2014
DOI: 10.1109/tuffc.2014.3010
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Short-lag spatial coherence imaging on matrix arrays, Part 1: Beamforming methods and simulation studies

Abstract: Short-lag spatial coherence (SLSC) imaging is a beamforming technique that has demonstrated improved imaging performance compared with conventional B-mode imaging in previous studies. Thus far, the use of 1-D arrays has limited coherence measurements and SLSC imaging to a single dimension. Here, the SLSC algorithm is extended for use on 2-D matrix array transducers and applied in a simulation study examining imaging performance as a function of subaperture configuration and of incoherent channel noise. SLSC im… Show more

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Cited by 21 publications
(18 citation statements)
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“…Spatial coherence can be expressed as spatial correlation and further simplified to a product of two triangle functions when the diffuse scatterers are insonified with a narrowband pulse from an unapodized rectangular aperture. The spatial correlation for this case (of diffuse scatterers) has been derived in Part I [7] and is given here again: RDS(Δx,Δy)=true(1true∣ΔxDxtrue∣true)true(1true∣ΔyDytrue∣true), In 1, Δ x and Δ y denote the distance between two points in the aperture plane, and D x and D y denote the transmit aperture size in the x and y dimensions, respectively. The spatial correlation of the pressure field can be estimated from the signals of the individual elements of a matrix array as R^(i,j)=n=n1n2si(n)sj(n)n=n1n2si2(n)n=n1n2sj2(n), where i and j are two elements on the 2-D aperture, s i (n) and s j (n) are the signals sampled by those elements, n is a sample number in the time dimension, and the difference n 2 – n 1 represents the axial kernel length used to calculate interelement correlation and is typically on the order of a wavelength.…”
Section: Methodsmentioning
confidence: 99%
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“…Spatial coherence can be expressed as spatial correlation and further simplified to a product of two triangle functions when the diffuse scatterers are insonified with a narrowband pulse from an unapodized rectangular aperture. The spatial correlation for this case (of diffuse scatterers) has been derived in Part I [7] and is given here again: RDS(Δx,Δy)=true(1true∣ΔxDxtrue∣true)true(1true∣ΔyDytrue∣true), In 1, Δ x and Δ y denote the distance between two points in the aperture plane, and D x and D y denote the transmit aperture size in the x and y dimensions, respectively. The spatial correlation of the pressure field can be estimated from the signals of the individual elements of a matrix array as R^(i,j)=n=n1n2si(n)sj(n)n=n1n2si2(n)n=n1n2sj2(n), where i and j are two elements on the 2-D aperture, s i (n) and s j (n) are the signals sampled by those elements, n is a sample number in the time dimension, and the difference n 2 – n 1 represents the axial kernel length used to calculate interelement correlation and is typically on the order of a wavelength.…”
Section: Methodsmentioning
confidence: 99%
“…Then, to obtain a single SLSC voxel, R^(i,j) is computed (by applying equation 2 to the individual-element signals) and summed over all short-lag pairs of i and j . For a complete SLSC volume, the last step is repeated at each depth for every received individual-element data set [7]. …”
Section: Methodsmentioning
confidence: 99%
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