2010
DOI: 10.1029/2009rs004260
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A fast and automatically paired 2-D direction-of-arrival estimation with and without estimating the mutual coupling coefficients

Abstract: [1] A new technique is proposed for the solution of pairing problem which is observed when fast algorithms are used for two-dimensional (2-D) direction-of-arrival (DOA) estimation. Proposed method is integrated with array interpolation for efficient use of antenna elements. Two virtual arrays are generated which are positioned accordingly with respect to the real array. ESPRIT algorithm is used by employing both the real and virtual arrays. The eigenvalues of the rotational transformation matrix have the angle… Show more

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Cited by 11 publications
(5 citation statements)
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“…Scatter plots of the estimated azimuth and elevation are plotted in Figure 11, where the results have been averaged over 500 Monte Carlo runs. A challenge for further research is to incorporate the mutual coupling processing method to provide a more realistic scheme like the excellent algorithms [18,19,20] for applying sensor arrays.…”
Section: Simulation Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…Scatter plots of the estimated azimuth and elevation are plotted in Figure 11, where the results have been averaged over 500 Monte Carlo runs. A challenge for further research is to incorporate the mutual coupling processing method to provide a more realistic scheme like the excellent algorithms [18,19,20] for applying sensor arrays.…”
Section: Simulation Resultsmentioning
confidence: 99%
“…For each azimuth, they designed a new search-free rooting algorithm by expanding the array manifold into a double Fourier series. It is proved that even in the presence of severe mutual coupling [19,20], this hybrid approach can yield very robust 2D DOA estimation performances.…”
Section: Introductionmentioning
confidence: 99%
“…The array model in can be written for the m th antenna as ym(t)=α1am(normalΘ1)s(t)+i=2Nαitruea~m(normalΘi,di)s(t)+nm(t)which can always be written as ym(t)=α1am(normalΘ1)s(t)(1+βm2+βm3++βmN)+nm(t)where β mi is a complex direction‐dependent coefficient. Then the array model for far‐field sources can be given as boldy(t)=normalΓ(normalΘ)bolda(normalΘ)s(t)+boldn(t),3.0ptt=1,,Ewhere Γ ( Θ ) is a direction‐dependent diagonal matrix and it represents the effect of near‐field multipaths on far‐field source as well as the mutual coupling [ Filik and Tuncer , ] between the antennas and gain/phase mismatch errors. Note that the model in has a single far‐field source and the artifacts from near‐field sources are represented by Γ ( Θ ).…”
Section: Direction Finding For a Far‐field Source With Multipath Compmentioning
confidence: 99%
“…where (Θ) is a direction-dependent diagonal matrix and it represents the effect of near-field multipaths on far-field source as well as the mutual coupling [Filik and Tuncer, 2010] between the antennas and gain/phase mismatch errors. Note that the model in (9) has a single far-field source and the artifacts from near-field sources are represented by (Θ).…”
Section: Direction Finding For a Far-field Source With Multipath Compmentioning
confidence: 99%
“…Still under the single‐mode assumption, from a signal‐processing point of view, ( Z + Z L ) can be regarded as a coupling matrix [ Gupta and Ksienski , 1983; Clerckx et al , 2007], whose effects are easily undone as soon as the array impedance matrix is known. Such coupling matrices can then be used to obtain direction‐of‐arrival estimates that account for the effects of mutual coupling [ Filik and Tuncer , 2010].…”
Section: Generalities About Mutual Coupling In Finite Arraysmentioning
confidence: 99%