Coherent optical sensor with sparse illumination

Patent metadata

Field	Value
Publication number	US-12154194-B2
Application number	US-202016925680-A
Country	US
Kind code	B2
Filing date	Jul 10, 2020
Priority date	Jul 10, 2020
Publication date	Nov 26, 2024
Grant date	Nov 26, 2024

Abstract

A method for a target image reconstruction is provided. The method includes emitting stepped frequency waveforms having different constant frequencies at different periods of time, modulating the stepped frequency waveforms into frequency ranges each having a first frequency and a second frequency, wherein each of the stepped frequency waveforms are increased from the first frequency to the second frequency based on a range function, wherein the modulated stepped frequency waveforms are arranged with some sparsity factor. The method further includes transmitting the modulated stepped frequency waveforms to a target and accepting reflection of the modulated stepped frequency waveforms reflected from the target interfering the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms to produce beat signals of interferences between the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms, and reconstructing an image of the target from the beat signals.

First claim

We claim:

1. A method for a target image reconstruction, comprising:
emitting stepped frequency waveforms having different constant frequencies at different periods of time;
modulating the stepped frequency waveforms into frequency ranges each having a first frequency and a second frequency, wherein each of the stepped frequency waveforms is increased from the first frequency to the second frequency based on a range function, wherein the modulated stepped frequency waveforms have a sparsity factor, wherein the sparsity factor is defined as a number of wavelengths multiplied by a bandwidth per wavelength, divided by a total measurement bandwidth, wherein the sparsity factor is determined so as to be less than 1;
transmitting the modulated stepped frequency waveforms continuously to a target and accepting reflection of the modulated stepped frequency waveforms reflected from the target;
interfering the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms to produce beat signals of interferences between the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms; and
reconstructing an image of the target from the beat signals.

2. The method of claim 1 , wherein the reconstructing comprises:
using a low-bandwidth measurement from each step frequency of the unmodulated waveform to produce a set of low-bandwidth measurements;
increasing the sampling rate of each of the set of low-bandwidth measurements by zero padding in the frequency domain to produce a set of oversampled measurements;
applying frequency shifts to each of the low-bandwidth measurements corresponding to their relative optical frequencies, to produce a set of frequency shifted measurements;
summing the frequency shifted measurements to produce a single high-bandwidth measurement; and
transforming the high-bandwidth measurement with a Fourier transform to produce a target image, wherein a resolution of the target image is greater than resolution of each of the low-resolution images.

3. The method of claim 1 , further comprising:
generating a reference signal indicative of interference of the unmodulated step frequency waveform and the modulated step frequency waveform; and

reconstructing the target image using the beat signal and the reference signal.

4. The method of claim 3 , wherein the reconstructing comprises:
cross-correlating the beat signal and the reference signal in a frequency domain for each constant frequency of the unmodulated step frequency waveform to produce correlation signals, such that there is one correlation signal for each constant frequency;
combining the correlation signals in the frequency domain in an order of their respective frequencies to produce a frequency image of the target in the frequency domain; and
transforming the frequency image using a Fourier transform to produce the target image.

5. The method of claim 1 , wherein the interfering is performed in a digital domain.

6. The method of claim 1 , wherein the range function is a linear function as a function of time.

7. A system for a target image reconstruction, comprising:
a stepped frequency transmitter configured to emit stepped frequency waveforms having different constant frequencies at different periods of time;
a modulator configured to modulate the stepped frequency waveforms-into frequency ranges, each of the stepped frequency waveforms-having a first frequency and a second frequency, wherein each of the stepped frequency waveforms¬is increased from the first frequency to the second frequency based on a range function, wherein the arrangement of the modulated stepped frequency waveforms has a sparsity factor, wherein the sparsity factor is defined as a number of wavelengths multiplied by a bandwidth per wavelength, divided by a total measurement bandwidth, wherein the sparsity factor is determined so as to be less than 1;
a lens or antenna configured to transmit the modulated stepped frequency waveforms continuously to a target and accepting reflection of the modulated stepped frequency waveforms reflected from the target;
a mixer configured to interfere the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms to produce beat signals of interferences between the modulated stepped frequency waveforms and the reflection of the modulated stepped frequency waveforms; and
a signal processor configured to reconstruct an image of the target from the beat signals.

8. The system of claim 7 , wherein the signal processor performs steps of:
using a low-bandwidth measurement from each step frequency of the unmodulated waveform to produce a set of low-bandwidth measurements;
increasing the sampling rate of each of the set of low-bandwidth measurements by zero padding in the frequency domain to produce a set of oversampled measurements;
applying frequency shifts to each of the low-bandwidth measurements corresponding to their relative optical frequencies, to produce a set of frequency shifted measurements;
summing the frequency shifted measurements to produce a single high-bandwidth measurement; and
transforming the high-bandwidth measurement with a Fourier transform to produce a target image, wherein a resolution of the target image is greater than resolution of each of the low-resolution images.

9. The system of claim 7 , wherein the signal processor further performs steps of:
generating a reference signal indicative of interference of the unmodulated step frequency waveform and the modulated step frequency waveform; and

reconstructing the target image using the beat signal and the reference signal.

10. The system of claim 9 , wherein the reconstructing comprises:
cross-correlating the beat signal and the reference signal in a frequency domain for each constant frequency of the unmodulated step frequency waveform to produce correlation signals, such that there is one correlation signal for each constant frequency;
combining the correlation signals in the frequency domain in an order of their respective frequencies to produce a frequency image of the target in the frequency domain; and
transforming the frequency image using a Fourier transform to produce the target image.

11. The system of claim 7 , wherein the interfering is performed in a digital domain.

12. The system of claim 7 , wherein the range function is a linear function as a function of time.

Assignees

• Mitsubishi Electric Res Laboratories Inc

Inventors

• Millar David
• Atalar Okan
• Kojima Keisuke
• Koike-Akino Toshiaki
• Wang Pu
• Parsons Kieran

Classifications

• G06T12/10 Primary

  Image preprocessing, e.g. calibration, positioning of sources or scatter correction · CPC title

• G06T2207/10081

  Computed x-ray tomography [CT] · CPC title

• G01B9/02091

  Tomographic interferometers, e.g. based on optical coherence · CPC title

• G01B9/0209

  Low-coherence interferometers · CPC title

• G01B9/02087

  Combining two or more images of the same region · CPC title