Simultaneous forward and inverse synthetic aperture imaging LADAR

Patent metadata

Field	Value
Publication number	US-9354317-B2
Application number	US-201414274026-A
Country	US
Kind code	B2
Filing date	May 9, 2014
Priority date	Apr 9, 2014
Publication date	May 31, 2016
Grant date	May 31, 2016

Abstract

Devices and techniques for combined forward and inverse synthetic aperture imaging LADAR (combined SAL) include scanning a non-stationary target with an optical signal emitted from a non-stationary laser source, receiving reflections of the signal on a receiver, and determining the combined synthetic aperture.

First claim

What is claimed is:

1. A method for combined forward and inverse synthetic aperture LADAR imaging comprising:
scanning a non-stationary target by emitting an optical signal from a non-stationary laser source;
receiving, by a receiver having a real aperture, one or more reflections of the optical signal from the non-stationary target, wherein the one or more reflections are received over an observational duration; and
determining, by a processor, an angular resolution θ res of a synthetic aperture of the receiver in an azimuth direction according to a wavelength λ of the optical signal, a velocity vector {right arrow over (V)} of the non-stationary laser source, an angle θ measured between an axis perpendicular to {right arrow over (V)} and the non-stationary target, an angular velocity vector {right arrow over (Ω)} of the non-stationary target, a distance R between the non-stationary laser source and the non-stationary target, and the observational duration T SA ;
wherein the angular resolution of the synthetic aperture of the receiver in the azimuth direction is narrower than an angular resolution of the real aperture of the receiver in the azimuth direction; and
wherein the angular resolution θ res of the synthetic aperture of the receiver in the azimuth direction is according to the relationship

θ
res

=

λ

2
⁢

(

V
→

⁢
cos
⁢

⁢
θ

+

Ω
→

·
R

)

·

T
SA

.

2. The method of claim 1 , further comprising:
dividing the angular resolution of the real aperture of the receiver into a plurality of range bins in the down-range direction, each of the range bins sized according to a range resolution of the optical signal; and
assigning each of the one or more reflections received by the receiver to at least one of the plurality of range bins.

3. The method of claim 2 , further comprising:
dividing the angular resolution of the real aperture of the receiver into at least one synthetic aperture resolution element, the at least one synthetic aperture resolution element having a width in the azimuth direction corresponding to the angular resolution of the synthetic aperture of the receiver and a length in the down-range direction corresponding to a size of one of the plurality of range bins.

4. The method of claim 3 , further comprising plotting, for the at least one synthetic aperture resolution element, a range-Doppler map of any of the one or more reflections located within the at least one synthetic aperture element.

5. The method of claim 2 , further comprising: applying motion compensation to the one or more reflections assigned to each of the range bins, wherein the motion compensation includes one or more of global motion compensation, motion estimation, block motion compensation, variable block-size motion compensation, overlapped block motion compensation; quarter pixel motion compensation, half pixel motion compensation, a block-matching algorithm, a phase correlation, a pixel recursive algorithm, optical flow methods, corner detection, and/or random sample consensus.

6. The method of claim 1 , wherein a waveform of the optical signal is a pulse waveform, a chirp waveform, and/or a more complex waveform with a large time-bandwidth product.

7. The method of claim 1 , further comprising correcting errors in data processed by the processor.

8. The method of claim 7 , wherein the errors are due to at least one of motion and turbulence.

9. A LADAR imaging system comprising:
a non-stationary laser source configured to emit an optical signal;
a receiver having a real aperture and configured to receive one or more reflections of the optical signal from a non-stationary target;
one or more processors configured to determine an angular resolution θ res of a synthetic aperture of the receiver in an azimuth direction according to a wavelength λ of the optical signal, a velocity vector {right arrow over (V)} of the non-stationary laser source, an angle θ measured between an axis perpendicular to {right arrow over (V)} and the non-stationary target, an angular velocity vector {right arrow over (Ω)} of the non-stationary target, a distance R between the non-stationary laser source and the non-stationary target, and the observational duration T SA ;
wherein the angular resolution of the synthetic aperture of the receiver in the azimuth direction is narrower than an angular resolution of the real aperture of the receiver in the azimuth direction; and
wherein the angular resolution θ res of the synthetic aperture of the receiver in the azimuth direction is according to the relationship

θ
res

=

λ

2
⁢

(

V
→

⁢
cos
⁢

⁢
θ

+

Ω
→

·
R

)

·

T
SA

.

10. The system of claim 9 , wherein the one or more processors are configured to:
divide the angular resolution of the real aperture of the receiver into a plurality of range bins in the down-range direction, each of the range bins sized according to a range resolution of the optical signal; and
assign each of the one or more reflections received by the receiver to at least one of the plurality of range bins.

Assignees

• Raytheon Co

Inventors

• Halmos Maurice J

Classifications

• G01S17/90 Primary

  using synthetic aperture techniques · CPC title

• G01S17/50

  Systems of measurement based on relative movement of target · CPC title

• G01S17/895 Primary

  Physics · mapped topic