CN113721218A - Heterogeneous radar multiband bandwidth synthesis method and system - Google Patents

Heterogeneous radar multiband bandwidth synthesis method and system Download PDF

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CN113721218A
CN113721218A CN202111098818.8A CN202111098818A CN113721218A CN 113721218 A CN113721218 A CN 113721218A CN 202111098818 A CN202111098818 A CN 202111098818A CN 113721218 A CN113721218 A CN 113721218A
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echo signal
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echo
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CN113721218B (en
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张硕
杨君
葛鹏程
冯婷婷
杜钰
姜浩浩
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Peoples Liberation Army Strategic Support Force Aerospace Engineering University
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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
    • 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
    • G01S7/41Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section
    • G01S7/418Theoretical aspects
    • 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
    • G01S7/41Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00 using analysis of echo signal for target characterisation; Target signature; Target cross-section
    • G01S7/414Discriminating targets with respect to background clutter
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
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Abstract

The invention relates to a method and a system for synthesizing a multi-band bandwidth of a heterologous radar. The method comprises the steps of measuring echo signals of different frequency bands of the same target by using different radars; determining a DE model of echo signals of corresponding frequency bands according to the echo signals of different frequency bands; taking any echo signal as a reference echo signal, solving the pole and the amplitude of an all-pole DE model of the echo signal of the residual frequency band by adopting an improved TLS-ESPRIT algorithm, estimating and compensating non-phase parameters contained in the pole and the amplitude, and performing coherent registration on non-coherent multi-segment echo signals; and reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration, and reconstructing a full-frequency-band echo signal by combining an improved TLS-ESPRIT algorithm. The method and the device can improve the accuracy of the data reconstruction of the heterogeneous radar multiband.

Description

Heterogeneous radar multiband bandwidth synthesis method and system
Technical Field
The invention relates to the field of radar data reconstruction, in particular to a heterogeneous radar multiband bandwidth synthesis method and system.
Background
The existing heterogeneous radar multiband data reconstruction, namely multiband fusion broadband coherent processing, mainly comprises two main methods, namely a spectrum estimation method and a sparse reconstruction method. Most of spectrum estimation methods are difficult to estimate model orders and sensitive to noise, and a sparse reconstruction method based on compressed sensing has the possibility of failure as a method for reconstructing signals with high probability due to more iteration times and larger calculated amount.
Therefore, a method or system is needed to solve the above problems.
Disclosure of Invention
The invention aims to provide a heterogeneous radar multiband bandwidth synthesis method and system, which can improve the accuracy of data reconstruction of the heterogeneous radar multiband.
In order to achieve the purpose, the invention provides the following scheme:
a heterogeneous radar multiband bandwidth synthesis method comprises the following steps:
measuring echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
determining attenuation index (DE) models of echo signals of corresponding frequency bands according to the echo signals of different frequency bands; the DE model is an all-pole DE model;
taking any echo Signal as a reference echo Signal, solving the pole and the amplitude of an all-pole DE model of the echo signals of the residual frequency band by adopting an improved Total Least square-rotation invariant technical Signal parameter estimation (TLS-ESPRIT) algorithm, Estimating and compensating non-phase parameters contained in the pole and the amplitude, and enabling the non-coherent multi-section echo signals to be coherent and registered;
and reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration, and reconstructing a full-frequency-band echo signal by combining an improved TLS-ESPRIT algorithm.
Optionally, determining a DE model of the echo signal of the corresponding frequency band according to the echo signals of different frequency bands specifically includes:
carrying out spline interpolation homogenization treatment on echo signals of different frequency bands;
and determining a DE model of the echo signals of the corresponding frequency bands according to the processed echo signals of different frequency bands and a geometric diffraction theory.
Optionally, the method for performing coherent registration on multiple echo signals with non-coherent segments includes:
using formulas
Figure BDA0003269963890000021
Carrying out all-pole DE model coherent registration;
wherein the content of the first and second substances,
Figure BDA0003269963890000022
for the coherent registered all-pole DE model, s2For the unregistered echo signal, j is the imaginary unit j ═ sqrt (-1), N2Number of frequency samples, n, corresponding to the coherent registered echo2=0,1,…,N2-1,
Figure BDA0003269963890000023
Is an estimate of the fixed phase term,
Figure BDA0003269963890000024
is an estimate of the linear phase term.
Optionally, the reconstructing an echo signal by using a Hankel matrix and the echo signal after the coherent registration and reconstructing a full-band echo signal by combining an improved TLS-ESPRIT algorithm specifically includes:
determining parameters of an all-band all-pole DE model by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
according to the parameters of the full-band all-pole DE model, using a formula
Figure BDA0003269963890000025
Reconstructing a full-band echo signal;
wherein Q is the number of target scattering centers, N is the length of a full-band signal, and diIs the amplitude coefficient, P, of the ith scattering centeriN-1, which is the pole of the ith scattering center, 0, 1.
A heteroradar multiband bandwidth synthesis system, comprising:
the echo signal acquisition module is used for measuring echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
the model determining module is used for determining a DE model of the echo signal of the corresponding frequency band according to the echo signals of different frequency bands; the DE model is an all-pole DE model;
the coherent registration module is used for solving the pole and the amplitude of an all-pole DE model of the echo signals of the residual frequency band by adopting an improved TLS-ESPRIT algorithm by taking any echo signal as a reference echo signal, estimating and compensating non-coherent parameters contained in the pole and the amplitude, and performing coherent registration on non-coherent multi-section echo signals;
and the full-band echo signal reconstruction module is used for reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration and reconstructing the full-band echo signal by combining an improved TLS-ESPRIT algorithm.
Optionally, the echo signal attenuation index and model determining module specifically includes:
the spline interpolation homogenization processing unit is used for carrying out spline interpolation homogenization processing on the echo signals of different frequency bands;
and the attenuation index and model determining unit of the echo signals is used for determining a DE model of the echo signals of the corresponding frequency bands according to the processed echo signals of different frequency bands and a geometric diffraction theory.
Optionally, the coherent registration module specifically includes:
a coherent registration unit for utilizing the formula
Figure BDA0003269963890000031
Carrying out all-pole DE model coherent registration;
wherein the content of the first and second substances,
Figure BDA0003269963890000032
for the coherent registered all-pole DE model, s2For the unregistered echo signal, j is the imaginary unit j ═ sqrt (-1), N2Number of frequency samples, n, corresponding to the coherent registered echo2=0,1,…,N2-1,
Figure BDA0003269963890000033
Is an estimate of the fixed phase term,
Figure BDA0003269963890000034
is an estimate of the linear phase term.
Optionally, the full-band echo signal reconstructing module specifically includes:
the echo processing data determining unit of the all-band all-pole is used for determining all-band all-pole DE model parameters by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
full-band echo signal reconstruction unit for formula
Figure BDA0003269963890000035
Reconstructing a full-band echo signal;
wherein Q is the number of target scattering centers, N is the length of a full-band signal, and diIs the amplitude coefficient, P, of the ith scattering centeriN-1, which is the pole of the ith scattering center, 0, 1.
According to the specific embodiment provided by the invention, the invention discloses the following technical effects:
according to the method and the system for synthesizing the multi-band bandwidth of the heterologous radar, an improved TLS-ESPRIT algorithm is adopted to obtain the attenuation index of an echo signal of a residual frequency band and the pole and the amplitude of a model; the full-band echo signal is reconstructed based on the Hankel matrix and the improved TLS-ESPRIT algorithm, so that the problems of distance image blurring caused by insufficient bandwidth in space target monitoring and identification under the condition of low signal-to-noise ratio, large number of targets in the missile target range or the missile early warning system, different sizes and the like and high resolution difficulty are effectively solved. The improved TLS-ESPRIT-based heterogeneous radar multiband fusion coherent processing method has the characteristics of high precision, high efficiency and good noise resistance. Furthermore, the accuracy of the data reconstruction of the heterogeneous radar multiband is effectively improved.
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In order to more clearly illustrate the embodiments of the present invention or the technical solutions in the prior art, the drawings required to be used in the embodiments will be briefly described below, and it is obvious that the drawings in the following description are only some embodiments of the present invention, and it is obvious for those skilled in the art that other drawings can be obtained according to the drawings without inventive labor.
Fig. 1 is a schematic flow chart of a method for synthesizing a multiband bandwidth of a radar system according to the present invention;
fig. 2 is a schematic structural diagram of a hetero-radar multi-band bandwidth synthesis system provided by the present invention.
Detailed Description
The technical solutions in the embodiments of the present invention will be described clearly and completely with reference to the accompanying drawings in the embodiments of the present invention, and it is obvious that the described embodiments are only a part of the embodiments of the present invention, and not all of the embodiments. All other embodiments, which can be derived by a person skilled in the art from the embodiments given herein without making any creative effort, shall fall within the protection scope of the present invention.
The invention aims to provide a heterogeneous radar multiband bandwidth synthesis method and system, which can improve the accuracy of data reconstruction of the heterogeneous radar multiband.
In order to make the aforementioned objects, features and advantages of the present invention comprehensible, embodiments accompanied with figures are described in further detail below.
Fig. 1 is a schematic flow chart of a method for synthesizing a multi-band bandwidth of a radar diversity system according to the present invention, as shown in fig. 1, the method for synthesizing a multi-band bandwidth of a radar diversity system according to the present invention includes:
s101, measuring echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
namely, two radars satisfy the principle of adjacent registration; the proximity registration principle is that the spacing between radars is smaller than the radar-to-target radial distance, and the spacing between radars is much smaller than the radar-to-target radial distance.
S102, determining attenuation indexes and DE models of echo signals of corresponding frequency bands according to the echo signals of different frequency bands; the DE model is an all-pole DE model;
s102 specifically comprises the following steps:
carrying out spline interpolation homogenization treatment on echo signals of different frequency bands;
and determining attenuation indexes and models of the echo signals of the corresponding frequency bands according to the processed echo signals of different frequency bands and a geometric diffraction theory.
The specific establishing process of the attenuation index and the model of the echo signal is as follows:
two radars working independently are set, and the initial carrier frequencies under adjacent registration are respectively f1,f2The number of frequency samples is N1,N2The frequency sampling interval of both is delta f, the blank band width between the initial carrier frequencies is delta B, and f2=f1+ Δ B. The baseband echoes of two radars of a stationary target consisting of Q scattering points can be represented as:
Figure BDA0003269963890000051
Figure BDA0003269963890000052
the two above formulas are respectively s1And s2The Geometric Theory of Diffraction (GTD) model, where j is sqrt (-1), model parameters
Figure BDA0003269963890000061
Collectively, the characteristics of the Q scattering centers described above are shown. A. theiIs the amplitude of the scattering center, riIs the distance of the scattering center from a reference point, αiThe diffraction term coefficient (shown in Table 1) is an integral multiple of 0.5. f. ofn=f1+n·Δf,fn'=f2+ n'. DELTA.f, c is the propagation velocity of the electromagnetic wave in air, here approximately the speed of light. Gamma ray1And gamma2Are respectively s1And s2The non-coherent quantities of the fixed phase term and the linear phase term existing in between.
In a relative bandwidth of not large
Figure BDA0003269963890000062
When is driven by s1For example, the GTD model may be approximated as follows:
Figure BDA0003269963890000063
will f isn、fn'And (3) substituting the expressions into the expressions (1) and (2) to obtain attenuation indexes of corresponding echoes and the expressions (4) and (5) of the models, and equivalent to an all-pole model.
Figure BDA0003269963890000064
Figure RE-GDA0003321045020000064
Wherein P is1i、P2iAre respectively s1,s2The pole of (a); d1i、d2iAre respectively s1,s2The pole of (a) corresponds to the amplitude coefficient. When two radars are arranged adjacently, the target scattering center intensity, namely the amplitude, can be normalized on a frequency domain. And it is the phase relationship of the signals that mainly affects the imaging quality, so it can be assumed that a is belowi=1。
TABLE 1
Figure BDA0003269963890000071
S103, with any echo signal as a reference echo signal, solving the pole and the amplitude of an all-pole DE model of the echo signal of the residual frequency band by adopting an improved total least square-rotation invariant technology signal parameter estimation TLS-ESPRIT algorithm, estimating and compensating non-phase parameters contained in the pole and the amplitude, and enabling the non-phase-coherent multi-section echo signals to be in coherent registration;
s103 specifically comprises the following steps:
using formulas
Figure BDA0003269963890000072
Carrying out all-pole DE model coherent registration;
wherein the content of the first and second substances,
Figure BDA0003269963890000073
for the coherent registered all-pole DE model, s2For the unregistered echo signal, j is the imaginary unit j ═ sqrt (-1), N2Number of frequency samples, n, corresponding to the coherent registered echo2=0,1,…,N2-1,
Figure BDA0003269963890000074
Is an estimate of the fixed phase term,
Figure BDA0003269963890000075
is an estimate of the linear phase term.
The process of solving the pole and the amplitude of the all-pole DE model of the echo signals of the residual frequency bands by adopting the improved TLS-ESPRIT algorithm comprises the following steps:
definitions x (N) ═ s (N), N ═ 1,2, … N, y (N) ═ s (N + 1). Is provided with
Figure BDA0003269963890000076
Wherein Q is the number of scattering centers and N is the signal length; introduction of M0X 1-dimensional vector:
X(n)=[s(n),s(n+1),…,s(n+M0-1)]T
n=1,2,…N;
Y(n)=[s(n+1),s(n+2),…,s(n+M0)]T
n=1,2,…N;
then, the estimated values of the autocorrelation matrix and the cross-correlation matrix thereof can be respectively expressed as:
Figure BDA0003269963890000077
Figure BDA0003269963890000081
by using
Figure BDA0003269963890000082
Direct pair autocorrelation function RXXCarrying out singular value decomposition;
determining the effective order of the model by utilizing the regular correlation technique, and taking the diagonal matrix sigma corresponding to Q main left singular valuesZ1,UZ1And VZ1The matrix is formed by Q main left and right singular vectors, and the product of the vectors is used as a signal subspace. SigmaZ2Diagonal matrix, U, composed of non-dominant singular valuesZ2And VZ2The matrices formed by the non-dominant left and right singular vectors are multiplied to form a noise subspace.
According to the obtained sigma, the minimum singular value is taken and recorded as sigma2Constructing a covariance matrix Cxy=Rxy-σ2I';
Using obtained sigmaZ1
Figure BDA0003269963890000083
Cxy、VZ1Building a matrix bundle
Figure BDA0003269963890000084
Solving the generalized eigenvalue of the matrix beam is the pole PiAnalogically determining the pole in each echo segment, and combining the equations
Figure BDA0003269963890000085
That is, the estimated value of the linear phase term can be obtained
Figure BDA0003269963890000086
And (3) amplitude estimation process:
according to the obtained model pole
Figure BDA0003269963890000087
By passing
Figure BDA0003269963890000088
Find out the
Figure BDA0003269963890000089
Individual pole and its corresponding amplitude coefficient
Figure BDA00032699638900000810
In the formula
Figure BDA00032699638900000811
Is made by
Figure BDA00032699638900000812
The Vandermonde matrix generated by each pole.
When two radars collect echo signals of the same target under coherent registration, non-coherent quantities between the two radars can be summarized into a linear phase term contained in a pole and a fixed phase term contained in amplitude.
Figure BDA00032699638900000813
Figure BDA00032699638900000814
Wherein, γ1' is a fixed phase term, γ2' is a linear phase term. p is a radical of1i、p2iAre respectively s1,s2The pole of (a); d1i、d2iAre respectively s1,s2The pole of (a) corresponds to the amplitude coefficient.
And S104, reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration, and reconstructing a full-band echo signal by combining an improved TLS-ESPRIT algorithm.
S104 specifically comprises the following steps:
determining a full-band all-pole model as follows:
Figure BDA0003269963890000091
wherein j ═ sqrt (-1), AiFor echo signal amplitude, Q represents the number of scattering centers of the target, αiFor the diffraction term coefficients (as shown in table 1),
Figure RE-GDA0003321045020000094
is the frequency sampling interval, B is the full-band signal bandwidth, N is the full-band signal length, f0A carrier frequency is initiated for the signal. r isi=Ri-Rref,RiRadial distance, R, from the i-th scattering center to the radarrefIs a reference distance;
determining parameters of an all-band all-pole DE model by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
according to the parameters of the full-band all-pole DE model, using a formula
Figure BDA0003269963890000093
Reconstructing a full-band echo signal;
and a vacant frequency band exists between the high frequency band and the low frequency band after the coherent registration, and a new matrix needs to be constructed in order to continue to use the improved TLS-ESPRIT algorithm to complete parameter estimation of the full-frequency band all-pole model. Therefore, an improved TLS-ESPRIT all-band all-pole model solving method based on the Hankel matrix is provided. According to the method, a Hankel matrix is introduced during multi-band echo signal processing, and the influence of noise on signals is greatly reduced by using the special properties of a special structure of the Hankel matrix.
Rearrangement into a form with a Hankel matrix, namely:
Figure BDA0003269963890000101
Figure BDA0003269963890000102
where L is often 1/3 the signal length. Composed new matrix
Figure BDA0003269963890000103
Echo processing data as full band all poles;
reconstructing a full-band echo signal by adopting an improved TLS-ESPRIT algorithm according to the echo processing data of the full-band all-pole and the full-band all-pole model;
and obtaining estimation data of each sub-band and the vacant frequency band:
Figure BDA0003269963890000104
in order to reduce estimation errors, raw measurement data may be used as much as possible. Thus, the full-band bandwidth extrapolated fusion signal can be expressed as:
Figure BDA0003269963890000105
the Hankel matrix greatly reduces the influence of noise on signals by utilizing the special property of a special structure of the Hankel matrix; second, the improved TLS-ESPRIT corrects for noise present in both signal subspaces by perturbing the signal subspaces of both data matrices simultaneously and keeping the square of the perturbation norm to a minimum.
Therefore, the full-band echo signal estimated by the algorithm is closer to the original target echo signal acquired by an ideal full-band radar (the initial carrier frequency of a low-band radar is taken as the initial carrier frequency of the full band, and the total synthesized bandwidth is taken as the actual bandwidth of the full-band radar). The method is embodied in that the estimation and compensation precision of the multiband phase to be registered (a linear phase term and a fixed phase term) and the extrapolation data is high, and the calculation efficiency is high.
Fig. 2 is a schematic structural diagram of a hetero-radar multi-band bandwidth synthesis system provided by the present invention, and as shown in fig. 2, the hetero-radar multi-band bandwidth synthesis system provided by the present invention includes:
an echo signal acquiring module 201, configured to measure echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
an attenuation index and model determining module 202 for echo signals, configured to determine a DE model of echo signals of corresponding frequency bands according to echo signals of different frequency bands; the DE model is an all-pole DE model;
the coherent registration module 203 is configured to use any echo signal as a reference echo signal, solve the pole and amplitude of the all-pole DE model of the echo signal of the remaining frequency band by using an improved TLS-ESPRIT algorithm, estimate and compensate non-coherent parameters included in the pole and amplitude, and perform coherent registration on non-coherent multiple echo signals;
and the full-band echo signal reconstruction module 204 is configured to reconstruct an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration, and reconstruct a full-band echo signal by combining with an improved TLS-ESPRIT algorithm.
The echo signal attenuation index and model determining module 202 specifically includes:
the spline interpolation homogenization processing unit is used for carrying out spline interpolation homogenization processing on the echo signals of different frequency bands;
and the attenuation index and model determining unit of the echo signals is used for determining an ED model of the echo signals of the corresponding frequency band according to the processed echo signals of different frequency bands and a geometric diffraction theory.
The coherent registration module 203 specifically includes:
a coherent registration unit for utilizing the formula
Figure BDA0003269963890000111
Carrying out all-pole DE model coherent registration;
wherein
Figure BDA0003269963890000112
For the coherent registered all-pole DE model, s1For the unregistered echo signal, j is the imaginary unit j ═ sqrt (-1), N2Number of frequency samples, n, corresponding to the coherent registered echo2=0,1,…,N2-1,
Figure BDA0003269963890000113
Is an estimate of the fixed phase term,
Figure BDA0003269963890000114
is an estimate of the linear phase term.
The full-band echo signal reconstruction module 204 specifically includes:
the echo processing data determining unit of the all-band all-pole is used for determining all-band all-pole DE model parameters by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
full-band echo signal reconstruction unit for formula
Figure BDA0003269963890000121
Reconstructing a full-band echo signal;
wherein Q is the number of target scattering centers, N is the length of a full-band signal, and diIs the amplitude coefficient of the ith scattering center, PiN-1, which is the pole of the ith scattering center, 0, 1.
The embodiments in the present description are described in a progressive manner, each embodiment focuses on differences from other embodiments, and the same and similar parts among the embodiments are referred to each other. For the system disclosed by the embodiment, the description is relatively simple because the system corresponds to the method disclosed by the embodiment, and the relevant points can be referred to the method part for description.
The principles and embodiments of the present invention have been described herein using specific examples, which are provided only to help understand the method and the core concept of the present invention; meanwhile, for a person skilled in the art, according to the idea of the present invention, the specific embodiments and the application range may be changed. In view of the above, the present disclosure should not be construed as limiting the invention.

Claims (8)

1. A method for synthesizing a multiband bandwidth of a heterologous radar, comprising:
measuring echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
determining attenuation indexes and DE models of echo signals of corresponding frequency bands according to the echo signals of different frequency bands; the DE model is an all-pole DE model;
taking any echo signal as a reference echo signal, solving the pole and the amplitude of an all-pole DE model of the echo signal of the residual frequency band by adopting an improved total least square-rotation invariant technology signal parameter estimation TLS-ESPRIT algorithm, estimating and compensating non-phase parameters contained in the pole and the amplitude, and performing coherent registration on non-coherent multi-segment echo signals;
and reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration, and reconstructing a full-frequency-band echo signal by combining an improved TLS-ESPRIT algorithm.
2. The method according to claim 1, wherein the determining the DE model of the echo signals of the corresponding frequency band according to the echo signals of the different frequency bands specifically comprises:
carrying out spline interpolation homogenization treatment on echo signals of different frequency bands;
and determining a DE model of the echo signals of the corresponding frequency bands according to the processed echo signals of different frequency bands and a geometric diffraction theory.
3. The method according to claim 1, wherein any echo signal is used as a reference echo signal, an improved overall least squares-rotation invariant technology signal parameter estimation TLS-ESPRIT algorithm is used to solve the pole and amplitude of an all-pole DE model of the echo signals of the remaining frequency bands, and non-coherent parameters included in the pole and amplitude are estimated and compensated, so that non-coherent multi-segment echo signals are subjected to coherent registration, specifically comprising:
using formulas
Figure FDA0003269963880000011
Carrying out all-pole DE model coherent registration;
wherein the content of the first and second substances,
Figure FDA0003269963880000012
for the coherent registered all-pole DE model, s2For the unregistered echo signal, j is the imaginary unit j ═ sqrt(-1),N2Number of frequency samples, n, corresponding to the coherent registered echo2=0,1,…,N2-1,
Figure FDA0003269963880000013
Is an estimate of the fixed phase term,
Figure FDA0003269963880000014
is an estimate of the linear phase term.
4. The method as claimed in claim 1, wherein the reconstructing echo signals of the reference echo signal and the echo signals after coherent registration by using a Hankel matrix and reconstructing full-band echo signals by combining with an improved TLS-ESPRIT algorithm specifically comprises:
determining parameters of an all-band all-pole DE model by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
according to the parameters of the full-band all-pole DE model, using a formula
Figure FDA0003269963880000021
Reconstructing a full-band echo signal;
wherein Q is the number of target scattering centers, N is the length of a full-band signal, and diIs the amplitude coefficient, P, of the ith scattering centeriN-1, which is the pole of the ith scattering center, 0, 1.
5. A heteroradar multiband bandwidth synthesis system, comprising:
the echo signal acquisition module is used for measuring echo signals of different frequency bands of the same target by using different radars; different radar initial carrier frequencies are different; the distance between the radars is smaller than the radial distance from the radars to the target; the difference of the visual angles between the radars is between 5 and 10 degrees;
the model determining module is used for determining a DE model of the echo signal of the corresponding frequency band according to the echo signals of different frequency bands; the DE model is an all-pole DE model;
the coherent registration module is used for solving the pole and the amplitude of an all-pole DE model of the echo signals of the residual frequency band by adopting an improved TLS-ESPRIT algorithm by taking any echo signal as a reference echo signal, estimating and compensating non-coherent parameters contained in the pole and the amplitude, and performing coherent registration on non-coherent multi-section echo signals;
and the full-band echo signal reconstruction module is used for reconstructing an echo signal by using a Hankel matrix according to the reference echo signal and the echo signal after the coherent registration and reconstructing the full-band echo signal by combining an improved TLS-ESPRIT algorithm.
6. The hetero-radar multi-band bandwidth synthesis system of claim 5, wherein the echo signal attenuation index and model determination module specifically comprises:
the spline interpolation homogenization processing unit is used for carrying out spline interpolation homogenization processing on the echo signals of different frequency bands;
and the attenuation index and model determining unit of the echo signals is used for determining a DE model of the echo signals of the corresponding frequency bands according to the processed echo signals of different frequency bands and a geometric diffraction theory.
7. The hetero-radar multi-band bandwidth synthesis system of claim 5, wherein the coherent registration module specifically comprises:
a coherent registration unit for utilizing the formula
Figure FDA0003269963880000031
Carrying out all-pole DE model coherent registration;
wherein the content of the first and second substances,
Figure FDA0003269963880000032
for the coherent registered all-pole DE model, s2For the unregistered echo signal, j is the imaginary unit j ═ sqrt (-1), N2Are coherentFrequency sampling number n corresponding to the registered echo2=0,1,…,N2-1,
Figure FDA0003269963880000033
Is an estimate of the fixed phase term,
Figure FDA0003269963880000034
is an estimate of the linear phase term.
8. The hetero-radar multi-band bandwidth synthesis system of claim 5, wherein the full-band echo signal reconstruction module specifically comprises:
the echo processing data determining unit of the all-band all-pole is used for determining all-band all-pole DE model parameters by combining a Hankel matrix and a TLS-ESPRIT algorithm according to the reference echo signal and the echo signal after the coherent registration;
full-band echo signal reconstruction unit for formula
Figure FDA0003269963880000035
Reconstructing a full-band echo signal;
wherein Q is the number of target scattering centers, N is the length of a full-band signal, and diIs the amplitude coefficient, P, of the ith scattering centeriN-1, which is the pole of the ith scattering center, 0, 1.
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