CN110109061B - Frequency spectrum zero setting signal design method based on template matching - Google Patents

Frequency spectrum zero setting signal design method based on template matching Download PDF

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CN110109061B
CN110109061B CN201910274637.2A CN201910274637A CN110109061B CN 110109061 B CN110109061 B CN 110109061B CN 201910274637 A CN201910274637 A CN 201910274637A CN 110109061 B CN110109061 B CN 110109061B
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杨晓波
杨婧
崔国龙
蒋歆玥
葛萌萌
余显祥
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University of Electronic Science and Technology of China
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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
    • G01S7/023Interference mitigation, e.g. reducing or avoiding non-intentional interference with other HF-transmitters, base station transmitters for mobile communication or other radar systems, e.g. using electro-magnetic interference [EMI] reduction 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
    • G01S7/282Transmitters
    • 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
    • G01S7/35Details of non-pulse systems

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Abstract

The invention discloses a frequency spectrum zero setting signal design method based on template matching, belongs to the field of radar signal processing, and particularly relates to a radar fast time domain signal design method which is suitable for multi-system frequency spectrum coexistence under radar anti-interference or frequency spectrum resource shortage in a narrow-band interference environment. Aiming at the problem of template matching and fitting, the method has higher descending speed and convergence speed, better fitting effect with the template and better optimization effect, and in addition, compared with other template algorithms, the algorithm used by the method has lower calculation complexity and improves the algorithm efficiency.

Description

Frequency spectrum zero setting signal design method based on template matching
Technical Field
The invention belongs to the field of radar signal processing, and particularly relates to a radar fast time domain signal design method which is suitable for multi-system frequency spectrum coexistence under the condition of radar anti-interference or frequency spectrum resource shortage in a narrow-band interference environment.
Background
Due to the limited electromagnetic spectrum resources and the rapid development of electromagnetic space applications, the spectrum resources are increasingly tense, and the problem of spectrum compatibility is increasingly prominent. The frequency spectrums of radar in modern battlefield environment and wireless applications such as timely wireless communication, remote sensing and navigation are overlapped and interleaved. The frequency spectrum overlapping causes mutual interference among applications, and simultaneously, the radar detection performance is seriously influenced, so that the problem of frequency spectrum compatibility between the radar and the applications is very important to solve, and the requirement of a radar system on the frequency spectrum utilization effectiveness of a transmitted waveform is increased day by day. The power spectrum information can be obtained through electromagnetic environment sensing, and further the influence of mutual interference and hostile interference of radar signals and civil signals is prevented through design of waveforms.
Dynamic spectrum estimation information is obtained through an electromagnetic environment sensing process, and a phase sequence of a phase coding waveform is designed in an auxiliary mode, so that power spectral density distribution of the waveform is adjusted, and the method is an effective method for solving the problem of frequency spectrum compatibility. In order to meet the practical application, the radar emission signal generally needs to satisfy some constraints. Specifically, to fully utilize the transmit power of the radar transmitter, the designed signal satisfies an energy constraint and a peak-to-average ratio (PAR) constraint. Assuming that the waveform to be designed has a very low power spectral density over some frequency band at the normalized frequency, the spectrum of the designed waveform is brought close to the desired template by minimizing the covariance of the spectrum of the designed signal and the designed template. Documents "p.ge, g.cui, s.m.karbasi, l.kong, and j.yang," a template fixing for coherent unidentive uniform sequence design, "Signal Processing, vol.128, pp.360-368, nov.2016" use the principle of iterative decrement of tolerance to make the power spectrum of the design waveform and the autocorrelation function gradually iteratively approximate to a template in the algorithm, thereby realizing the requirements of spectrum compatibility and target detection performance. However, this approach has limited optimization performance, and employs a constant modulus constraint, not a PAR constraint.
Disclosure of Invention
Aiming at the problem of spectrum coexistence in a narrow-band interference environment, the invention provides a method for designing a spectrum nulling signal based on template matching by considering PAR constraint and energy and minimizing covariance of a spectrum of a design signal and a design template on the assumption of target narrow-band interference resistance, such as other communication systems. Firstly, establishing a template according to a frequency spectrum environment, and deducing a target function; then, an optimization problem is constructed, and finally the optimization problem is solved.
The technical scheme of the invention is as follows: a frequency spectrum zero setting signal design method based on template matching comprises the following steps:
step 1, establishing a problem model;
consider the transmit waveform s ═ s (1), s (2), …, s (n)] T Is a fast time signal of dimension Nx 1 T Representing a transpose; the pass band and stop band of the frequency spectrum are defined as omega respectively pass And Ω stop And satisfy omega pass Ω stop 0,1, …, N-1 }; s (n) an nth code word representing a phase encoded waveform, the discrete Fourier transform of the signal s being y, f i The ith lattice point which is the normalized frequency; assuming that the desired energy spectral density template p (i) is
Figure BDA0002019591930000021
Wherein: ζ represents the expected amplitude of the stop band, and in order to make the ESD of the signal close to the expected ESD template, an objective function is defined as
Figure BDA0002019591930000022
Wherein,
Figure BDA0002019591930000023
representing a frequency f i A time Fourier transform vector, w (i) ≧ 0, i ═ 0, …, N-1 is the weight to the ith frequency bin, and α is the matching scale factor of expected ESD and design ESD energy; | · | represents modulo;
furthermore, the transmit signal s satisfies an energy constraint and a peak-to-average ratio (PAR) constraint, i.e.
s H s=N
Figure BDA0002019591930000024
Gamma represents the amplitude constraint on the waveform and therefore the optimization problem of the constraint
Figure BDA0002019591930000025
Step 2: solving the problem by adopting a sequence iteration four-time optimization algorithm;
step 2.1:
let α be the ratio of the design ESD and the expected ESD energy, then α is converted to α ═ s H Cs; wherein C isIs a hermitian matrix; build a satisfaction
Figure BDA0002019591930000026
Her-rice matrix y(s), her
h(α,s)=s H Υ(s)s
Due to the fact that
Figure BDA0002019591930000027
Y(s) is thus a semi-positive definite matrix, with no non-negative characteristic values;
Figure BDA0002019591930000028
equivalence translates into the following optimization problem:
Figure BDA0002019591930000031
step 2.2:
in the form of sequence iteration
Figure BDA0002019591930000032
Is converted into
Figure BDA0002019591930000033
Wherein s is (t) Expressing the optimized variable obtained by the t iteration, wherein I represents a unit array; will be provided with
Figure BDA0002019591930000034
Is further converted into
Figure BDA0002019591930000035
The solution to the problem is
s (t+1) =Q(s (t) )
Wherein Q (·) represents solving
Figure BDA0002019591930000036
A function of the problem solution;
and step 3: an acceleration algorithm;
accelerating by adopting an EM algorithm during each iteration;
first solve for s a =Q(s (t) ),s b =Q(s a ) (ii) a Then solving for r ═ s a -s (t) ,u=s b -s a -r,α=-||r||/||u||,s (t+1) =Q(s (t) -2αr+α 2 u),s a Represents when s (t) When it is an initial value
Figure BDA0002019591930000037
Solution of the problem, s b Represents when s a When it is an initial value
Figure BDA0002019591930000038
Solution of the problem, r denotes the two previous and subsequent iterations s a And s (t) U represents the difference between two successive iteration differences r; when s is (t+1)H [λI-Υ(s (t) )]s (t) <s (t)H [λI-Υ(s (t) )]s (t) Let α be (α -1)/2, s (t+1) =Q(s (t) -2αr+α 2 u), when α is-1, exit iteration,
Figure BDA0002019591930000039
representing a real part; when | | | s (t+1) -s (t) When | | < epsilon or a preset iteration number or preset iteration time is reached, exiting the iteration, wherein epsilon is a preset threshold value; at this time s (t+1) The spectrum nulling signal optimized for the present invention.
Compared with the prior art, the invention has the following advantages:
aiming at the problem of template matching and fitting, the method has higher descending speed and convergence speed, better fitting effect with the template and better optimization effect, and in addition, compared with other template algorithms, the algorithm used by the method has lower calculation complexity and improves the algorithm efficiency.
Drawings
FIG. 1 is a flow chart of a sequence iteration four-time optimization algorithm;
FIG. 2 is a graph comparing the variation of the average power spectrum of the stop band with the iteration number obtained by the optimization of the algorithm and the template matching (TFA) algorithm
FIG. 3 is a power spectrum diagram of the sequence obtained by the algorithm of the present invention and the TFA algorithm under different PAR constraints.
Detailed Description
The specific implementation steps of the invention are described as follows:
step 1, establishing a problem model;
Consider the transmit waveform s ═ s (1), s (2), …, s (n)] T Is a fast time signal of Nx 1 dimension, and the passband and stopband of the frequency spectrum are defined as omega respectively pass And Ω stop And satisfy Ω pass ∪Ω stop 0,1, …, N-1. The Discrete Fourier Transform (DFT) of the signal s is
Figure BDA0002019591930000041
Wherein,
Figure BDA0002019591930000042
(·) T 、(·) H respectively representing transpose and conjugate transpose, f i Is the ith lattice point of the normalized frequency. Assume a desired Energy Spectral Density (ESD) template p (i) is
Figure BDA0002019591930000043
To approximate the ESD of a signal to a desired ESD template, an objective function is defined as
Figure BDA0002019591930000044
Where w (i) ≧ 0, i ═ 0, …, and N-1 are the weights for the ith frequency bin, and α is the matching scale factor for the expected ESD and design ESD energies. | · | represents modulo.
Furthermore, the transmit signal s satisfies an energy constraint and a peak-to-average ratio (PAR) constraint, i.e.
s H s=N
Figure BDA0002019591930000045
Optimization problem of the constraints thus
Figure BDA0002019591930000046
Step 2: solving the problem by adopting a sequence iteration four-time optimization algorithm;
step 2.1:
let α be the ratio of the design ESD and the desired ESD energy:
Figure BDA0002019591930000051
wherein,
Figure BDA0002019591930000052
is a hermitian matrix. Then h (. alpha., s) can be changed to
Figure BDA0002019591930000053
Wherein,
Figure BDA0002019591930000054
D i i-0, …, N-1, y(s) are all hermite matrices. Then
Figure BDA0002019591930000055
Due to the fact that
Figure BDA0002019591930000056
Thus γ(s) is a semi-positive definite matrix with no non-negative eigenvalues.
Figure BDA0002019591930000057
The method can equivalently convert into the following optimization problems:
Figure BDA0002019591930000058
wherein
Figure BDA0002019591930000059
Step 2.2:
in the form of sequence iteration
Figure BDA00020195919300000510
Is converted into
Figure BDA00020195919300000511
Wherein s is (t) Representing an optimized variable obtained by the t iteration;
Figure BDA0002019591930000061
can be further converted into
Figure BDA0002019591930000062
The solution to the problem is
s (t+1) =Q(s (t) )
Wherein Q (-) represents the solution s (t+1) As a function of (c). In particular, the method of manufacturing a semiconductor device,
Figure BDA0002019591930000063
wherein s is (t+1) (n) representing the optimised variable s from the t +1 th iterationThe nth element.
Figure BDA0002019591930000064
arg (a) denotes the angle of vector a. v. of (t) Can be expressed as
v (t) =(λI N -Υ(s (t) ))s (t)
Let us assume v (t) (1)≥v (t) (2)≥…≥v (t) (N),v (t) The number of elements other than 0 in (1) is z. When z is gamma 2 When the content is less than or equal to N,
Figure BDA0002019591930000065
when z is gamma 2 When the content is more than or equal to N,
|s (t+1) (n)|=min{δ|v (t) (n)|,γ}
wherein,
Figure BDA0002019591930000066
δ can be solved by a dichotomy.
Step 2.3:
further, let
Figure BDA0002019591930000067
Accelerating by adopting an EM algorithm in each iteration, specifically, firstly solving s a =Q(s (t) ),s b =Q(s a ) (ii) a Then solving for r ═ s a -s (t) ,u=s b -s a -r,α=-||r||/||u||,s (t+1) =Q(s (t) -2αr+α 2 u); when in use
Figure BDA0002019591930000071
Let α be (α -1)/2, s (t+1) =Q(s (t) -2αr+α 2 u), when α is-1, the iteration exits. When s is (t +1) And when the iteration condition is met, exiting the iteration.
The effects of the present invention can be further illustrated by the following simulations:
simulation scene: setting the code length N of fast time waveform as 200, the initial sequence selects random phase code sequence and normalized frequency spectrum stop band as [0.1,0.2 ]]∪[0.7,0.8]Let the stop band level ζ equal to-150 dB, when | | | s (t+1) -s (t) ||≤10 -9 The iteration is exited.
Simulation content:
simulation 1: aiming at the same spectrum coexistence problem, the same convergence condition is set, and the optimization efficiency of the algorithm and the TFA algorithm adopted by the invention is compared. Fig. 2 illustrates a variation curve of the average power spectrum of the stop band optimized by the algorithm of the present invention and other template matching algorithms along with the number of iterations, from which it can be seen that the algorithm of the present invention represents an obvious advantage in optimizing the level, specifically, the algorithm of the present invention can achieve-147.2 dB for 142 iterations of stop band average power spectrum when PAR is 1, and achieve-149.7 dB for 47 iterations of stop band average power spectrum when PAR is 4; and the TFA algorithm reaches-43.41 dB in stopband average power spectrum at PAR 1 for 3000 iterations. Therefore, by means of the algorithm, the invention can realize the energy zero setting of the specific frequency band of the power spectrum, and is beneficial to the coexistence of the frequency spectrum under the complex electromagnetic environment.
Simulation 2: in order to analyze the robustness of the method, based on the simulation parameters, the power spectrum fitting performance of the algorithm and the TFA algorithm under different PAR constraints is compared.
Fig. 3 illustrates the power spectral densities of different sequences under different PAR constraints, and it can be seen that all three sequences have power spectral nulls at [0.1,0.2] < 0.7,0.8], where the sequence optimized by the algorithm of the present invention when PAR ═ 4 is closest to the template, and then the sequence optimized by the algorithm of the present invention when PAR ═ 1 is next, and the spectrum fitting effect of TFA is the worst.
In summary, the sequence quartic optimization design method provided by the invention can design the spectrum coexistence sequence aiming at the complex electromagnetic crowding scene, effectively resist the interference of other electromagnetic systems in the space, and enable the designed sequence to have better spectrum compatibility compared with the non-electromagnetic coexistence sequence.

Claims (1)

1. A frequency spectrum zero setting signal design method based on template matching comprises the following steps:
step 1, establishing a problem model;
consider the transmit waveform s ═ s (1), s (2), …, s (n)] T Is a fast time signal of dimension Nx 1 T Representing a transpose; the pass band and stop band of the frequency spectrum are defined as omega respectively pass And Ω stop And satisfy omega pass ∪Ω stop 0,1, …, N-1 }; s (n) an nth code word representing a phase encoded waveform, the discrete Fourier transform of the signal s being y, f i The ith lattice point which is the normalized frequency; assuming that the desired energy spectral density template p (i) is
Figure FDA0002019591920000011
Wherein: ζ represents the expected amplitude of the stop band, and in order to make the ESD of the signal close to the expected ESD template, an objective function is defined as
Figure FDA0002019591920000012
Wherein,
Figure FDA0002019591920000013
representing a frequency f i A time Fourier transform vector, w (i) ≧ 0, i ═ 0, …, N-1 is the weight to the ith frequency bin, and α is the matching scale factor of expected ESD and design ESD energy; | · | represents modulo;
furthermore, the transmit signal s satisfies an energy constraint and a peak-to-average ratio (PAR) constraint, i.e.
s H s=N
Figure FDA0002019591920000014
Gamma represents the amplitude constraint on the waveform and therefore the optimization problem of the constraint
Figure FDA0002019591920000015
Step 2: solving the problem by adopting a sequence iteration four-time optimization algorithm;
step 2.1:
let α be the ratio of the design ESD and the expected ESD energy, then α is converted to α ═ s H Cs; wherein C is a hermitian matrix; build a satisfaction
Figure FDA0002019591920000016
Her-rice matrix y(s), her
h(α,s)=s H Υ(s)s
Due to the fact that
Figure FDA0002019591920000021
Y(s) is thus a semi-positive definite matrix, with no non-negative characteristic values;
Figure FDA0002019591920000022
equivalence translates into the following optimization problem:
Figure FDA0002019591920000023
step 2.2:
in the form of sequence iteration
Figure FDA0002019591920000024
Is converted into
Figure FDA0002019591920000025
Wherein s is (t) Expressing the optimized variable obtained by the t iteration, wherein I represents a unit array; will be provided with
Figure FDA0002019591920000026
Is further converted into
Figure FDA0002019591920000027
The solution to the problem is
s (t+1) =Q(s (t) )
Wherein Q (·) represents solving
Figure FDA0002019591920000028
A function of the problem solution;
And 3, step 3: an acceleration algorithm;
accelerating by adopting an EM algorithm during each iteration;
first solve for s a =Q(s (t) ),s b =Q(s a ) (ii) a Then solving for r ═ s a -s (t) ,u=s b -s a -r,α=-||r||/||u||,s (t+1) =Q(s (t) -2αr+α 2 u),s a Represents when s (t) When it is an initial value
Figure FDA0002019591920000029
Solution of the problem, s b Represents when s a When it is an initial value
Figure FDA00020195919200000210
Solution of the problem, r denotes the two previous and subsequent iterations s a And s (t) U represents the difference between two successive iteration differences r; when s is (t+1)H [λI-Υ(s (t) )]s (t) <s (t)H [λI-Υ(s (t) )]s (t) Let α be (α -1)/2, s (t+1) =Q(s (t) -2αr+α 2 u), when α is-1, exit iteration,
Figure FDA00020195919200000211
representing a real part; when | | | s (t+1) -s (t) | | < epsilon orWhen the preset iteration times or the preset iteration time is reached, the iteration is stopped, and epsilon is a preset threshold value; at this time s (t+1) The signal is nulled for an optimized spectrum.
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