2013
DOI: 10.1371/journal.pone.0066612
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Turbo-FLASH Based Arterial Spin Labeled Perfusion MRI at 7 T

Abstract: Motivations of arterial spin labeling (ASL) at ultrahigh magnetic fields include prolonged blood T1 and greater signal-to-noise ratio (SNR). However, increased B0 and B1 inhomogeneities and increased specific absorption ratio (SAR) challenge practical ASL implementations. In this study, Turbo-FLASH (Fast Low Angle Shot) based pulsed and pseudo-continuous ASL sequences were performed at 7T, by taking advantage of the relatively low SAR and short TE of Turbo-FLASH that minimizes susceptibility artifacts. Consist… Show more

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Cited by 47 publications
(73 citation statements)
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“…Moreover, the imaging acquisition parameters were adjusted at 7T to accommodate the SAR constraint. Theoretically, performing ASL at ultrahigh magnetic field strength can be beneficial because of the increased SNR, as well as the lengthened T 1 -realxation time (Zuo et al, 2013). The latter feature not only loosens the restriction on the length of the PLD and image acquisition window, it also creates less spatial blurring as indicated by the simulated PSF shown in Fig.…”
Section: Discussionmentioning
confidence: 99%
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“…Moreover, the imaging acquisition parameters were adjusted at 7T to accommodate the SAR constraint. Theoretically, performing ASL at ultrahigh magnetic field strength can be beneficial because of the increased SNR, as well as the lengthened T 1 -realxation time (Zuo et al, 2013). The latter feature not only loosens the restriction on the length of the PLD and image acquisition window, it also creates less spatial blurring as indicated by the simulated PSF shown in Fig.…”
Section: Discussionmentioning
confidence: 99%
“…Incorporating the train of RF excitations pulses from the TFL readout into the final perfusion weighted signal presentation, the TFL-based pCASL signal Δ S can be modeled as (Zuo et al, 2013): normalΔS=2αfSM0[e-wR1a-e-false(τ+wfalse)R1a]false(E1cosθfalse)jλR1a[false(E1cosθfalse)j+false(1-E1false)1-false(E1cosθfalse)j1-E1cosθ] where E 1 = e −TR / T 1 , θ is the FA of the RF excitation pulses in TFL, S M 0 is the M 0 signal (control image intensity), and j is the number of acquired PE lines till it reaches the center of k-space in the TFL readout. Since multiple MB slices are acquired sequentially after each pCASL preparation, the nominal PLD was adjusted for each slice according to w =PLD + n *Tacq, where Tacq is the imaging time for each 2D slice, and n is the index for the slice ordering.…”
Section: Methodsmentioning
confidence: 99%
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