2013 IEEE International Ultrasonics Symposium (IUS) 2013
DOI: 10.1109/ultsym.2013.0148
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Compensating the combined effects of absorption and dispersion in plane wave pulse-echo ultrasound imaging using sparse recovery

Abstract: We extended our concept for fast image acquisition in pulse-echo ultrasound imaging based on sparse recovery (SR) to compensate for the combined effects of absorption and dispersion. Using measurement data obtained from a multi-tissue phantom (A) and a human thyroid (B, in vivo), we demonstrated that image quality can be significantly improved by this extension. Emitting only two steered plane waves, our extended SR-based concept outperformed synthetic aperture (SA) imaging (128 wave emissions), delay-and-sum … Show more

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Cited by 12 publications
(27 citation statements)
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“…For a polyfrequent perturbation exhibiting N f components with equispaced discrete frequencies f l ∈ R + , 0 ≤ l < N f , the acoustic pressure p l associated with each component is governed by [1] Δ +k 2 l p l (r) = k l 2 γ κ (r)p l (r) + ∇ · γ ρ (r)∇p l (r) , (1) where Δ denotes the Laplacian,k l is a complex-valued wavenumber depending on the absorption mechanism (cf. [3], [1], [2]), k l = 2πf l c 0 −1 is the wavenumber in the lossless case and c 0 = (κ 0 ρ 0 ) −1/2 is the small-signal equilibrium sound speed in the homogeneous medium. The acoustic pressurep l in the time domain is related to each component p l via the identityp l (r, t) = Re p l (r)e j2πf l t .…”
Section: A Integral Equation For the Scattered Acoustic Pressurementioning
confidence: 99%
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“…For a polyfrequent perturbation exhibiting N f components with equispaced discrete frequencies f l ∈ R + , 0 ≤ l < N f , the acoustic pressure p l associated with each component is governed by [1] Δ +k 2 l p l (r) = k l 2 γ κ (r)p l (r) + ∇ · γ ρ (r)∇p l (r) , (1) where Δ denotes the Laplacian,k l is a complex-valued wavenumber depending on the absorption mechanism (cf. [3], [1], [2]), k l = 2πf l c 0 −1 is the wavenumber in the lossless case and c 0 = (κ 0 ρ 0 ) −1/2 is the small-signal equilibrium sound speed in the homogeneous medium. The acoustic pressurep l in the time domain is related to each component p l via the identityp l (r, t) = Re p l (r)e j2πf l t .…”
Section: A Integral Equation For the Scattered Acoustic Pressurementioning
confidence: 99%
“…We utilized the sparse recovery formalism [3] to solve the ill-posed system (8). For this purpose, we assumed that there exist orthonormal linear transforms Ψ (κ) and Ψ (ρ) such that γ κ,ρ,BP = Ψ (κ,ρ) θ (κ,ρ) with nearly sparse coefficient vectors θ (κ,ρ) .…”
Section: B Linear Inverse Scattering Problemmentioning
confidence: 99%
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