Fast Signal Recovery in the Presence of Mutual Coupling Based on New 2-D Direct Data Domain Approach

Open Access
Research Article
  • 1.1k Downloads

Abstract

The performance of adaptive algorithms, including direct data domain least square, can be significantly degraded in the presence of mutual coupling among array elements. In this paper, a new adaptive algorithm was proposed for the fast recovery of the signal with one snapshot of receiving signals in the presence of mutual coupling, based on the two-dimensional direct data domain least squares (2-D D3LS) for uniform rectangular array (URA). In this method, inverse mutual coupling matrix was not computed. Thus, the computation was reduced and the signal recovery was very fast. Taking mutual coupling into account, a method was derived for estimation of the coupling coefficient which can accurately estimate the coupling coefficient without any auxiliary sensors. Numerical simulations show that recovery of the desired signal is accurate in the presence of mutual coupling.

Keywords

Coupling Coefficient Adaptive Algorithm Antenna Element Mutual Coupling Uniform Linear Array 

1. Introduction

Adaptive antenna arrays are strongly affected by the existence of mutual coupling (MC) effect between antenna elements; thus, if the effects of MC are ignored, the system performance will not be accurate [1, 2]. Research into compensation for the MC has been mainly based on the idea of using open circuit voltages, firstly proposed by Gupta and Ksienski [2]. While this method has calculated the mutual impedance, the presence of other antenna elements has been ignored and a very simplified current distribution has been assumed for each antenna elements. Many efforts have been made to compensate for the MC effect for uniform linear array (ULA) and uniform circular array (UCA) [2, 3, 4, 5, 6, 7, 8, 9]. In [3], an adaptive algorithm was used to compensate for the MC effect in a ULA. In [7], the authors introduced a minimum norm technique MC compensation method, which is based on the technique in [2] for general arrays with arbitrary elements and more accurate. In [9], a new method was proposed to compensate for the MC effect which relied on the calculation of a new definition of mutual impedance. however, the authors did not deal with 2-D DOA estimation problem.

On the other hand, many algorithms of the 1-D DOA estimation have been extended to solve the 2-D cases [10, 11]; however, a few have considered the effect of mutual coupling or any other array errors [12]. Besides, most of these proposed adaptive algorithms are based on the covariance matrix of the interference. However, these statistical algorithms suffer from two major drawbacks. First, they require independent identically-distributed secondary data in order to estimate the covariance matrix of the interference. Unfortunately, the statistics of the interference may fluctuate rapidly over a short distance, limiting the availability of homogeneous secondary data. The resulting errors in the covariance matrix reduce the ability to suppress the interference. The second drawback is that the estimation of the covariance matrix requires the storage and processing of the secondary data. This is computationally intensive, requiring many calculations in real-time. Recently, direct data domain algorithms have been proposed to overcome these drawbacks of statistical techniques [13, 14, 15, 16]. The approach is to adaptively minimize the interference power while maintaining the array gain in the direction of the signal. The sample support problem is eliminated by avoiding the estimation of a covariance matrix which leads to enormous savings in the required real-time computations. The performance of this algorithm is affected by the MC effect, too [17] and must be compensated.

Unfortunately, the MC matrix tends to change with time due to environmental factors, so full elimination of its effect and prediction of its variability are impossible. Therefore, calibration procedures based upon signal processing algorithms are needed to estimate and compensate for the effect of the MC. The most likely way is to carry out some measurements for calibration. However, this procedure has the drawbacks of being time-consuming and very expensive [18]. Some other researches suggested self-calibration adaptive algorithms for damping the MC effect [19, 20, 21].

In this paper, a new adaptive algorithm was proposed for the fast recovery of the signal with one snapshot of receiving signals in the presence of mutual coupling, based on 2-D D3LS algorithm for URA. Then, utilizing the 2-D D3LS algorithm properties, a novel technique for the coupling coefficients estimation, without using any auxiliary sensors is presented.

This paper is organized as follows. Section 2, conventional 2-D D3LS algorithm is reviewed. In Section 3, a fast adaptive algorithm of direct data domain including mutual coupling effect is presented. In Section 4, a new technique is presented for compensation of the MC effect. In Section 5, numerical simulations illustrate these proposed techniques which can accurately recover the desired signal in the presence of MC.

2. 2-D Direct Data Domain Algorithm

Consider a URA consisting of Open image in new window equally spaced elements with the spacing of Open image in new window in rows (in the Open image in new window direction) and Open image in new window in columns (in the Open image in new window direction). The array receives a signal from a known direction Open image in new window and Open image in new window interferers from unknown directions Open image in new window , Open image in new window as shown in Figure 1.
Figure 1

URA with Open image in new window elements.

The output of the array voltage can be expressed as
where Open image in new window , Open image in new window , Open image in new window , and Open image in new window denote the received signal vector, steering matrix, signal plus jammers vector and additive white Gaussian noise vector, respectively, defined as:
We define Open image in new window and Open image in new window which represent the phase progression of the signal between one element and the next in the row and column, respectively. The Open image in new window is Open image in new window th signal's direction manifold vector, superscript Open image in new window is the transpose operation and the symbol Open image in new window denotes the Kronecker tensor. Therefore, by suppression of time dependence in the phasor notation, complex vector of phasor voltage is:
where Open image in new window and Open image in new window are the complex amplitude of the desired signal and Open image in new window th interferers, respectively. Next, the first row from each column is multiplied by Open image in new window and subtracted from the second row; then the result of each column is multiplied by Open image in new window and subtracted from the next column. This cancels out all the signals and only noise and interferers are left. The first row of the matrix in (5) is the constraint to the desired signal which produces a gain factor of Open image in new window . For a conventional adaptive array system, the Open image in new window weights Open image in new window are used and the relationship between Open image in new window with Open image in new window and Open image in new window can be chosen as Open image in new window , Open image in new window ,  Open image in new window [16]. Matrix equation can be constructed as:
For simplicity Open image in new window and Open image in new window . Because the matrix in (5) is not square, the conjugate gradient method (CGM) is used to solve the matrix equation and to obtain the weighting solution. It has a good convergence characteristic and converges to the minimum norm solution, even for the singular problem [13]. Now, the amplitude of the recovered signal is as [16]:
where Open image in new window is the weights vector in the absence of coupling and subscript, Open image in new window , denotes rounding down to the integer:

3. 2-D Fast Signal Recovery Algorithm in the Presence of Mutual Coupling

If one assumes that Open image in new window denotes the mutual coupling matrix (MCM) of the array, the output will be as:
Svantesson [6] showed that the coupling between the neighboring elements with the same interspace is almost the same and the magnitude of the mutual coupling coefficient between two far apart elements is so small that can be approximated to zero. Thus, a banded symmetric Toeplitz matrix can be used as a model for the mutual coupling of ULA and URA. In this paper, each sensor is assumed to be affected by the coupling of the 8 sensors around it, which is shown in Figure 2.
Figure 2

Map of mutual coupling.

We define MCM as [12]:
Then, the following equation is derived to recover the desired signal in the presence of mutual coupling (Proof in the appendix), notwithstanding to compute the inverse matrix of MC. Hence, this equation could be reduced the computation of the algorithm
where Open image in new window is the weights vector when coupling is known and
The conventional recovering of the signal is as the following:

where Open image in new window denotes, Open image in new window rows from the vector. Open image in new window is computationally intensive and requires many calculations in the real-time because evaluation of the inverse requires an Open image in new window process (here Open image in new window denotes "on the order of"). Therefore, (14) can be replaced with (16) and the number of processes would be an Open image in new window .

4. Mutual Coupling Compensation

In this section, a new method is presented to estimate the coupling coefficients from the properties of the 2-D D3LS algorithm. If the mutual coupling effect is ignored, the term Open image in new window , for Open image in new window and Open image in new window will have no signal components. However, in the presence of MC, for the edge elements in the URA, the above term can be written as the following:
As is seen in (17), when there are no interferers, the equations can be solved. In this paper, it is assumed that Open image in new window ; so Open image in new window . The above equations can be solved in order to estimate Open image in new window , Open image in new window , and Open image in new window . Once the system estimates the coupling coefficient, it needs only one snapshot of the data in order to obtain an acceptable solution. So, when the coupling is unknown, first we can estimate mutual coupling from (17) and then, the fast recovering of the signal is as the following:

where Open image in new window is the estimation of Open image in new window and Open image in new window is Open image in new window with replacement of Open image in new window , Open image in new window , Open image in new window with Open image in new window , Open image in new window , Open image in new window .

5. Numerical Examples

In this section, the capability of MC compensation for the proposed algorithm will be tested with two examples. Consider a URA with Open image in new window elements in which the spacing between each two elements in rows and columns is Open image in new window . The array receives the desired signal with one jammer. The signal to noise ratio is 20 dB and other parameters are listed in Table 1.
Table 1

Parameters for the desired signal and interferer.

 

Magnitude

Phase

Open image in new window

Open image in new window

Signal

1–10 V/m

0

75°

45°

Jammer1

1000 V/m

0

43°

−77°

The number of adaptive weights chosen for our simulation will be 16 [16]. Jammer is 60 dB stronger than the intensity of the desired signal. The magnitude of incident signal varies from 1 V/m to 10 V/m; but jammer intensities are constant as given in Table 1. Figure 3 shows the accuracy of the recovered signal in the presence of MC using new formulation (18) with comparison to the ideal recovering. Figure 4 shows the result of the recovered signal in the presence of MC, using a new proposed algorithm with comparison to the ideal recovering. The expected linear relationship is clearly seen and the jammer has been nulled and signal recovered correctly.
Figure 3

Recovered strength of the desired signal in the absence and presence of mutual coupling.

Figure 4

Recovered strength of the desired signal with the proposed algorithm in the presence of mutual coupling.

Later on, the performance of the proposed method is illustrated by the various simulations. The amplitude of the desired signal accuracy is measured by the root mean-squared error (RMSE), and Open image in new window is the number of Monte Carlo runs.

Figure 5 shows the RMSE of the estimated coupling coefficients versus signal-to-noise ratio (SNR). Figure 6 shows the RMSE of the estimated amplitude of the desired signal, versus SNR. For high SNR, error is very low and in case there is no noise, new formulation is equal to the ideal.
Figure 5

RMSE of the coupling coefficients versus the SNR.

Figure 6

RMSE of the recovered amplitude versus the SNR.

6. Conclusion

In this paper, the problems of 2-D D3LS algorithms were studied for recovering of the signal in the presence of mutual coupling and driving a new formulation to recover the signal in the presence of MC. Without using the moment of method and impedance matrix calculation, coupling coefficients can be automatically estimated and without computing the inverse matrix, the desired signal can be recovered. Because we did not use the inverse MC matrix, the amount of computation would be reduced. Moreover, simulation results were confirmed when SNR was high and the RMSE of the method was very close to the ideal D3LS in the absence of MC.

Appendix

In this appendix, (8) and (14) are proved. Consider a URA consisting of Open image in new window elements. The array receives one signal Open image in new window from a known direction Open image in new window and one interferer Open image in new window (this proof can be extended similarly). From (1), let the received signal at the array in the presence of mutual coupling for each element be
where Open image in new window , Open image in new window are the received signal and jammer at the Open image in new window th element, expressed as
By taking mutual coupling into account, from (11) for each column

(a) Absence of the Mutual Coupling

If the one row from each column is multiplied by Open image in new window and subtracted from the next row and then the result of each column is multiplied by Open image in new window and subtracted from the next column, in the absence of mutual coupling, this will cancel out all the signals and only noise and interferer will be left

The weight vectors should be in a way that produces zero output; therefore, a reduced rank matrix is formed in which the weighted sum of all its elements would be zero. In order to make the matrix not singular, the additional equation is introduced through the constraint that the same weights when operating on the signal produced a gain factor Open image in new window , which is the first equation. Therefore, (5) will be
Then, performing the matrix multiplication in (A.6) for the first row of the matrix will give
With performing the matrix multiplication in (A.6) for the second row of the matrix the following is obtained:
Open image in new window , Open image in new window , and Open image in new window , (A.9) will be true for all Open image in new window if and only if each summation in the parenthesis is equal to zero. Therefore, the first summation will be used
Similarly, the same can be done for the third row of the matrix (A.5), and so forth. In the absence of mutual coupling Open image in new window . From (A.3) and (A.10)
Then, (A.11) will be as simple as
Therefore, the desired signal can be recovered by

(b) Presence of the Mutual Coupling

When there is mutual coupling, the matrix (A.5) can be formed and the (A.3) and (A.10) can be written in a similar way
Similar to (A.11), the following can be presented
The recovered signal will be as follows:

Notes

Acknowledgment

The authors want to acknowledge the Iran Telecommunication Research Centre (ITRC) for their kindly supports.

References

  1. 1.
    Nishimura T, Bui HP, Nishimoto H, Ogawa Y, Ohgane T: Channel characteristics and performance of MIMO E-SDM systems in an indoor time-varying fading environment. Eurasip Journal on Wireless Communications and Networking 2010, 2010:-14.Google Scholar
  2. 2.
    Gupta IJ, Ksienski AA: Effect of mutual coupling on the performance of adaptive array. IEEE Transactions on Antennas and Propagation 1983, 31(5):785-791. 10.1109/TAP.1983.1143128CrossRefGoogle Scholar
  3. 3.
    Friedlander B, Weiss AJ: Direction finding in the presence of mutual coupling. IEEE Transactions on Antennas and Propagation 1991, 39: 273-284. 10.1109/8.76322CrossRefGoogle Scholar
  4. 4.
    Friel EM, Pasala KM: Effects of mutual coupling on the performance of STAP antenna arrays. IEEE Transactions on Aerospace and Electronic Systems 2000, 36(2):518-527. 10.1109/7.845236CrossRefGoogle Scholar
  5. 5.
    Lui HS, Hui HT: Mutual coupling compensation for direction-of-arrival estimations using the receiving-mutual-impedance method. International Journal of Antennas and Propagation 2010, 2010:-7.Google Scholar
  6. 6.
    Svantesson T: Modeling and estimation of mutual coupling in a uniform linear array of dipoles. Dept. Signals and Systems, Chalmers Univ. of Tech., Sweden; 1999.CrossRefGoogle Scholar
  7. 7.
    Lau CKE, Adve RS, Sarkar TK: Minimum norm mutual coupling compensation with applications in direction of arrival estimation. IEEE Transactions on Antennas and Propagation 2004, 52(8):2034-2041. 10.1109/TAP.2004.832511CrossRefGoogle Scholar
  8. 8.
    Huang Z, Balanis CA, Britcher CR: Mutual coupling compensation in UCAs: simulations and experiment. IEEE Transactions on Antennas and Propagation 2006, 54(11):3082-3086.CrossRefGoogle Scholar
  9. 9.
    Zhang TT, Lu YL, Hui HT: Compensation for the mutual coupling effect in uniform circular arrays for 2D DOA estimations employing the maximum likelihood technique. IEEE Transactions on Aerospace and Electronic Systems 2008, 44(3):1215-1221.CrossRefGoogle Scholar
  10. 10.
    Zoltowski MD, Haardt M, Mathews CP: Closed-form 2-D angle estimation with rectangular arrays in element space or beamspace via unitary ESPRIT. IEEE Transactions on Signal Processing 1996, 44(2):316-328. 10.1109/78.485927CrossRefGoogle Scholar
  11. 11.
    Liu J, Liu X: Joint 2-D DOA tracking for multiple moving targets using adaptive frequency estimation. Proceedings of IEEE International Conference on Acoustics, Speech and Signal Processing (ICASSP '07), 2007 2: 1113-1116.Google Scholar
  12. 12.
    Ye Z, Liu C: 2-D DOA estimation in the presence of mutual coupling. IEEE Transactions on Antennas and Propagation 2008, 56(10):3150-3158.MathSciNetCrossRefGoogle Scholar
  13. 13.
    Sarkar TK, Sangruji N: Adaptive nulling system for a narrow-band signal with a look-direction constraint utilizing the conjugate gradient method. IEEE Transactions on Antennas and Propagation 1989, 37(7):940-944. 10.1109/8.29389CrossRefGoogle Scholar
  14. 14.
    Sarkar TK, Wang H, Park S, Adve R, Koh J, Kim K, Zhang Y, Wicks MC, Brown RD: A deterministic least-squares approach to space-time adaptive processing (STAP). IEEE Transactions on Antennas and Propagation 2001, 49(1):91-103. 10.1109/8.910535MATHCrossRefGoogle Scholar
  15. 15.
    Sarkar T, Wicks M, Palma M, Bonneau R: Smart Antennas. Wiley, New York, NY, USA; 2003.CrossRefGoogle Scholar
  16. 16.
    Wang LL, Fang DAG: Modified 2-D direct data domain algorithm in adaptive antenna arrays. Proceedings of Asia-Pacific Microwave Conference (APMC '05), December 2005Google Scholar
  17. 17.
    Adve RS, Sarkar TK: Compensation for the effects of mutual coupling on direct data domain adaptive algorithms. IEEE Transactions on Antennas and Propagation 2000, 48(1):86-94. 10.1109/8.827389CrossRefGoogle Scholar
  18. 18.
    Wang B, Wang Y, Guo Y: Mutual coupling calibration with instrumental sensors. Electronics Letters 2004, 40(7):406-408. 10.1049/el:20040287CrossRefGoogle Scholar
  19. 19.
    Horiki Y, Newman EH: A self-calibration technique for a DOA array with near-zone scatterers. IEEE Transactions on Antennas and Propagation 2006, 54(4):1162-1166. 10.1109/TAP.2006.872672CrossRefGoogle Scholar
  20. 20.
    Sellone F, Serra A: A novel online mutual coupling compensation algorithm for uniform and linear arrays. IEEE Transactions on Signal Processing 2007, 55(2):560-573.MathSciNetCrossRefGoogle Scholar
  21. 21.
    Ye Z, Liu C: On the resiliency of MUSIC direction finding against antenna sensor coupling. IEEE Transactions on Antennas and Propagation 2008, 56(2):371-380.MathSciNetCrossRefGoogle Scholar

Copyright information

© Ali Azarbar et al. 2011

This article is published under license to BioMed Central Ltd. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Authors and Affiliations

  • Ali Azarbar
    • 1
  • G. R. Dadashzadeh
    • 2
  • H. R. Bakhshi
    • 2
  1. 1.Department of Computer and Information Technology EngineeringIslamic Azad University, Parand BranchTehranIran
  2. 2.Faculty of EngineeringShahed UniversityTehranIran

Personalised recommendations