2017
DOI: 10.1002/mp.12375
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Fast computation of full density matrix of multispin systems for spatially localizedin vivomagnetic resonance spectroscopy

Abstract: Purpose Numerical simulations of three-dimensionally localized MRS spectra have been very time-consuming for multi-spin systems because the current state-of-the-art requires computation of a large ensemble of spins pixel-by-pixel in three dimensional space. This paper describes a highly accelerated technique for computing spatially localized MRS spectra using the full solution to the Liouville–von Neumann equation. Methods The time evolution of spatially localized multispin density matrix as the full solutio… Show more

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Cited by 44 publications
(56 citation statements)
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“…Chemical shifts and coupling constants were taken from literature (Govind et al, 2015;Govindaraju et al, 2000;Near et al, 2013). To account for the spatially varying editing efficiency within the voxel due to chemical shift displacement effects Kaiser et al, 2008;Near et al,2013), a fast computation algorithm for spatially localized MRS was employed (Zhang et al, 2017). All simulations were performed on a three-dimensional grid of 21 × 21 × 21 spatial points within a 3 × 3 × 3 cm 3 voxel, using ideal excitation and shaped refocusing pulses.…”
Section: Phantom and In Vivo Datamentioning
confidence: 99%
“…Chemical shifts and coupling constants were taken from literature (Govind et al, 2015;Govindaraju et al, 2000;Near et al, 2013). To account for the spatially varying editing efficiency within the voxel due to chemical shift displacement effects Kaiser et al, 2008;Near et al,2013), a fast computation algorithm for spatially localized MRS was employed (Zhang et al, 2017). All simulations were performed on a three-dimensional grid of 21 × 21 × 21 spatial points within a 3 × 3 × 3 cm 3 voxel, using ideal excitation and shaped refocusing pulses.…”
Section: Phantom and In Vivo Datamentioning
confidence: 99%
“…The localized density‐matrix simulations of the GABA, GSH, and EtOH spin systems following the HERMES experiment at 3T were performed in FID‐A, accelerated by the recently published spatial averaging method . Ideal excitation and experimental refocusing and editing pulses were used.…”
Section: Methodsmentioning
confidence: 99%
“…The localized density-matrix simulations of the GABA, GSH, and EtOH spin systems following the HERMES experiment at 3T were performed in FID-A, 18 accelerated by the recently published spatial averaging method. 19 Ideal excitation and experimental refocusing and editing pulses were used. Simulations were performed on a 101 × 101 two-dimensional spatial array in the dimensions defined by the refocusing pulses spanning 4.5 × 4.5 cm 2 (ie the voxel length plus 50% in each dimension), with the following parameters: T E 80 ms; 20 ms editing pulse duration; 8192 data points; 5 kHz spectral width; 2 Hz simulated linewidth; additional line broadening using a 2 Hz exponential filter.…”
Section: Simulations Editing Efficiency and Phantom Experimentsmentioning
confidence: 99%
“…Metabolite concentrations were determined using an LCModel fitting routine developed in-house [1416]. To generate the basis set for LCModel fitting, the exact PRESS readout sequence used in the in vivo studies was simulated using the highly accelerated one-dimensional projection technique [21]. Effects of scalar evolution of the Glu signal during iPFG train were quantified and results are included in the supporting information.…”
Section: Methodsmentioning
confidence: 99%