single point measurements - one during a linear increase in the laser frequency (upward ramp) and one during a linear decrease in the laser frequency (downward ramp). The pixel time shows consecutive pairs of upward and downward ramps.

[0029] In method B, the laser source (or multiple sources) is chirped such that there are two complementary triangular chirp signals (denoted as chirp 1 and chirp 2). Such complementary chirp signals can be applied to the same light beam or to two separate beams. For example, in the case of two beams, the first laser source is chirped to have a chirp 1 frequency response and the second laser source is chirped to have a chirp 2 frequency response at the same time. Thus, the laser sources are simultaneously chirped in a complementary manner (i.e., having the same pattern but 180 degrees out of phase) to provide up-ramp and down-ramp measurements simultaneously over a single pixel time. In an embodiment using a single laser source, the solid-state FMCW LiDAR system chirps the laser source (e.g., chirp 1) and performs an up-ramp measurement on the object while scanning. The solid-state FMCW LiDAR system then chirps the beam in a complementary manner (e.g., chirp 2) and performs a down-ramp measurement (for the same location on the object). In this case, the period of both chirp signals does not need to be the same as the time window required to perform a single Fourier transform. This reduces the chirp bandwidth requirement for the FMCW source. Both methods also ensure that we always see the same duration for the frequency up and down ramps in each SDFT window. By using a CP that generates a complex signal (e.g., I / Q of an optical hybrid), FMCW measurements (velocity and distance calculations) can be made without ambiguity. Note that local frequency modulation may be added on top of a slowly varying wavelength sweep that can be used for chromatic scanning.

[0030] FIG. 7 illustrates a solid-state LiDAR system including an FPA system according to one or more embodiments. The FPA system can be a reciprocal system. The FPA system includes an optical grating 705, a lens system 300, and a LiDAR chip 111. The grating can be a transmissive grating or a reflective grating as described in FIG. 4a and FIG. 4b. The CPs in the LiDAR chip 111 are part of one or more SPCAs 101 controlled by an FPA driver 710. One or more individual CPs of the LiDAR chip 111 can be activated to emit and receive light. The light emitted by the LiDAR chip 111 is generated by a Q-channel laser array 715. The Q-channel laser array 715 is a laser array with Q parallel channels, where Q is an integer. The Q-channel laser array 715 can be directly integrated with the LiDAR chip 111 or can be a separate module packaged together with the LiDAR chip 111. The Q-channel laser array 715 is controlled by a laser controller 720. In some embodiments, the Q-channel laser array 715 can be tunable over a range of wavelengths.

[0031] The laser controller 720 receives control signals from the LiDAR processing engine 725 via a digital-to-analog converter 730. The processing also controls the FPA driver 710 to send and receive data from the LiDAR chip 111.

[0032] The LiDAR processing engine 725 includes a microcomputer 735. The microcomputer 735 processes data coming from the FPA system and sends control signals to the FPA system via the FPA driver 710 and the laser controller 720. The LiDAR processing engine 725 also includes an N-channel receiver 740. Signals are received by the N-channel receiver 740 and the signals are digitized using a set of M-channel analog-to-digital converters (ADCs) 745.

[0033] Additional configuration information It should be noted that the drawings and the foregoing description relate to preferred embodiments by way of example only, and as previously mentioned, alternative embodiments of the structures and methods disclosed herein are readily discernible as viable alternatives that may be employed without departing from the principles of the claims.

[0034] Although the detailed description includes many details, these should not be interpreted as limiting the scope of the present invention, but merely as illustrating different examples. It should be understood that the scope of the present disclosure includes other embodiments not described in detail above. Various other modifications, changes and changes that are obvious to those of ordinary skill in the art may be made in the arrangement, operation and details of the methods and apparatus disclosed herein without departing from the spirit and scope defined in the appended claims. Therefore, the scope of the present invention should be determined by the appended claims and their legal equivalents.

[0035] Alternative embodiments are implemented in computer hardware, firmware, software and / or combinations thereof. Implementations may be implemented as a computer program product substantially embodied in a machine-readable storage device for execution by a programmable processor, and method steps may be performed by the programmable processor executing an instruction program to perform functions by operating on input data and generating output. The embodiments may advantageously be implemented in one or more computer programs executable on a programmable system including at least one programmable processor coupled to receive data and instructions from, and transmit data and instructions from, a data storage system, at least one input device and at least one output device. Each computer program may be implemented in a high level procedural or object-oriented programming language, or assembly or machine language as appropriate, and in any case the language may be a compiled or interpreted language. Suitable processors include, by way of example, general-purpose and special-purpose microprocessors. Typically, the processor receives instructions and data from a read-only memory (ROM) and / or a random access memory (RAM). Typically, a computer will include one or more mass storage devices for storing data files; such devices include magnetic disks, such as internal hard disks and removable disks, magneto-optical disks, and optical disks. Suitable storage devices for substantially implementing computer program instructions and data include, by way of example, all forms of non-volatile memory, including semiconductor memory devices, such as EPROM, EEPROM, and flash memory devices, magnetic disks, such as internal hard disks and removable disks, magneto-optical disks, and CD-ROM disks. All of the foregoing may be supplemented by, or integrated with, Application-Specific Integrated Circuits (ASICs) and other forms of hardware.

Claims

1. As a focal plane array (FPA) system for solid-state frequency modulated continuous wave (FMCW) light detection and ranging (LiDAR) systems, a Switchable Coherent Pixel Array (SCPA) on a LiDAR chip, the SCPA including coherent pixels (CP), each of the coherent pixels configured to emit coherent light; and and a lens system positioned to direct coherent light emitted from the SCPA into an environment as one or more light beams, the one or more light beams each emitted at a specific angle, the wavelengths of the one or more light beams being tuned over a range of wavelengths, the specific angle being based in part on the wavelengths tuned over the range of wavelengths and the position of the CP on the LiDAR chip that generated the coherent light forming the one or more light beams.

2. said focal plane array system comprising:

10. The focal plane array system of claim 1 configured to scan the one or more light beams in two dimensions within the environment at a first scanning resolution based in part on selective activation of different CPs of the SCPA.

3. said focal plane array system comprising: a diffraction grating positioned to diffract the one or more light beams emitted from the lens system into the environment, the amount of diffraction being based in part on the wavelengths of the one or more light beams; 3. The focal plane array system of claim 2, wherein the amount of diffraction of said diffraction grating is altered to provide a second scanning resolution that is finer than said first scanning resolution.

4. 4. The focal plane array system of claim 3, wherein the diffraction grating is a blazed grating that primarily emits light of a first diffraction order.

5. 4. The focal plane array system of claim 3, wherein the diffraction grating is a reflective diffraction grating.

6. 4. The focal plane array system of claim 3, wherein said diffraction grating is a transmission type diffraction grating.

7. a first set of CPs in the SCPA, wherein coherent light emitted from each CP in the first set is mapped to a respective section of a first continuous line in the environment; 4. The focal plane array system of claim 3, wherein a second set of CPs in the SCPA are arranged such that coherent light emitted from each CP in the second set is mapped to a respective section of a second continuous line that is different from the first continuous line in the environment.

8. a portion of the one or more light beams being reflected by an object in the environment and detected by a group of at least two CPs of the SCPA; Each group of CPs corresponds to a different region of the environment; 2. The focal plane array system of claim 1, wherein a Sliding Discrete Fourier Transform (SDFT) is used to interpolate an angular position of the object from detected portions of the one or more light beams.

9. 9. The focal plane array system of claim 8, wherein the frequency response of the coherent light emitted by an FMCW source providing coherent light to the focal plane array system is a triangular waveform and has the same period as a pixel time for an SDFT.

10. a first FMCW source and a second FMCW source configured to provide coherent light to the focal plane array system; the first FMCW source is configured to emit coherent light having a first frequency response that is a triangular waveform at a first phase; the second FMCW source is configured to emit coherent light having a second frequency response that is a triangular waveform with a second phase; 9. The focal plane array system of claim 8, wherein said second phase differs from said first phase by 180 degrees.

11. As a solid-state frequency modulated continuous wave (FMCW) light detection and ranging (LiDAR) system, a laser source emitting coherent light; a Switchable Coherent Pixel Array (SCPA) on a LiDAR chip, the SCPA configured to selectively emit the coherent light via one or more Coherent Pixels (CPs) using the coherent light from at least the laser source; and and a lens system positioned to direct coherent light emitted from the SCPA into an environment as one or more light beams, the one or more light beams each emitted at a specific angle, the wavelengths of the one or more light beams being tuned over a range of wavelengths, the specific angle being based in part on the wavelengths tuned over the range of wavelengths and the position of the CP on the LiDAR chip that generated the coherent light forming the one or more light beams.

12. The LiDAR system includes:

12. The LiDAR system of claim 11, further comprising a controller configured to instruct the LiDAR chip to scan the one or more light beams in two dimensions within the environment at a first scanning resolution based in part on selective activation of different CPs of the SCPA.

13. The solid-state FMCW LiDAR system comprises: a diffraction grating positioned to diffract the one or more light beams emitted from the lens system into the environment, the amount of diffraction being based in part on the wavelengths of the one or more light beams; 13. The LiDAR system of claim 12, wherein the amount of diffraction of the diffraction grating is altered to provide a second scanning resolution that is finer than the first scanning resolution.

14. The LiDAR system of claim 13 , wherein the diffraction grating is a blazed grating that primarily emits light of a first diffraction order.

15. The LiDAR system of claim 13 , wherein the diffraction grating is a reflective diffraction grating.

16. The LiDAR system of claim 13 , wherein the diffraction grating is a transmission type diffraction grating.

17. a first set of CPs in the SCPA, wherein coherent light emitted from each CP in the first set is mapped to a respective section of a first continuous line in the environment; The LiDAR system of claim 13 , wherein a second set of CPs in the SCPA are arranged such that coherent light emitted from each CP in the second set is mapped to a respective section of a second continuous line that is different from the first continuous line in the environment.

18. a portion of the one or more light beams being reflected by an object in the environment and detected by a group of at least two CPs of the SCPA; Each group of CPs corresponds to a different region of the environment; 12. The LiDAR system of claim 11, wherein a Sliding Discrete Fourier Transform (SDFT) is used to interpolate an angular position of the object from detected portions of the one or more light beams.

19. 20. The LiDAR system of claim 18, wherein the frequency response of the coherent light is a triangular waveform and has the same period as a pixel time for the SDFT.

20. The coherent light emitted from the laser source has a frequency response that is a triangular waveform with a first phase, and the FMCW LiDAR system further comprises: a second laser source configured to emit coherent light having a second frequency response that is a triangular waveform at a second phase, the second phase differing from the first phase by 180 degrees; The LiDAR system of claim 18 , wherein the coherent light emitted from the SCPA includes all of the coherent light emitted from the laser source and the second laser source.

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