Diagnostic image generating apparatus, medical image system, and beamforming method
US-9220481-B2 · Dec 29, 2015 · US
US9955943B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9955943-B2 |
| Application number | US-201414339780-A |
| Country | US |
| Kind code | B2 |
| Filing date | Jul 24, 2014 |
| Priority date | Feb 3, 2012 |
| Publication date | May 1, 2018 |
| Grant date | May 1, 2018 |
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Systems and methods for super-resolution ultrasound imaging using a windowed and generalized TR-MUSIC algorithm that divides the imaging region into overlapping sub-regions and applies the TR-MUSIC algorithm to the windowed backscattered ultrasound signals corresponding to each sub-region. The algorithm is also structured to account for the ultrasound attenuation in the medium and the finite-size effects of ultrasound transducer elements.
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What is claimed is: 1. A method of performing ultrasound imaging of a medium, comprising: exciting a first transducer element in an array of transducer elements to direct an ultrasound signal into a target region within the medium; receiving a backscatter signal from the target region within the medium with the array of transducer elements; generating an inter-element transfer matrix of the received backscatter signal; generating a generalized time-reversal (TR) matrix from the inter-element transfer matrix; and generating a pseudo-spectrum for generalized TR-Music imaging of the target region, wherein generating the inter-element transfer matrix comprises calculating the inter-element transfer matrix as a function of an electro-mechanical response of each transducer element in the array, a diffraction response of each transducer element in the array, and attenuation in the target region. 2. A method as recited in claim 1 , wherein the diffraction response of each transducer element is a function of finite size effects of the array of transducer elements. 3. A method as recited in claim 2 , wherein the inter-element transfer matrix is calculated as according to a function a i (r 0 ,ω) over a surface of a transducer element i, wherein: a i ( r 0 , ω ) = ∫ ∫ S i g 0 ( r ❘ r 0 ) d s , and wherein ω is an angular frequency, ds is a delimiter of integration, g 0 (ω,r|r 0 ) is the free-space Green's function, a i (r 0 ,ω) is the integral of the Green's function over the surface of element i, and r corresponds to a location of a wavefield resulting from a point source at a location r 0 . 4. A method as recited in claim 1 , wherein the inter-element transfer matrix K is calculated according to the function: K = 2 i k _ 4 ω κ 0 F ( ω ) ∫ ∫ ∫ V 0 γ κ ( r 0 ) A r 0 A r 0 T d v 0 ; and wherein i is an imaginary unit, k is a complex wave number, ω is an angular frequency, κ 0 is an average compressibility of the medium, F(ω) is an electromechanical transfer function, V 0 is a scattering volume, γ κ is a fluctuation equation, r 0 is a location, dv 0 is a delimiter of integration, and the superscript T in A r a T denotes that A r 0 T is the transpose of A r 0 which is an N-dimensional column vector given by: [ a 1 ( r 0 ,ω) a 2 ( r 0 ,ω) . . . a N ( r 0 ,ω)]. 5. A method as recited in claim 1 , wherein the generalized time-reversal matrix is calculated according to: T = - 4 k _ 8 ( ω κ 0 ) 2 F
combining overlapping images, e.g. spatial compounding · CPC title
using a transducer array · CPC title
using synthetic aperture techniques · CPC title
using special techniques for image reconstruction, e.g. FFT, geometrical transformations, spatial deconvolution, time deconvolution · CPC title
Tomography (A61B8/10, A61B8/12 take precedence) · CPC title
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