Multi-tone continuous wave detection and ranging
US-2021382164-A1 · Dec 9, 2021 · US
US11630189B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-11630189-B2 |
| Application number | US-201916666582-A |
| Country | US |
| Kind code | B2 |
| Filing date | Oct 29, 2019 |
| Priority date | Nov 9, 2018 |
| Publication date | Apr 18, 2023 |
| Grant date | Apr 18, 2023 |
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Various examples for multi-tone continuous wave detection and ranging are disclosed herein. In some embodiments, an initial signal is generated using initial radio frequency (RF) tones, and is emitted as a multi-tone continuous wave signal. The initial signal is reflected from a target and received as a reflected signal. Resultant RF tones, including a frequency and a power, are determined from the reflected signal in a frequency domain. A frequency-domain sinusoidal wave is fitted to the resultant RF tones in the frequency domain, and a distance to the target is determined using a modulation of the frequency-domain sinusoidal wave.
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Therefore, the following is claimed: 1. An apparatus, comprising: a signal emitter; a signal receiver; and at least one computing device comprising at least one processor and a data store comprising executable instructions, wherein the instructions, when executed by the at least one processor, cause the apparatus to at least: generate an initial signal based at least in part on a sum of a plurality of predetermined individual radio frequency (RF) tones, wherein the signal emitter emits the initial signal as a multi-tone continuous wave signal; identify a reflected signal, the reflected signal being a version of the initial signal reflected from a target, wherein the signal receiver receives the reflected signal; determine a plurality of resultant RF tones based at least in part on the reflected signal, a respective one of the plurality of resultant RF tones comprising a frequency and a power; fit a frequency-domain sinusoidal wave to the plurality of resultant RF tones in a frequency domain; and determine a distance to the target based at least in part on a modulation of the frequency-domain sinusoidal wave. 2. The apparatus of claim 1 , wherein the instructions, when executed by the at least one processor, further cause the apparatus to at least: determine a velocity of the target based at least in part on a frequency shift between the plurality of initial RF tones and the plurality of resultant RF tones. 3. The apparatus of claim 1 , wherein the signal emitter comprises: a laser source; a Mach-Zehnder modulator; a beam splitter; and wherein the Mach-Zehnder modulator outputs the initial signal as an amplitude modulated laser beam based at least in part on inputs to the Mach-Zehnder modulator comprising: a laser beam, and the plurality of initial RF tones. 4. The apparatus of claim 3 , wherein the beam splitter splits the amplitude modulated laser beam into an emitted component and a reference component, wherein the reference component is recombined with the reflected signal to generate an interference pattern from the plurality of resultant RF tones. 5. The apparatus of claim 4 , further comprising: a frequency shifter, wherein the frequency shifter shifts the reference component to compensate for a velocity of the apparatus. 6. The apparatus of claim 3 , wherein the laser source comprises a plurality of colored laser sources of respective colors, the initial signal is emitted as a plurality of initial laser beams corresponding to the respective colors, and the reflected signal is received as a plurality of resultant laser beams corresponding to the respective colors. 7. The apparatus of claim 6 , wherein the instructions, when executed by the at least one processor, further cause the apparatus to at least: determine a color of the target is based at least in part on a respective amplitude of each of the plurality of resultant laser beams corresponding to the respective colors. 8. The apparatus of claim 1 , further comprising: a summing amplifier that outputs the sum of the plurality of initial RF tones to generate the initial signal; and wherein the signal emitter comprises an antenna that emits the initial signal as electromagnetic waves. 9. The apparatus of claim 8 , wherein the signal emitter further comprises a power splitter that splits the initial signal into an emitted component and a reference component, wherein another summing amplifier sums the reference component with the reflected signal to generate an interference pattern from the plurality of resultant RF tones. 10. The apparatus of claim 9 , further comprising: a frequency shifter, wherein the frequency shifter shifts the reference component to compensate for a velocity of the apparatus. 11. A method, comprising: generating an initial signal based at least in part on a sum of a plurality of predetermined individual radio frequency (RF) tones, wherein a signal emitter emits the initial signal as a multi-tone continuous wave signal; identifying a reflected signal, the reflected signal being a version of the initial signal reflected from a target, wherein a signal receiver receives the reflected signal; determining a plurality of resultant RF tones based at least in part on the reflected signal, a respective one of the plurality of resultant RF tones comprising a frequency and a power; fitting a frequency-domain sinusoidal wave to the plurality of resultant RF tones in a frequency domain; and determining a distance to the target based at least in part on a modulation of the frequency-domain sinusoidal wave. 12. The method of claim 11 , further comprising: determining a velocity of the target based at least in part on a frequency shift between the plurality of initial RF tones and the plurality of resultant RF tones. 13. The method of claim 11 , wherein the signal emitter comprises: a laser source; a Mach-Zehnder modulator; a beam splitter; and wherein the Mach-Zehnder modulator outputs the initial signal as an amplitude modulated laser beam based at least in part on inputs to the Mach-Zehnder modulator comprising: a laser beam, and the plurality of initial RF tones. 14. The method of claim 13 , wherein the beam splitter splits the amplitude modulated laser beam into an emitted component and a reference component, wherein the reference component is recombined with the reflected signal to generate an interference pattern from the plurality of resultant RF tones. 15. The method of claim 14 , wherein a frequency shifter shifts the reference component for velocity compensation. 16. The method of claim 13 , wherein the laser source comprises a plurality of colored laser sources of respective colors, the initial signal is emitted as a plurality of initial laser beams corresponding to the respective colors, and the reflected signal is received as a plurality of resultant laser beams corresponding to the respective colors. 17. The method of claim 16 , further comprising: determining a color of the target is based at least in part on a respective amplitude of each of the plurality of resultant laser beams corresponding to the respective colors. 18. The method of claim 11 , further comprising: outputting, from a summing circuit, the sum of the plurality of initial RF tones to generate the initial signal, wherein the signal emitter comprises an antenna that emits the multi-tone continuous wave signal as electromagnetic waves. 19. The method of claim 18 , wherein the signal emitter further comprises a power splitter that splits the initial signal into an emitted component and a reference component, wherein another summing amplifier sums the reference component with the reflected signal to generate an interference pattern from the plurality of resultant RF tones. 20. The method of claim 19 , wherein a frequency shifter shifts the reference component for velocity compensation.
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