CN104535959A - Signal frequency and DOA joint measurement method and device under spatial-temporal sub-nyquist sampling - Google Patents

Signal frequency and DOA joint measurement method and device under spatial-temporal sub-nyquist sampling Download PDF

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CN104535959A
CN104535959A CN201410737350.6A CN201410737350A CN104535959A CN 104535959 A CN104535959 A CN 104535959A CN 201410737350 A CN201410737350 A CN 201410737350A CN 104535959 A CN104535959 A CN 104535959A
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signal
frequency
array element
sensor array
doa
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黄翔东
冼弘宇
闫子阳
景森学
朱展宏
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Tianjin University
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Tianjin 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
    • G01S3/00Direction-finders for determining the direction from which infrasonic, sonic, ultrasonic, or electromagnetic waves, or particle emission, not having a directional significance, are being received
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R23/00Arrangements for measuring frequencies; Arrangements for analysing frequency spectra
    • G01R23/02Arrangements for measuring frequency, e.g. pulse repetition rate; Arrangements for measuring period of current or voltage

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  • General Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Radar, Positioning & Navigation (AREA)
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Abstract

The invention discloses a signal frequency and DOA joint measurement method and device under spatial-temporal sub-nyquist sampling. The method comprises the steps that DFT is carried out on L paths of signal samples, frequency and phase position correction is carried out on each path of DFT spectrum peak through a Candan interpolation estimator, and L pairs of normalization frequencies and phase position estimation values are obtained; by adoption of a closed type CRT algorithm, a signal frequency value is obtained through the L pairs of normalization frequencies; a receiving signal phase position difference estimated value of sensor array elements 1 and other array elements is obtained, then a phase position remainder is formed, and finally the spatial signal incidence angle is calculated. The device comprises the sensor array elements, A/D samplers, a DSP, an output driver and a display circuit of the output driver, wherein the spatial far-field narrowband signals reach the sensor array elements by a certain incidence angle theta, and array receiving signals are obtained; the A/D samplers on the sensor array elements sample the signals and input the obtained sample sequences into the DSP in parallel, frequency estimation and DOA estimation of the incident signals are obtained after processing by an internal algorithm of the DSP, and finally the estimation results are displayed through the output driver and the display circuit of the output driver.

Description

Signal frequency and DOA union measuring method and device under space-time lack sampling
Technical field
The present invention relates to digital processing field, particularly relate to one and utilize sensor array to carry out time domain, space lack sampling to space incident signal, by carrying out method and the device of high-precision frequency and DOA combined measurement to sample analysis.
Background technology
Array parameter is estimated as the important component part of Array Signal Processing, and rapidly, its application has related to the numerous areas such as sonar, radar, communication and biomedicine for very active in recent years and development.Wherein, the Frequency Estimation of space incident signal and direction of arrival (Direction of Arrival, DOA) estimate it is hot research content.And more go deep into extensive along with what apply, the requirement of people to parameter estimation is more and more higher, such as require that arithmetic accuracy is higher, fault-tolerance and robustness stronger, calculate simpler, hardware layout cost is lower, these require the development also having promoted array parameter estimation technique.Wherein, how under the condition of space-time lack sampling, the attention in obtaining academia in recent years is accurately measured to signal frequency and DOA parameter.
Find through literature survey, in classical way, such prerequisite is needed to the frequency of space incident signal, the isoparametric measurement of DOA: all will meet nyquist sampling condition to signal in the sampling of time domain and spatial domain, namely require that sampling rate is greater than the twice of incoming signal frequency, and the arrangement pitch of adjacent sensors array element is not more than the half-wavelength of incoming signal.But above condition is difficult to meet in some actual environments.Such as, document [1] is pointed out, the operating frequency range of military airborne radar investigation receiver is 2-18GHz, and it is unpractical for directly carrying out time domain nyquist sampling to the signal be distributed in broadband like this.Although there is the analog to digital converter of sampling rate at the GHz order of magnitude, its price is very expensive, and is also difficult to reach so large data throughput with the back-end digital processor of system support.Depend merely on its effect of data acquisition performance improving hardware device very limited, only propose new spectrum analysis theory method in signal transacting field and could fundamentally solve this kind of problem.Equally, the layout of so wide working band to sensor array it is also proposed rigors.At classics without in fuzzy DOA measuring method, require that the spacing of adjacent sensors array element on array is not more than the half-wavelength of incoming signal.When signal wavelength is less (half-wavelength as corresponding in 18GHz signal is 0.83cm), the difficulty that so short spacing not only can cause sensor array element installing, also will certainly strengthen the mutual coupling of low frequency signal between different sensors array element.Therefore, widen sensor array element distance, realize the sparse layout of array, under the condition that space lack sampling is carried out to signal, realize high precision DOA measure significant in actual applications.
But space-time lack sampling can cause frequency, the phase ambiguity of signal, for this problem, ancient Chinese remainder theorem (Chinese Remainder Theorem, CRT) [2] can be introduced this field and is solved.From CRT, if a certain positive integer is less than the lowest common multiple of one group of relatively prime between two integer, then this positive integer uniquely can be determined by the remainder after its modulo operation.But CRT is very responsive to Residue error, if remainder exists minimum error, larger reconstructed error can be caused.At radio interference location (Radio Interferometric Positioning, RIPS [3]), inevitably there is noise in the system such as radar [4], this must bring Residue error to CRT, and therefore the range of application of traditional C RT is very limited.Document [5] proposes a kind of CRT algorithm of robust, and be no more than the condition of certain limit at Residue error under, this algorithm can more accurately reconstruct unknown integer, but this algorithm just can must realize by two-dimensional search, and operand is large.Document improves the algorithm of document [5] in [6,7], and by two-dimensional search being reduced to linear search thus reducing operand, but when the number of institute's delivery is more or numerical value is larger, its search complexity is still very high.For fundamentally avoiding heavy search procedure, document [8] proposes a kind of CRT enclosed method for solving of robust, greatly reduces operand, is conducive to real-time implementation in engineering, thus for the invention provides suitable theoretical tool.
Have benefited from the improvement to classical CRT and optimization [5-8], at signal frequency estimation, DOA, CRT estimates that fields such as [9] obtains application in recent years.In signal frequency estimation, if document [10-12] is by carrying out the sampling of multi-path low speed rate to signal, achieve the Accurate Reconstruction of signal frequency under time domain lack sampling in conjunction with CRT theorem.But in these methods, CRT remainder values is directly obtained by DFT spectrum peak search, when the leakage of existence spectrum can bring error to remainder thus affect estimated accuracy.DFT counts and is set to sampling rate value corresponding to each road (frequency resolution of corresponding DFT is 1Hz) by document [10-12], and supposition measured signal frequency values is integer (being namely the integral multiple of DFT frequency resolution just), thus avoid the observation Residue error brought because spectrum is leaked.Obviously integer-valued hypothesis is done to signal frequency and limit its range of application, and due to the value (usually larger) that is set to sampling rate and bring larger operand of counting by DFT; In addition, owing to using the CRT method based on search in document [10-12], when measured signal frequency is higher, the large and length consuming time of computational complexity, is unfavorable for real-time measurement.In DOA estimation, document [9] realizes the sparse layout of array element by the form extracting the grouping of sensor array element from imaginary even linear array, utilizes the phase differential structure remainder of sensor array tuple Received signal strength, carrys out the incident angle of estimated signal in conjunction with CRT.But, do not provide concrete sampling plan and the measuring method of signal phase in document [9]; Document [13] proposes CRT to be applied to signal frequency under space-time lack sampling and DOA Combined estimator, the method first utilizes separately certain sensor array element to carry out a point frequency multi-channel sampling to carry out estimated signal frequency, and then utilizes array grouping multiple repairing weld to estimate DOA.Because its sampling of the method in document [13] and parameter estimation procedure complete stage by stage, consuming time longer and sample utilization factor is low, its actual application value is restricted.At present, under space-time lack sampling, real-time combined measurement is carried out to the frequency of signal and DOA, still belong to technological gap.
Summary of the invention
The invention provides signal frequency and DOA union measuring method and device under a kind of space-time lack sampling, present invention achieves and the high precision of signal frequency to be estimated under time domain lack sampling and DOA high precision under spatial domain lack sampling is estimated, described below:
Signal frequency and DOA union measuring method under a kind of space-time lack sampling, described measuring method comprises the following steps:
Arrange the non-uniform linear arrays containing L sensor array element, with sensor array element 1 for reference array element, the spacing of definition sensor array element i and sensor array element 1 is d i, 1;
Interval T at one time 0in, L sensor array element is respectively with sampling rate F 1~ F lparallel lack sampling is done to space incident signal, wherein, F 1~ F lthere is positive common divisor M f;
DFT is done to L road sample of signal, with Candan interpolation estimator, frequency, phase correction is done to each road DFT spectrum peak, obtain L to normalized frequency and phase estimation value;
Adopt enclosed CRT algorithm, by L, signal frequency value is obtained to normalized frequency
Obtain sensor array element 1 estimated value poor with the phase of received signal of other array element, and form phase place remainder further, calculate spacing wave incident angle.
Described employing enclosed CRT algorithm, obtains signal frequency value by L to normalized frequency step be specially:
? as frequency remainder, using the value of each sensor array element sampling rate as the mould needed for CRT, remainder group prime number group Γ 1... Γ i... Γ land M fsubstitute into enclosed CRT and try to achieve signal frequency value
The described phase of received signal difference estimated value obtaining sensor array element 1 and other array element, and form phase place remainder further, calculate spacing wave incident angle and be specially:
Obtain sensor array element 1 estimated value poor with the phase of received signal of other array element and form phase place remainder further; By phase place remainder group, prime number group η 1~ η l-1and M θthe CRT substituting into closed form reconstructs nonnegative constant N 0, and then by N 0calculate spacing wave incident angle
Under described space-time lack sampling, signal frequency and DOA combined measurement device comprise: sensor array element, A/D sampling thief, DSP and output driving and display circuit thereof,
Space far-field narrow band signal s (t) arrives each sensor array element with a certain incidence angle θ, obtains array received signal; A/D sampling thief in each sensor array element is respectively with F 1, F 2..., F lspeed signal parallel is sampled, be input to DSP device by parallel for the sample sequence obtained, through the internal algorithm process of DSP, the Frequency Estimation and the DOA that obtain incoming signal estimate, finally drive by output and display circuit display estimated result.
Signal frequency under the space-time lack sampling that the present invention proposes and DOA union measuring method, if be applied to Practical Project field, can produce following beneficial effect:
The first, under achieving time domain lack sampling, the high precision of signal frequency is estimated;
In traditional frequency measurement method, require that sampling rate is higher than the twice of measured signal frequency, otherwise will frequency ambiguity be caused thus correct frequency estimation cannot be obtained.And the present invention adopts the scheme of multi-path low speed rate time domain lack sampling, achieve the measurement to high-frequency signal, considerably increase the measurement range of frequency.To the low sampling rate F in L road 1~ F l, the signal frequency range utilizing the present invention accurately to measure is (0, f max], wherein f maxequal F 1~ F llowest common multiple.
Such as, in experiment, the sampling rate of sensor array element is respectively F 1=52400Hz, F 2=54800Hz, F 3=55600Hz, with the measurement range of classical DFT method then frequency be (0,27800], according to the present invention then maximum detection frequency be f max=997853200Hz, improves 4 orders of magnitude than classic method.
The second, the DOA high precision achieved under spatial domain lack sampling is estimated, and is achieved the flexible arrangement of sensor array element;
In tradition without in fuzzy DOA measuring method, require that the spacing of adjacent sensors array element is less than the half-wavelength of incoming signal, so not only can cause the difficulty that sensor array element is being installed, also will certainly strengthen the mutual coupling of low frequency signal between different sensors array element, reduce the precision of each estimating DOA forsingals.The present invention proposes the sparse arrangement of concrete array, and can according to actual conditions flexible configuration sensor array element distance.
Such as, the incoming signal wavelength supposed in experiment is λ 0=0.3426m, if according to tradition without fuzzy DOA estimation method, then adjacent sensors array element distance d need meet d < λ 0/ 2=0.1713m, and according to the array that the present invention arranges, the minimum spacing of its adjacent sensors array element is 0.3m, breaches the restriction of half-wavelength.And by changing the value of systematic parameter, the flexible configuration of sensor array element distance can be realized.
Three, make full use of array sample, improve efficiency and the real-time of parametric joint measurement.
Its sampling of the parametric joint estimation technique of document [13] and measuring process are divided into two stages, namely first carry out frequeney division multiple (FDM) sampling by certain sensor array element independent and carry out measuring-signal frequency, and then utilize sensor array parallel sampling to carry out measuring-signal DOA, longer being unfavorable for consuming time of sampling measures in real time, and the data of two sample phase can not be multiplexing, sample utilization factor is low.The present invention directly utilizes sensor array to carry out parallel duplex sampling, then must obtain frequency and the DOA measured value of signal, being more conducive to engineer applied by analyzing a few sample collected.
Accompanying drawing explanation
Fig. 1 is frequency and the DOA combined measurement process flow diagram of signal under space-time lack sampling;
Fig. 2 is that sensor array element arranges schematic diagram;
Fig. 3 (a) is signal to noise ratio (S/N ratio) and signal frequency detection probability relation curve;
Fig. 3 (b) estimates square error relation curve for signal to noise ratio (S/N ratio) and signal frequency;
Fig. 4 is signal to noise ratio (S/N ratio) and signal DOA estimation property relationship curve;
Fig. 5 is hardware implementation figure of the present invention;
Fig. 6 is DSP internal processes flow graph.
Embodiment
For making the object, technical solutions and advantages of the present invention clearly, below embodiment of the present invention is described further in detail.
The present invention is in conjunction with the enclosed CRT algorithm of robust [8]frequency and the DOA combined measurement of signal under space-time lack sampling is carried out with DFT spectrum correction method.Owing to introducing enclosed CRT algorithm, avoid the search in calculating process thus to decrease computing consuming time.Compared with the method for document [13], present invention eliminates the step of first carrying out multiple repairing weld frequency measurement by a certain separated sensor array element, consuming time shorter and sample utilization factor is higher.Different from document [10-12], DFT when processing sample of signal in the present invention counts and elects number of samples as but not sampling rate value, greatly reduces calculated amount and the requirement to hardware.Meanwhile, be the Residue error that " fence effect " that overcome DFT causes, the present invention introduces Candan interpolation estimator [14,15]frequency spectrum and phase correction are carried out to DFT result, improves Parameter Estimation Precision.Therefore, the present invention has higher practical value and application prospect widely.
101: arrange the non-uniform linear arrays containing L sensor array element, with sensor array element 1 for reference array element, the spacing of definition sensor array element i and sensor array element 1 is d i, 1and meet d i, 1=K η 1η 2... η l-1/ η i-1, i=2 ..., L, wherein η 1~ η l-1for array relatively prime between two, K be according to actual conditions setting constant and be required to meet 0 < K < λ minminfor system maximum detection frequency f maxcorresponding signal wavelength).
To comprise the linear array of 3 sensor array elements, make K=0.9 λ min, η 1=3, η 2=2, then d 2,1=K η 2, d 3,1=K η 1=2.7 λ min.Obviously, apart nearest array element is sensor 2 and 3 in the array, its spacing d 3,2=0.9 λ min> λ min/ 2, breach in classic method and require that array element distance is not more than the restriction of signal half-wavelength.In actual applications, by changing prime number group η 1~ η l-1and the value of K can realize the flexible configuration of sensor array element distance.
102: interval T at one time 0in, L sensor array element is respectively with sampling rate F 1~ F lparallel lack sampling is done to space incident signal and (requires F 1~ F lthere is positive common divisor M f, and F 1~ F ldivided by M fafter relatively prime between two);
In radar, sonar etc. much application, incoming signal meets as drag:
s(t)=Aexp(j2πf 0t)+ω(t) (1)
Wherein, A is non-zero constant, and ω (t) is additive noise, f 0for incoming signal frequency.The array received comprising L sensor array element to signal be:
y(t)=a·s(t) (2)
Wherein, a is direction vector, is jointly determined by array structure and incoming signal.The matrix form of formula (2) is
y 1 ( t ) . . . y i ( t ) . . . y L ( t ) = 1 . . . e - j 2 &pi; d i , 1 sin &theta; / &lambda; . . . e - j 2 &pi; d L , 1 sin &theta; / &lambda; s ( t ) - - - ( 3 )
Wherein θ is the space incident angle of signal, and λ is incoming signal wavelength, y ifor the signal that sensor array element i receives.Interval T at one time 0interior all the sensors array element is sampled to space incident signal, supposes that the sampling rate of sensor array element i is F i, i=1 ... L, then the sample of signal that sensor array element i obtains is:
y i ( n ) = y i ( t ) | t = n / F i = A e - j 2 &pi; d i , 1 sin &theta; / &lambda; [ exp ( j 2 &pi; f 0 n / F i ) + &omega; ( n i ) ] , n = 1 , . . . , N i - - - ( 4 )
Wherein, N ifor the sample number that sensor array element i gathers.
103: DFT is done to L road sample of signal, with Candan interpolation estimator, frequency, phase correction are done to each road DFT spectrum peak, obtain L to normalized frequency and phase estimation value
The amplitude A=2 of hypothesis space incoming signal s (t), frequency f 0=6 × 10 8hz.Appoint and get a certain sensor array element i, suppose that the signal first phase arriving this sensor array element is zero, if sensor array element sampling rate F i=54321Hz, then frequency remainder should be f 0modF i=24555 (remainder operation is got in mod representative).If the sample number N that this sensor array element gathers i=64, sample is counted equal F respectively iand N idFT (for F ithe DFT of=54321 needs to carry out zero padding to sample sequence), the position of spectrum peak is obtained by spectrum peak search frequency remainder (the F as shown in table 1 of signal phase estimated value and correspondence ithe frequency remainder of some DFT n ithe frequency remainder of some DFT
Table 1 DFT spectrum peak position and phase information
By the DFT analysis of spectrum result that in comparison sheet 1, two kinds are counted different, find the contradiction existed between calculated amount and analysis precision.For the large (F that counts i=54321 points) DFT, analysis precision is high, and frequency remainder and phase value error are almost 0, but computing length consuming time; And for the little (N that counts i=64 points) DFT, computing is consuming time few, but analysis precision is poor, frequency remainder exist | the deviation of 24614-24555|=59Hz, phase estimation deviation reach-12.3592 degree.
Because CRT is responsive to Residue error, the DFT spectrum analysis errors under therefore needing introducing spectrum alignment technique to reduce small point situation, solves the contradiction between calculated amount and analysis precision.The present invention adopts Candan interpolation estimator to correct each road frequency, the frequency deviation value that recycling frequency correction obtains phase place is corrected.Idiographic flow is as follows
Step1 counts to the data sample that sensor array element i gathers and equals sample number N idFT, obtain amplitude spectrum Y i(k i) and phase spectrum
Step2 utilizes place's peak value spectrum with its about two other spectral lines to frequency deviation value do to estimate by following formula, wherein real represents real part.
&delta; ^ i = tan ( &pi; / N i ) &pi; / N i &CenterDot; teal { Y i ( k i * ) - Y i ( k i * + 1 ) 2 Y i ( k i * ) - Y i ( k i * - 1 ) - Y i ( k i * + 1 ) } - - - ( 5 )
Step3 is according to the frequency deviation value obtained carry out frequency and phase correction, the normalized frequency after correction and phase estimation be respectively:
f ^ i = ( k i * + &delta; ^ i ) / N i - - - ( 6 )
Step4 is through above correction process, and can calculate the CRT remainder estimated value corresponding with Frequency Estimation is
r ^ i = ( k i * + &delta; ^ i ) &CenterDot; F i / N i - - - ( 8 )
Learnt by emulation, under identical condition N ithe frequency remainder that some DFT obtains after overcorrect is 24555, and phase correcting value is 4.8298 × 10 -5degree, error is almost nil.
104: adopt the enclosed CRT algorithm that document [8] proposes, as frequency remainder, using the value of each sensor array element sampling rate as the mould needed for CRT, (L corresponding relatively prime integer is for Γ i=F i/ M f, i=1...L).Remainder group prime number group Γ 1... Γ i... Γ land M fsubstitute into enclosed CRT and try to achieve signal frequency value algorithm idiographic flow is as follows:
Step1 is from given frequency remainder calculating parameter wherein
q ^ i , 1 = [ r ^ i - r ^ 1 M f ] , 2 &le; i &le; L - - - ( 9 )
Step2 calculates mould is except Γ iremainder:
&xi; ^ i , 1 = q ^ i , 1 &Gamma; &OverBar; i , 1 mod &Gamma; i , 2 &le; i &le; L - - - ( 10 )
Wherein, Γ 1about Γ imould inverse.
Step3 calculates fuzzy integer
n ^ 1 = &Sigma; i = 2 L &xi; ^ i , 1 b i , 1 &gamma; 1 &Gamma; i mod &gamma; 1 - - - ( 11 )
Wherein, b i, 1be about Γ imould inverse, and γ i=Γ/Γ i, Γ is Γ 1~ Γ lproduct.
Step4 calculates other fuzzy integer
n ^ i = n ^ 1 &Gamma; 1 - q ^ i , 1 &Gamma; i - - - ( 12 )
Step5 calculates each road frequency estimation 1≤i≤L, gets its mean value as Frequency Estimation namely
f ^ 0 i = n ^ i M f &Gamma; i + r ^ i , 1 &le; i &le; L - - - ( 13 )
f ^ 0 = 1 L &Sigma; i = 1 L f ^ 0 i - - - ( 14 )
From document [8], maximum detection frequency of the present invention is f max=lcm (F 1..., F l), wherein lcm represents lowest common multiple.
105: obtain sensor array element 1 estimated value poor with the phase of received signal of other array element and form phase place remainder further.By phase place remainder group, prime number group η 1~ η l-1and M θthe CRT substituting into closed form reconstructs nonnegative constant N 0, and then by N 0calculate spacing wave incident angle concrete steps are as follows:
Step1 gets any positive integer M θ, definition for the spacing of sensor array element i and sensor array element 1 and phase of received signal difference and then phase place remainder is constructed
Step2 is by prime number group η 1~ η l-1, phase place remainder group and M θsubstitute into enclosed CRT (its solution procedure is similar to Frequency Estimation process of the present invention, does not repeat) here and reconstruct nonnegative constant
Step3 by obtain signal wavelength estimated value (c is constant propagation velocity of electromagnetic wave), then calculates incident angle estimated value wherein parameter d 0=KM θη 1η 2... η l-1.
The principle of above DOA estimating step and optimum configurations is as follows:
When adjacent sensors array element distance is greater than a half of incoming signal wavelength X, the phase differential of corresponding Received signal strength its estimated value scope be [-π, π], it is fuzzy observed reading with 2 π, namely
Wherein n is unknown fuzzy integer, and ε is phase measurement error.If θ is the incident angle of spacing wave, λ is signal wavelength, and d is the spacing of adjacent sensors, then
Parameter d is multiplied by formula (16) both sides 0and carry out equation conversion,
Use N 0represent d 0sin θ/λ, obvious N 0be a nonnegative constant, CRT can be utilized reconstruct.Defined parameters d 0, sensor array element i and array element 1 spacing d i, 1with phase of received signal difference be
d 0=KM θη 1η 2...η L-1
d i,1=Kη 1...η i-2η i...η L-1(18)
Wushu (18) substitutes into, even d=d i, 1, n=n i, 1, then (17) are rewritten as
N 0 = d 0 sin &theta; &lambda; = n i - 1 M &theta; &eta; i - 1 + r ^ &theta; , i - 1 , i = 2 , . . . , L
(19)
Wherein ε i, 1for the measuring error of phase differential.Formula (19) meets the data model of CRT, by prime number group η 1~ η l-1, remainder group and parameter M θsubstitute into enclosed CRT to obtain reconstructing nonnegative constant then binding signal wavelength estimated value the incident angle estimated value of signal can be obtained
&theta; ^ = arcsin &lambda; ^ N ^ 0 d 0 - - - ( 20 )
By Chinese remainder theorem, nonnegative constant N 0need meet the following conditions
0 &le; N 0 = d 0 sin &theta; &lambda; < M &theta; &eta; 1 &eta; 2 . . . &eta; L - 1 - - - ( 21 )
By d 0=KM θη 1η 2... η lsubstitution formula (21), has
K < &lambda; sin &theta; - - - ( 22 )
Suppose λ minfor the signal wavelength that system maximum detection frequency is corresponding, for ensureing that the measurement range of incident angle meets θ ∈ [-pi/2, pi/2], in practical application, K being set to and being less than λ mina constant.In order to ensure parameter energy Accurate Reconstruction, CRT requires that Residue error is less than 1/4th of lowest common multiple, uses ε i, 1represent the phase measurement error of sensor array element i and array element 1,
M &theta; 4 > M &theta; &eta; i - 1 &epsiv; i , 1 2 &pi;
(23)
Namely &epsiv; i , 1 < &pi; 2 &eta; i - 1 , i = 2 , . . . , L
Obtain prime number group η thus 1~ η l-1the relation with DOA estimated accuracy of choosing.
Emulation experiment and result
According to Fig. 1 scheme, arrange the linear array comprising three sensor array elements.Sampling rate corresponding to each sensor array element is respectively F 1=52400Hz, F 2=54800Hz, F 3=55600Hz, then the common divisor M of each sensor array element sampling rate f=400, corresponding prime number group { Γ 1, Γ 2, Γ 3}={ 131,137,139}.
The signal frequency range that system can be surveyed is (0, f max], wherein f max=lcm (F 1..., F 3)=997853200Hz, corresponding signal wavelength lambda min=c 0/ f max=0.3006m.If K=0.3, meet K < λ mincondition.If η 1=3, η 2=2, then corresponding sensor array element distance d 2,1=K η 2=0.6m, d 3,1=K η 1=0.9m (obviously the spacing of the adjacent array element of this array is all greater than half-wavelength).If space incident signal amplitude A=2, signal frequency is for being in (0, f max] f in measurement range 0=875697821.6Hz (obvious each road sampling rate, much smaller than measured signal frequency, belongs to time domain lack sampling situation), the additive noise of sensor array element Received signal strength is the white Gaussian noise of zero-mean.Suppose the sampling time T of array 0=0.1s, then correspond to three sampling rate F within this period 1~ F 3interior number of samples is respectively N 1=5250, N 2=5480, N 3=5560, thus respectively N is done to the sample that three sensor array elements are collected 1, N 2, N 3the DFT of point, then utilizes Candan interpolation estimator to carry out spectrum and corrects, obtain frequency and phase place remainder.In DOA estimation procedure, setting parameter M θbe 3.
In order to verify parameter estimation performance of the present invention under space-time lack sampling, follow Fig. 1 scheme 5 steps, under different signal to noise ratio (S/N ratio), carry out 1000 Monte-carlo experiment, Fig. 3 (a), Fig. 3 (b), Fig. 4 give signal frequency when changing with signal to noise ratio (S/N ratio) and DOA estimated performance relation curve.
The frequency detecting probability of Fig. 3 (a) is as undefined: when frequency detecting relative error exceeds 0.1%, be then judged as detecting successfully, otherwise be judged as detecting unsuccessfully.Can find out from Fig. 3 (a), when signal to noise ratio (S/N ratio) is higher than threshold value-22dB, reach the detection probability of success of 100%.Can find out from Fig. 3 (b), when signal to noise ratio (S/N ratio) is higher than threshold value-22dB, the square error of its frequency estimation is tending towards 0.
Detect square error curve from the DOA of Fig. 4 can find out, when signal to noise ratio (S/N ratio) is higher than threshold value-22dB, its DOA estimates that square error can be controlled within 5 °.
See Fig. 5, under space-time lack sampling, signal frequency and DOA combined measurement device comprise: sensor array element, A/D sampling thief, DSP and output driving and display circuit thereof, space far-field narrow band signal s (t) arrives each sensor array element with a certain incidence angle θ, obtain array received signal y (t)=as (t), wherein a is array direction vector.A/D sampling thief in each sensor array element is respectively with F 1, F 2..., F lspeed signal parallel is sampled, will obtain that sample sequence is parallel is input to DSP (Digital Signal Processor, digital signal processor) device.Through the internal algorithm process of DSP, the Frequency Estimation and the DOA that obtain incoming signal estimate, finally drive by output and display circuit display estimated result.
Wherein, the DSP in Fig. 5 is core component, in whole estimation procedure, complete following function:
1, call core algorithm, complete the DFT process of each road sample of signal and correct the estimated value of frequency, phase place, the frequency and the DOA that complete spacing wave measure;
2, sampling rate F is adjusted in time according to actual needs 1, F 2..., F l, make it meet actual needs;
3, measurement result is exported to driving and display module.
Wherein, the principal element determining the complexity of Fig. 5 system, degree of accuracy and degree of stability is the kernel estimation algorithm that DSP internal program memory stores.The internal processes flow process of DSP device is as shown in Figure 6:
The flow process of Fig. 6 is divided into following step:
First according to actual requirement, the frequency range of guestimate incoming signal, and according to real needs setpoint frequency measurement range and each road sampling rate;
CPU primary controller reads sampled data from I/O port, enters internal RAM;
DC processing.Flip-flop in measured signal can reduce measuring accuracy, therefore needs to eliminate direct current impact;
By the most crucial part that the processing procedure of Fig. 1 carries out frequency, DOA measurement is DSP algorithm, by will frequency and the DOA estimated value of incoming signal be obtained after this algorithm process;
Judge whether measurement result meets engineering demand, if do not meet, then reset sampling rate and frequency measurement scope according to result and actual demand;
If the measurement result obtained meets the demands, then export driving or display device to by DSP output bus.
The embodiment of the present invention is to the model of each device except doing specified otherwise, and the model of other devices does not limit, as long as can complete the device of above-mentioned functions.
List of references
[1]Tsui J.Digital techniques for wideband receivers[M].SciTech Publishing,2004.
[2]Arazi B.A generalization of the Chinese remainder theorem[J].Pacific Journal of Mathematics,1977,70(2):289-96.
[3]Maróti M, P,Dóra S,et al.Radio interferometric geolocation[C].Proceedings of the Proceedings of the 3rd international conference on Embedded networked sensor systems,ACM,2005:1-12.
[4]Ruegg M,Meier E,Nuesch D.Capabilities of dual-frequency millimeter wave SAR with monopulse processing for ground moving target indication[J].Geoscience and Remote Sensing,IEEE Transactions on,2007,45(3):539-53.
[5]Xia X-G,Wang G.Phase unwrapping and a robust Chinese remainder theorem[J].IEEE Signal Processing Letters,2007,14(4):247.
[6]Li G,Xu J,Peng Y-N,et al.An efficient implementation of a robust phase-unwrapping algorithm[J].Signal Processing Letters,IEEE,2007,14(6):393-6.
[7]Xia X L X-G.A fast robust Chinese remainder theorem based phase unwrapping algorithm[J].Signal Processing,2008.
[8]Wang W,Xia X-G.A closed-form robust Chinese remainder theorem and its performance analysis[J].Signal Processing,IEEE Transactions on,2010,58(11):5655-66.
[9] Liang Hong, Zhang Qi, Yang Changsheng. the sane Chinese remainder theorem of broad sense and the application [J] in space undersampled signal DOA estimates thereof. Northwestern Polytechnical University's journal, 2010,3): 409-14.
[10]Xia X-G,Liu K.A generalized Chinese remainder theorem for residue sets with errors and its application in frequency determination from multiple sensors with low sampling rates[J].Signal Processing Letters,IEEE,2005,12(11):768-71.
[11]Li X,Liang H,Xia X-G.A robust Chinese remainder theorem with its applications in frequency estimation from undersampled waveforms[J].Signal Processing,IEEE Transactions on,2009,57(11):4314-22.
[12] Liang Hong, Zhang Qi, Yang Changsheng. the Chinese remainder theorem that broad sense is sane and the application [J] in lack sampling rate lower frequency is estimated thereof. electronics and information journal, 2010,32 (8): 1802-5.
[13] Liang Hong, Zhang Heng. multiple goal frequency and orientation joint estimate new method [J] under lack sampling time empty. Northwestern Polytechnical University's journal, 2012,30 (5): 694-8.
[14]Candan C.A method for fine resolution frequency estimation from three DFT samples[J].Signal Processing Letters,IEEE,2011,18(6):351-4.
[15]Candan C.Statistical Analysis and Improvement of Fine Resolution Frequency Estimation Method From Three DFT Samples[J].2013.
It will be appreciated by those skilled in the art that accompanying drawing is the schematic diagram of a preferred embodiment, the invention described above embodiment sequence number, just to describing, does not represent the quality of embodiment.
The foregoing is only preferred embodiment of the present invention, not in order to limit the present invention, within the spirit and principles in the present invention all, any amendment done, equivalent replacement, improvement etc., all should be included within protection scope of the present invention.

Claims (4)

1. signal frequency and a DOA union measuring method under space-time lack sampling, it is characterized in that, described measuring method comprises the following steps:
Arrange the linear nonuniform noise containing L sensor array element, with sensor array element 1 for reference array element, the spacing of definition sensor array element i and sensor array element 1 is d i, 1;
Interval T at one time 0in, L sensor array element is respectively with sampling rate F 1~ F lparallel lack sampling is done to space incident signal, wherein, F 1~ F lthere is positive common divisor M f;
DFT is done to L road sample of signal, with Candan interpolation estimator, frequency, phase correction is done to each road DFT spectrum peak, obtain L to normalized frequency and phase estimation value;
Adopt enclosed CRT algorithm, by L, signal frequency value is obtained to normalized frequency
Obtain sensor array element 1 and the phase of received signal difference estimated value of other array element, form phase place remainder further, finally calculate spacing wave incident angle.
2. signal frequency and DOA union measuring method under a kind of space-time lack sampling according to claim 1, is characterized in that, described employing enclosed CRT algorithm, obtains signal frequency value by L to normalized frequency step be specially:
? as frequency remainder, using the value of each sensor array element sampling rate as the mould needed for CRT, remainder group prime number group Γ 1Γ iΓ land M fsubstitute into enclosed CRT and try to achieve signal frequency value
3. signal frequency and DOA union measuring method under a kind of space-time lack sampling according to claim 1, it is characterized in that, the described phase of received signal difference estimated value obtaining sensor array element 1 and other array element, and form phase place remainder further, calculate spacing wave incident angle and be specially:
Obtain sensor array element 1 estimated value poor with the phase of received signal of other array element and form phase place remainder further; By phase place remainder group, prime number group η 1~ η l-1and parameter M θsubstitute into closed form CRT and reconstruct nonnegative constant N 0, and then by N 0calculate spacing wave incident angle
4. signal frequency and DOA union measuring method under a kind of space-time lack sampling according to claim 1, it is characterized in that, under described space-time lack sampling, signal frequency and DOA combined measurement device comprise: sensor array element, A/D sampling thief, DSP and output driving and display circuit thereof
Space far-field narrow band signal s (t) arrives each sensor array element with a certain incidence angle θ, obtains array received signal; A/D sampling thief in each sensor array element is respectively with F 1, F 2..., F lspeed signal parallel is sampled, be input to DSP device by parallel for the sample sequence obtained, through the internal algorithm process of DSP, the Frequency Estimation and the DOA that obtain incoming signal estimate, finally drive by output and display circuit display estimated result.
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Cited By (12)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259410A (en) * 2015-10-26 2016-01-20 天津大学 Under-sampling waveform frequency estimation method and device under strong noise interference
CN106777505A (en) * 2016-11-18 2017-05-31 天津大学 The frequency estimating methods and device of the robust of the undersampled signal based on frequency deviation identification
CN107656237A (en) * 2017-08-03 2018-02-02 天津大学 The method and its device of a kind of multiple source frequency and DOA joint-detections
CN108037481A (en) * 2017-12-01 2018-05-15 天津大学 The gradable thinned array frequency of robustness and DOA estimation method and device
CN108112265A (en) * 2016-09-21 2018-06-01 东莞华南设计创新院 Wifi localization methods with on-plane surface mimo antenna and its system
CN108344967A (en) * 2018-01-20 2018-07-31 中国人民解放军战略支援部队信息工程大学 2-d direction finding method for quick estimating based on relatively prime face battle array
CN108957386A (en) * 2018-04-03 2018-12-07 燕山大学 A kind of incoherent wave arrival direction estimating method under phase error
CN109151672A (en) * 2018-09-19 2019-01-04 西安交通大学 Audio source tracking system and its control method based on array microphone
CN109308453A (en) * 2018-08-10 2019-02-05 天津大学 Undersampled signal frequency estimating methods and device based on pattern clustering and spectrum correction
CN110146842A (en) * 2019-06-14 2019-08-20 哈尔滨工业大学 Signal carrier frequency and two dimension DOA method for parameter estimation based on lack sampling
CN110391820A (en) * 2019-06-11 2019-10-29 东南大学 A kind of Novel Communication method of reseptance for evading co-channel interference based on DFT
CN112333718A (en) * 2020-11-05 2021-02-05 哈尔滨商业大学 Frequency and arrival angle joint estimation method based on undersampled signals

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20090115650A1 (en) * 2007-11-07 2009-05-07 Lockheed Martin Corporation System and method for wideband direct sampling and beamforming using complex analog to digital converter
CN103941087A (en) * 2014-04-09 2014-07-23 天津大学 Method and device for measuring frequencies of high-frequency cosine signals under undersampling rate
CN104007316A (en) * 2014-05-29 2014-08-27 天津大学 High precision frequency measurement method and instrument at under-sampling rate

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20090115650A1 (en) * 2007-11-07 2009-05-07 Lockheed Martin Corporation System and method for wideband direct sampling and beamforming using complex analog to digital converter
CN103941087A (en) * 2014-04-09 2014-07-23 天津大学 Method and device for measuring frequencies of high-frequency cosine signals under undersampling rate
CN104007316A (en) * 2014-05-29 2014-08-27 天津大学 High precision frequency measurement method and instrument at under-sampling rate

Non-Patent Citations (4)

* Cited by examiner, † Cited by third party
Title
HUANG XIAODONG ET AL.: "Simplified Method of Designing FIR Filter with Controllable Center Frequency", 《TRANSACTIONS OF TIANJIN UNIVERSITY》 *
梁红等: "广义稳健中国剩余定理及其在空间欠采样信号DOA估计中的应用", 《西北工业大学学报》 *
梁红等: "空时欠采样下多目标频率和方位联合估计新方法", 《西北工业大学学报》 *
黄翔东等: "基于中国余数定理的欠采样下余弦信号的频率估计", 《物理学报》 *

Cited By (16)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN105259410A (en) * 2015-10-26 2016-01-20 天津大学 Under-sampling waveform frequency estimation method and device under strong noise interference
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