CN103954963A - Step frequency SAR imaging method based on CS algorithm - Google Patents

Step frequency SAR imaging method based on CS algorithm Download PDF

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Publication number
CN103954963A
CN103954963A CN201410187122.6A CN201410187122A CN103954963A CN 103954963 A CN103954963 A CN 103954963A CN 201410187122 A CN201410187122 A CN 201410187122A CN 103954963 A CN103954963 A CN 103954963A
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frequency
signal
broadband
algorithm
carries out
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丁泽刚
曾涛
朱动林
高文斌
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Beijing Institute of Technology BIT
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Beijing Institute of Technology BIT
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    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • G01S13/9004SAR image acquisition techniques
    • G01S13/9011SAR image acquisition techniques with frequency domain processing of the SAR signals in azimuth
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S13/00Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
    • G01S13/88Radar or analogous systems specially adapted for specific applications
    • G01S13/89Radar or analogous systems specially adapted for specific applications for mapping or imaging
    • G01S13/90Radar or analogous systems specially adapted for specific applications for mapping or imaging using synthetic aperture techniques, e.g. synthetic aperture radar [SAR] techniques
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01SRADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
    • G01S7/00Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
    • G01S7/02Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
    • G01S7/28Details of pulse systems
    • G01S7/285Receivers
    • G01S7/295Means for transforming co-ordinates or for evaluating data, e.g. using computers

Abstract

The invention discloses a step frequency SAR imaging method based on a CS algorithm. With the method, step frequency SAR high-resolution imaging can be conducted. A frequency domain broadband splicing method is improved, under the condition that the operand is not increased, time domain broadband chirp signals with narrow pulse widths can be generated, the operation efficiency is high, and imaging can be performed on the generated chirp signals with the CS algorithm. Due to broadband synthesis, the signal to noise ratio of the range resolution and a point target is improved, and therefore compared with an existing synthetic algorithm, the step frequency SAR imaging method is more suitable for high-resolution imaging.

Description

A kind of Step Frequency SAR formation method based on CS algorithm
Technical field
The present invention relates to synthetic-aperture radar SAR technical field of imaging, be specifically related to a kind of Step Frequency SAR formation method based on CS algorithm.
Background technology
Synthetic-aperture radar (SAR) is a kind of high-resolution microwave imaging radar of round-the-clock, round-the-clock.Along with the development of technology, the resolution of SAR improves gradually, and the highest resolution of SAR system has reached 0.1m at present.There are some special problems in high-resolution acquisition, such as, in order to obtain the resolution of 0.1m, require the bandwidth transmitting to surpass 1.5GHz.Produce and concerning this Sampling for Wide-Band Signal for actual treatment being all difficulty very.
Step Frequency technology is that a kind of conventional distance of obtaining is to high-resolution technology.Ultra-broadband signal is synthesized by aftertreatment by one group of narrow band signal.The major advantage of Step Frequency technology is that the instant bandwidth transmitting will be much smaller than the bandwidth of final synthesized wideband signal, therefore Step Frequency SAR when obtaining identical high-resolution than common SAR to system require much lower, therefore distance can realize easily to high-resolution.
In Step Frequency SAR imaging based on Chirp scaling (CS) algorithm, by narrow band signal, generate broadband signal and need to carry out broadband splicing.At present, more efficient broadband joining method is frequency domain broadband joining method.The result of frequency domain broadband joining method is one dimension High Range Resolution, also pass through the broadband chirp signal of pulse compression, therefore it can only just carry out the algorithm apart from pulse pressure for first steps such as Range-Doppler (RD) algorithm, SPECAN algorithms, and can not before apart from pulse pressure, need to carry out the algorithm that nonlinear phase multiplies each other for CS algorithm etc.
Summary of the invention
In view of this, the invention provides a kind of Step Frequency SAR formation method based on CS algorithm, frequency domain broadband joining method is improved, making to splice result can carry out Step Frequency SAR high-resolution imaging by enough CS algorithms.
Step Frequency SAR formation method based on CS algorithm of the present invention comprises the steps:
Step 1, carries out broadband signal frequency spectrum by subpulse signal and synthesizes;
Step 2, the broadband signal frequency spectrum that step 1 is obtained is multiplied by a quadratic phase, and described quadratic phase is
H virt ( f ) = exp [ jπ f r 2 K virt ]
Wherein, f rrepresent frequency of distance, K virtfor frequency modulation rate,
K virt = - NΔf T p
Wherein, N represents stepped-frequency interval, and Δ f represents stepped-frequency interval, T pindicating impulse width;
Step 3, the broadband signal frequency spectrum that step 2 is obtained carries out IFFT and transforms to apart from time domain, obtains the chirp signal of a narrow pulsewidth wide bandwidth;
Step 4, the chirp signal of the narrow pulsewidth wide bandwidth that step 3 is synthesized carries out imaging processing for CS algorithm, obtains SAR imaging results.
Wherein, described step 1 comprises the steps:
Step 1.1, transforms to subpulse signal apart from frequency domain through FFT;
Step 1.2, is carrying out pulse compression apart from frequency domain antithetical phrase pulse signal;
Step 1.3, carries out zero padding, windowing at frequency domain antithetical phrase pulse signal frequency spectrum;
Step 1.4, the signal that step 1.3 is obtained carries out IFFT and transforms to time domain;
Step 1.5, carries out frequency domain displacement;
Step 1.6, the signal that step 1.5 is obtained carries out distance and transforms to frequency domain to FFT;
Step 1.7, does coherence stack by subpulse signal spectrum, obtains broadband signal frequency spectrum.
Beneficial effect:
The inventive method, in the situation that not increasing operand, can generate the time domain broadband chirp signal of narrow pulsewidth, and operation efficiency is higher, and synthetic result can be carried out imaging processing by enough CS class algorithms.The synthetic signal to noise ratio (S/N ratio) that has improved range resolution and point target in broadband, is therefore more suitable for high-resolution imaging than existing composition algorithm.
Accompanying drawing explanation
Fig. 1 is this method process flow diagram.
Fig. 2 (a) is the broadband splicing result in time domain against pulse pressure by narrow band signal frequency modulation rate; Fig. 2 (b) is the broadband splicing result in time domain against pulse pressure by frequency modulation rate of the present invention.
Fig. 3 is Area Objects imaging results, (a) is former figure; (b) be coarse resolution figure; (c) be broadband splicing+CS imaging results.
Embodiment
Below in conjunction with the accompanying drawing embodiment that develops simultaneously, describe the present invention.
The invention provides a kind of Step Frequency SAR formation method based on CS algorithm, first frequency domain broadband joining method is improved, compare with existing frequency domain broadband joining method, step before synthesized wideband signal frequency spectrum is identical, after synthesized wideband signal frequency spectrum, existing frequency domain broadband joining method directly carries out inverse fast Fourier transform (IFFT) to broadband signal frequency spectrum and obtains one dimension High Range Resolution, and the present invention also needs broadband signal frequency spectrum to be multiplied by a quadratic phase, carry out again afterwards IFFT to obtain a narrow pulsewidth, the chirp signal of wide bandwidth, then the broadband chirp signal of narrow pulsewidth is used to CS algorithm and carries out imaging processing, obtain final SAR image.Specifically comprise the following steps:
Step 1, broadband signal frequency spectrum synthesize
Subpulse signal expression for broadband splicing is
s ( t r , n ) = rect [ t r - 2 ( R - R min ) c T p ] · exp [ - jπ K r ( t r - 2 ( R - R min ) c ) 2 ] · exp [ - j 4 πR c ( f 0 + n · Δf ) ] - - - ( 1 )
Wherein, t rrepresent Distance Time, n represents frequency number, rect[] represent that gate function, R represent that radar and target distance are from, R minrepresent initial sampled distance, c represents the light velocity, T pindicating impulse width, K rrepresent signal chirp rate, f 0represent initial carrier frequency, N represents frequency modulation number of times, and Δ f represents stepped-frequency interval.
Through distance, to Fast Fourier Transform (FFT) (FFT), narrow band signal is transformed to apart from frequency domain, its expression formula is
S ( f r , n ) = rect [ f r B sub ] · exp [ - jπ f r 2 K r ] · exp [ - j 2 π f r 2 ( R - R min ) c ] · exp [ - j 4 πR c ( f 0 + n · Δf ) ] - - - ( 2 )
Wherein, f rrepresent frequency of distance, B subrepresent narrow band signal bandwidth.
Apart from frequency domain, narrow band signal is being carried out to pulse compression, the pulse compression factor is
H MF ( f r ) = exp [ jπ f r 2 K r ] - - - ( 3 )
Narrow band signal frequency spectrum after pulse compression is
S MF ( f r , n ) = rect [ f r B sub ] · exp [ - j 2 π f r 2 ( R - R min ) c ] · exp [ - j 4 πR c ( f 0 + n · Δf ) ] - - - ( 4 )
Because narrow band signal bandwidth is less, therefore sampling rate is lower and much smaller than broadband signal bandwidth, therefore need to carry out rising sampling to narrow band signal, this can realize by narrow band signal frequency spectrum blank space being carried out to zero padding at frequency domain.In addition, because narrow band signal bandwidth is generally greater than stepped-frequency interval, narrow band signal frequency spectrum need to carry out windowing and remove the lap between narrow band signal frequency spectrum, and this step is carried out together with frequency domain zero padding.
In order to carry out accurate frequency displacement, need to be by the narrow band signal Spectrum Conversion after pulse compression to time domain, the narrow band signal time-domain expression after pulse compression is
s MF ( t r , n ) = sin c [ Δf ( t r - 2 ( R - R min ) c ) ] · exp [ - j 4 πR c ( f 0 + n · Δf ) ] - - - ( 5 )
Sinc[wherein] represent sinc function.Frequency-shifting operator for frequency displacement is
φ fs ( t r , n ) = exp [ - j 2 π ( n - N - 1 2 ) Δf ( t r - 2 ( R - R min ) c ) ] - - - ( 6 )
Narrow band signal after multiplying each other with frequency-shifting operator is transformed to frequency domain through FFT, can obtain the narrow band signal frequency spectrum after frequency displacement, this spectrum expression formula is
S fs ( f r , n ) = rect [ f r - ( n - N - 1 2 ) Δf Δf ] · exp [ - j 2 π f r 2 ( R - R min ) c ] · exp [ - j 4 πR c ( f 0 + N - 1 2 · Δf ) ] - - - ( 7 )
Narrow band signal spectral overlay after each frequency displacement is got up, can obtain the broadband signal frequency spectrum of needs, broadband signal spectrum expression formula is
S wide ( f r ) = rect [ f r NΔf ] · exp [ - j 2 π f r 2 ( R - R min ) c ] · exp [ - j 4 πR c ( f 0 + N - 1 2 · Δf ) ] - - - ( 8 )
Step 2, narrow pulsewidth broadband chirp signal generate
In CS algorithm process, need to carry out CS processing to chirp signal, therefore need to not carry out the echo data apart from pulse pressure.Theoretically, only need to the broader frequency spectrum in formula (8), be multiplied by a quadratic phase at frequency domain, IFFT converts back time domain just can obtain a broadband chirp signal.But because the bandwidth of broadband signal is N times (wherein N represents stepped-frequency interval) of narrow band signal; if the frequency modulation rate of the quadratic phase multiplying each other is constant; the pulsewidth of broadband chirp signal can be also narrow band signal N doubly, this can cause data at time domain generation aliasing conventionally.Therefore it is infeasible, adopting the frequency modulation rate of narrow band signal to construct quadratic phase.According to existing conclusion, when bandwidth one timing, if frequency modulation rate increases, time domain pulsewidth reduces, therefore can consider to increase frequency modulation rate, constructs quadratic phase, the corresponding broadband chirp signal that can obtain a narrow pulsewidth.Its detailed process is as follows:
Broader frequency spectrum in formula (8) and a quadratic phase are multiplied each other, and this quadratic phase is
H virt ( f ) = exp [ jπ f r 2 K virt ] - - - ( 9 )
Wherein, K virtfor the frequency modulation rate after adjusting.Broader frequency spectrum after multiplying each other with quadratic phase can be expressed as
S virt ( f r ) = rect [ f r NΔf ] · exp [ - j 2 π f r 2 ( R - R min ) c ] · exp [ jπ f r 2 K virt ] · exp [ - j 4 πR c ( f 0 + N - 1 2 · Δf ) ] - - - ( 10 )
Through IFFT, convert back time domain, the broadband signal expression formula of time domain is
s virt ( t r ) = rect [ t r - 2 ( R - R min ) c | NΔf K virt | ] · exp [ j π K virt ( t r - 2 ( R - R min ) c ) 2 ] · exp [ - j 4 πR c ( f 0 + N - 1 2 · Δf ) ] - - - ( 11 )
From formula (11), the chirp signal that time domain forms, frequency modulation rate corresponding to quadratic phase that its frequency modulation rate is multiplied each other by frequency spectrum determine, pulsewidth is determined by the business of broadband signal bandwidth and frequency modulation rate.When frequency modulation rate is larger, the pulsewidth of time domain chirp signal is less.If get frequency modulation rate, be
K virt = - NΔf T p - - - ( 12 )
Time domain broadband chirp signal expression is
s virt 2 ( t r ) = rect [ t r - 2 ( R - R min ) c T p ] · exp [ j π ( - NΔf T p ) ( t r - 2 ( R - R min ) c ) 2 ] · exp [ - j 4 πR c ( f 0 + N - 1 2 · Δf ) ] - - - ( 13 )
Now chirp signal in broadband has and the identical pulsewidth of arrowband chirp signal, therefore can there is not time domain aliasing.Because processing is counted and is not increased, thus this synthetic method and traditional frequency domain broadband synthetic method to compare calculated amount basic identical.In addition, the result finally generating is chirp signal, and this synthetic method can be used in CS algorithm and carries out imaging processing.
Step 3, CS algorithm imaging processing
Broadband chirp signal through the synthetic narrow pulsewidth of step 2 will carry out imaging processing for CS algorithm, wherein the treatment scheme of CS algorithm is identical with the treatment scheme of classical CS algorithm: by the broadband chirp signal of narrow pulsewidth through orientation to FFT, the CS factor multiply each other, distance multiplies each other to FFT, distance to compensating factor, distance multiplies each other to IFFT, orientation to compensating factor and orientation to IFFT, obtain final SAR imaging results.
For the broadband synthetic method of verifying that the present invention provides, carried out relevant emulation, adopt narrow band signal frequency modulation rate against the broadband of pulse pressure acquisition, to splice result in time domain as shown in Figure 2 against the frequency modulation rate of pulse pressure and the present invention's employing, can find out, if the frequency modulation rate of using while not changing contrary pulse pressure, can there is time domain aliasing (Fig. 2 (a)), and change after the frequency modulation rate of contrary pulse pressure use, the pulsewidth of time domain chirp signal becomes very narrow (Fig. 2 (b)), therefore there will not be time domain aliasing.In order to verify the validity of the method, also carry out Area Objects emulation.Emulation former figure used and imaging results as shown in Figure 3, can find out, utilizes the method to use CS imaging to count in the situation that not increasing distance, and imaging results and former figure difference little, can meet the requirement of imaging.
In sum, these are only preferred embodiment of the present invention, be not intended to limit protection scope of the present invention.Within the spirit and principles in the present invention all, any modification of doing, be equal to replacement, improvement etc., within all should being included in protection scope of the present invention.

Claims (2)

1. the Step Frequency SAR formation method based on CS algorithm, is characterized in that, comprises the steps:
Step 1, carries out broadband signal frequency spectrum by subpulse signal and synthesizes;
Step 2, the broadband signal frequency spectrum that step 1 is obtained is multiplied by a quadratic phase, and described quadratic phase is
H virt ( f ) = exp [ jπ f r 2 K virt ]
Wherein, f rrepresent frequency of distance, K virtfor frequency modulation rate,
K virt = - NΔf T p
Wherein, N represents stepped-frequency interval, and Δ f represents stepped-frequency interval, T pindicating impulse width;
Step 3, the broadband signal frequency spectrum that step 2 is obtained carries out IFFT and transforms to apart from time domain, obtains the chirp signal of a narrow pulsewidth wide bandwidth;
Step 4, the chirp signal of the narrow pulsewidth wide bandwidth that step 3 is synthesized carries out imaging processing for CS algorithm, obtains SAR imaging results.
2. the Step Frequency SAR frequency domain broadband joining method for CS algorithm as claimed in claim 1, is characterized in that, described step 1 comprises the steps:
Step 1.1, transforms to subpulse signal apart from frequency domain through FFT;
Step 1.2, is carrying out pulse compression apart from frequency domain antithetical phrase pulse signal;
Step 1.3, carries out zero padding, windowing at frequency domain antithetical phrase pulse signal frequency spectrum;
Step 1.4, the signal that step 1.3 is obtained carries out IFFT and transforms to time domain;
Step 1.5, carries out frequency domain displacement;
Step 1.6, the signal that step 1.5 is obtained carries out distance and transforms to frequency domain to FFT;
Step 1.7, does coherence stack by subpulse signal spectrum, obtains broadband signal frequency spectrum.
CN201410187122.6A 2014-05-05 2014-05-05 Step frequency SAR imaging method based on CS algorithm Pending CN103954963A (en)

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110109101A (en) * 2019-04-04 2019-08-09 电子科技大学 A kind of compressed sensing three-dimensional S AR imaging method based on adaptive threshold
CN112462335A (en) * 2021-01-26 2021-03-09 四川写正智能科技有限公司 Multifunctional 3D radar transceiver and operation method
CN112731392A (en) * 2020-12-15 2021-04-30 中国科学院空天信息创新研究院 High-efficiency terahertz step frequency synthetic aperture radar imaging method
CN114626006A (en) * 2022-03-21 2022-06-14 电子科技大学 FPGA (field programmable Gate array) realization method for real-time generation of CS (Circuit switched) algorithm compensation factor in radar imaging

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6343510B1 (en) * 1999-04-22 2002-02-05 Vn Instruments Limited Ultrasonic testing using synthetic impulses
US6750809B1 (en) * 2003-04-15 2004-06-15 Raytheon Company High resolution SAR processing using stepped frequency chirp waveform
CN101984363A (en) * 2010-10-27 2011-03-09 南京航空航天大学 Ultrahigh-resolution synthetic aperture radar (SAR) imaging method based on frequency-stepped system
CN102901964A (en) * 2012-09-06 2013-01-30 内蒙古工业大学 Two-dimensional multi-aperture scan synthetic aperture radar (SAR) imaging method
CN103472449A (en) * 2013-09-16 2013-12-25 电子科技大学 BP wideband synthesis method based on MIMO image domain

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6343510B1 (en) * 1999-04-22 2002-02-05 Vn Instruments Limited Ultrasonic testing using synthetic impulses
US6750809B1 (en) * 2003-04-15 2004-06-15 Raytheon Company High resolution SAR processing using stepped frequency chirp waveform
CN101984363A (en) * 2010-10-27 2011-03-09 南京航空航天大学 Ultrahigh-resolution synthetic aperture radar (SAR) imaging method based on frequency-stepped system
CN102901964A (en) * 2012-09-06 2013-01-30 内蒙古工业大学 Two-dimensional multi-aperture scan synthetic aperture radar (SAR) imaging method
CN103472449A (en) * 2013-09-16 2013-12-25 电子科技大学 BP wideband synthesis method based on MIMO image domain

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
王岩飞等: ""基于多通道合成的优于0.1m分辨率的机载SAR系统"", 《电子与信息学报》, vol. 35, no. 1, 31 January 2013 (2013-01-31) *
黄平平等: ""基于CS算法的MIMO-SAR成像研究"", 《电子科技大学学报》, vol. 41, no. 2, 31 March 2012 (2012-03-31) *

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN110109101A (en) * 2019-04-04 2019-08-09 电子科技大学 A kind of compressed sensing three-dimensional S AR imaging method based on adaptive threshold
CN112731392A (en) * 2020-12-15 2021-04-30 中国科学院空天信息创新研究院 High-efficiency terahertz step frequency synthetic aperture radar imaging method
CN112731392B (en) * 2020-12-15 2023-07-04 中国科学院空天信息创新研究院 Efficient terahertz step frequency synthetic aperture radar imaging method
CN112462335A (en) * 2021-01-26 2021-03-09 四川写正智能科技有限公司 Multifunctional 3D radar transceiver and operation method
CN112462335B (en) * 2021-01-26 2021-05-18 四川写正智能科技有限公司 Multifunctional 3D radar transceiver and operation method
CN114626006A (en) * 2022-03-21 2022-06-14 电子科技大学 FPGA (field programmable Gate array) realization method for real-time generation of CS (Circuit switched) algorithm compensation factor in radar imaging
CN114626006B (en) * 2022-03-21 2023-03-14 电子科技大学 FPGA (field programmable Gate array) realization method for real-time generation of CS (Circuit switched) algorithm compensation factor in radar imaging

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Application publication date: 20140730