2014
DOI: 10.1002/mrm.25377
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Improved quantitative myocardial T2 mapping: Impact of the fitting model

Abstract: Purpose To develop an improved T2 prepared (T2prep) balanced steady-state free-precession (bSSFP) sequence and signal relaxation curve fitting method for myocardial T2 mapping. Methods Myocardial T2 mapping is commonly performed by acquisition of multiple T2prep bSSFP images and estimating the voxel-wise T2 values using a 2-parameter fit for relaxation. However, a 2-parameter fit model does not take into account the effect of imaging pulses in a bSSFP sequence or other imperfections in T2prep RF pulses, whic… Show more

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Cited by 58 publications
(103 citation statements)
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“…Akcakaya et al have proposed a saturation preparation module to eliminate T 1 relaxation effects when combining a T 2 preparation with a gradient echo readout. Using an additional saturation preparation scan they were able to remove T 1 weighting effects during the gradient echo readout in T 2 quantification of the myocardium with good noise performance . Therefore, the proposed approach for the use of an additional saturation preparation scan uses a similar principle.…”
Section: Discussionmentioning
confidence: 99%
“…Akcakaya et al have proposed a saturation preparation module to eliminate T 1 relaxation effects when combining a T 2 preparation with a gradient echo readout. Using an additional saturation preparation scan they were able to remove T 1 weighting effects during the gradient echo readout in T 2 quantification of the myocardium with good noise performance . Therefore, the proposed approach for the use of an additional saturation preparation scan uses a similar principle.…”
Section: Discussionmentioning
confidence: 99%
“…A composite saturation pulse, based on Sung and Nayak , with 1 kHz bandwidth and 10 ms duration is used. T 2 prep uses nonselective opening and closing 90° hard pulses with 2.3 kHz bandwidth and 0.44 ms duration, to minimize T 2 * effects that might occur during the pulse , while the refocus pulses are weighted in a MLEV opposing phase pairs scheme to compensate for RF pulse shape imperfection . Additionally, for TE prep = 0, a 90° followed immediately by a −90°, followed by a crusher gradient was used, similar to the one proposed in Huang et al , shown to reduce the effect of B 0 and B 1 variations of the excitation and refocusing pulses of the T 2 prep sequence, and improving the T 2 quantification accuracy .…”
Section: Methodsmentioning
confidence: 99%
“…This model is given by: normalM4parametertrue(normalTsat,TET2Ptrue)=Atrue(1 enormalTsat/normalT1true)normaleTET2P/normalT2+B, where the parameters, A and B do not depend on the saturation time, T sat or the T 2 prep time, TE T2P . As detailed in Akcakaya et al , the B parameter captures the effect of the imaging pulses, and is a function of the steady‐state magnetization, as well as sequence parameters. The A parameter is a function of the signal at full‐recovery, and sequence parameters (flip angle, number of pulses, repetition time, etc).…”
Section: Methodsmentioning
confidence: 99%
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