2019
DOI: 10.1002/mrm.28062
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T1‐corrected quantitative chemical shift‐encoded MRI

Abstract: Purpose To develop and validate a T1‐corrected chemical‐shift encoded MRI (CSE‐MRI) method to improve noise performance and reduce bias for quantification of tissue proton density fat‐fraction (PDFF). Methods A variable flip angle (VFA)‐CSE‐MRI method using joint‐fit reconstruction was developed and implemented. In computer simulations and phantom experiments, sources of bias measured using VFA‐CSE‐MRI were investigated. The effect of tissue T1 on bias using low flip angle (LFA)‐CSE‐MRI was also evaluated. The… Show more

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Cited by 13 publications
(26 citation statements)
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References 40 publications
(111 reference statements)
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“…10,26 This signal model uses a constrained common phase for fat and water as proposed by Bydder et al 24 A constrained phase assumption accurately reflects the physics of SGRE acquisitions so long as the flip angle used for RF excitation is maintained relatively low (i.e., ≤ ∼ 5 • ). 27 From here, the presence of CGs can be modeled in the SGRE acquisition for a localized voxel as follows:…”
Section: Theorymentioning
confidence: 99%
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“…10,26 This signal model uses a constrained common phase for fat and water as proposed by Bydder et al 24 A constrained phase assumption accurately reflects the physics of SGRE acquisitions so long as the flip angle used for RF excitation is maintained relatively low (i.e., ≤ ∼ 5 • ). 27 From here, the presence of CGs can be modeled in the SGRE acquisition for a localized voxel as follows:…”
Section: Theorymentioning
confidence: 99%
“…In this work, we use the following spoiled gradient echo (SGRE) CSE‐MRI signal model 24,25 for N echoes acquired at TEs t1,t2,,tN as a reference and starting point:snη,R2,ψ,M0,ϕ=M0eiϕ1η+ηCFtneR2tnei2πψtn,where M0eiϕ is the complex signal amplitude (M0) and constant phase (ϕ), η is PDFF, ψ is the B 0 field map (Hz), and C F is the sum of complex exponentials reflecting a multi‐peak spectral model of fat, typically 6 peaks 10,26 . This signal model uses a constrained common phase for fat and water as proposed by Bydder et al 24 A constrained phase assumption accurately reflects the physics of SGRE acquisitions so long as the flip angle used for RF excitation is maintained relatively low (i.e., 5) 27 . From here, the presence of CGs can be modeled in the SGRE acquisition for a localized voxel as follows:leftsn,CG)(x,y,z,bold-italicθ=sn)(θeiϕCG)(x,y,z,tn0.166667emfor0.3embold-italicθ=}{η,R2,ψ,M0,ϕ,where ϕitalicCGx,y,z,…”
Section: Theorymentioning
confidence: 99%
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“…The longitudinal relaxation time ( T 1 ) of fat and water are of interest for accurate fat‐water separation and fat quantification, for example, in the context of fatty liver disease 1,2 . One approach for fat quantification has included a multiresonance model of the fat spectrum, the T 1 of fat, and the T 1 of water as parameters to reduce bias 3–5 . That approach features a single T 1 for fat and thus cannot account for the different T 1 s of resonances in the fat spectrum 6 .…”
Section: Introductionmentioning
confidence: 99%
“…The variable flip angle (VFA) method is based on rapid spoiled gradient echo (SGRE) 4 acquisitions that enable fast and three‐dimensional whole liver T1 mapping within 1–2 breath‐holds. VFA methods are feasible to incorporate with chemical shift approaches, 5 which reduces the confounding effect of fat deposition. Multiecho chemical shift approaches can also measure R2* simultaneously.…”
mentioning
confidence: 99%