Techniques for mixing local oscillator signal with target return signal to generate target information
A light detection and ranging (LIDAR) apparatus includes an optical source to emit an optical beam, and free-space optics coupled with the optical source. The free space optics include a photodetector and other optical components to direct a propagated portion of the optical beam or a reflected portion of the optical beam toward the photodetector as a local oscillator signal, and to transmit the optical beam toward a target environment.
1. A light detection and ranging (LIDAR) apparatus, comprising:
an optical source to emit an optical beam comprising light of a first wavelength and a second wavelength; and
free-space optics coupled with the optical source, comprising:
a photodetector (PD); and
a polarizing beam-splitter (PBS) to transmit the optical beam in a first direction toward a target environment and to propagate a portion of the optical beam in a second direction toward the PD, wherein the propagated portion of the optical beam comprises a local oscillator (LO) signal to mix with a target return signal to generate target information, wherein both the target return signal and the LO signal comprise light of the first wavelength and the second wavelength.
2. The LIDAR apparatus of claim 1 , wherein the optical beam and the propagated portion of the optical beam have a first linear polarization, wherein the free-space optics further comprise a first polarization wave plate (PWP) to convert the transmitted optical beam from the first linear polarization to a first circular polarization, and to convert the target return signal from a second circular polarization to a second linear polarization, wherein the target return signal is reflected from the PBS in a third direction.
3. The LIDAR apparatus of claim 2 , wherein the free-space optics further comprise:
a second PWP to convert the target return signal from the second linear polarization to the first circular polarization; and
a reflector to convert the target return signal from the first circular polarization to the second circular polarization, and to reflect the target return signal through the second PWP, wherein the target return signal is converted from the second circular polarization to the first linear polarization.
4. The LIDAR apparatus of claim 3 , wherein the free-space optics further comprise a polarization filter coupled between the PBS and the PD, wherein the first linear polarization is selected.
5. The LIDAR apparatus of claim 4 , further comprising a second PD, wherein the LO signal and the target return signal of the first wavelength are directed toward the PD and the LO signal and the target return signal of the second wavelength are directed toward the second PD.
6. The LIDAR apparatus of claim 5 , wherein the free-space optics further comprise a first lens system coupled between the optical source and the PBS to collimate the optical beam.
7. The LIDAR apparatus of claim 5 , wherein the free-space optics further comprise a second lens system coupled between the PBS and the first PWP to magnify the optical beam.
8. The LIDAR apparatus of claim 2 , further comprising an optical scanner, coupled with the first PWP to illuminate the target environment, wherein a detection aperture of the PD is larger than a diameter of the target return signal plus a de-scan error contributed by the optical scanner.
9. The LIDAR apparatus of claim 1 , wherein the optical source is configured to emit the optical beam as a first optical beam having the first wavelength and a second optical beam having the second wavelength.
10. A light detection and ranging (LIDAR) apparatus, comprising:
an optical source to emit an optical beam comprising light of a first wavelength and a second wavelength; and
free-space optics coupled with the optical source, comprising:
a photodetector (PD); and
a polarizing beam-splitter (PBS) to transmit the optical beam in a first direction toward a target environment; and
a polarization wave plate (PWP) to transmit the optical beam toward the target environment and to reflect a portion of the optical beam to the PBS, wherein the reflected portion of the optical beam is directed in a second direction toward the PD, wherein the reflected portion of the optical beam comprises a local oscillator (LO) signal to mix with a target return signal to generate target information, and wherein both the target return signal and the LO signal comprise light of the first wavelength and the second wavelength.
11. The LIDAR apparatus of claim 10 , wherein the optical beam has a first linear polarization and the reflected portion of the optical beam has a second linear polarization, the PWP to convert the optical beam from the first linear polarization to a first circular polarization, to convert the target return signal from a second circular polarization to the second linear polarization, the PBS to direct the target return signal in the second direction toward the PD.
12. The LIDAR apparatus of claim 11 , wherein the free-space optics further comprise a polarization filter coupled between the PBS and the PD, wherein the second linear polarization is selected.
13. The LIDAR apparatus of claim 12 , wherein the free-space optics further comprise a wavelength demultiplexer coupled between the polarization filter, the PD, and a second PD.
14. The LIDAR apparatus of claim 13 , wherein the free-space optics further comprise a first lens system coupled between the optical source and the PBS to collimate the optical beam.
15. The LIDAR apparatus of claim 13 , wherein the free-space optics further comprise a second lens system coupled between the PBS and the PWP to magnify the optical beam.
16. The LIDAR apparatus of claim 10 , further comprising an optical scanner, coupled with the PWP to illuminate the target environment, wherein a detection aperture of the PD is larger than a diameter of the target return signal plus a de-scan error contributed by the optical scanner.
17. The LIDAR apparatus of claim 10 , wherein the optical source is configured to emit at least a second optical beam.
18. A method for light detection and ranging (LIDAR) with free-space optics, comprising:
generating an optical beam from an optical source having a first linear polarization, the optical beam comprising light of a first wavelength and a second wavelength;
directing the optical beam in a first direction, toward a target environment, with a polarizing beam splitter (PBS);
propagating a portion of the optical beam with the first linear polarization, from the PBS in a second direction, toward a photodetector (PD), as a local oscillator (LO) signal, wherein the LO signal comprises light of the first wavelength and the second wavelength;
receiving, at the PD, a portion of the LO signal having the first wavelength and a portion of a target return signal having the first wavelength and the first linear polarization; and
mixing the portion of the target return signal having the first wavelength with the portion of the LO signal having the first wavelength to generate target information.
19. The method of claim 18 , further comprising:
removing optical noise at the PD with a polarization filter at the PD;
maximizing a signal-to-noise ratio of the target return signal with a PD aperture approximately equal to an optical aperture of the free-space optics; and
minimizing a de-scan error with the PD aperture.
20. The method of claim 18 , further comprising:
converting the optical beam from the first linear polarization to a first circular polarization with a polarization wave plate (PWP);
converting the target return signal from a second circular polarization to a second linear polarization with the PWP;
reflecting the target return signal from the PBS in a third direction;
converting the target return signal from the second linear polarization to the first circular polarization with a second PWP; and
reflecting the target return signal, with a reflector, through the PBS, wherein the target return signal is converted from the first circular polarization to the first linear polarization.
21. A method for light detection and ranging (LIDAR) with free-space optics comprising:
generating an optical beam from an optical source having a first linear polarization, the optical beam comprising light of a first wavelength and a second wavelength;
directing the optical beam in a first direction, toward a target environment, with a polarizing beam splitter (PBS);
reflecting a portion of the optical beam from a polarization wave plate (PWP) as a local oscillator (LO) signal having a second linear polarization, toward the PBS;
receiving, at a photodetector (PD), the LO signal and a target return signal having the second linear polarization; and
mixing the target return signal with the LO signal to generate target information, wherein both the target return signal and the LO signal comprise light of the first wavelength and the second wavelength.
22. The method of claim 21 further comprising:
removing optical noise at the PD with a polarization filter at the PD;
maximizing a signal-to-noise ratio of the target return signal with a PD aperture approximately equal to an optical aperture of the free-space optics; and
minimizing a de-scan error with the PD aperture.
23. The method of claim 22 , further comprising:
converting the optical beam from the first linear polarization to a first circular polarization with the PWP;
converting the target return signal from a second circular polarization to the second linear polarization with the PWP; and
reflecting the target return signal and the LO signal from the PBS in a second direction toward the PD.