Junxian Jin1, Lin Chen1, and Zhong Chen1
1Department of Electronic Science, Fujian Provincial Key Laboratory of Plasma and Magnetic Resonance, School of Electronic Science and Engineering, National Model Microelectronics College, Xiamen University, Xiamen, China
Synopsis
Keywords: Relaxometry, Relaxometry, T2 Mapping, T2* Mapping
Motivation: T2 and T2* mapping can quantitatively characterize tissue pathologies, improving diagnosis and treatment, but their clinical applications are hindered by relatively long scan times.
Goal(s): To develop an ultrafast method for simultaneously obtaining T2 and T2* mapping.
Approach: A biaxial spatiotemporally encoded (SPEN) sequence with multi-spin-echo trains and spiral out-in-out-in trajectory was developed to obtain multiple images with different echo times within a single shot. The acquired signal was fitted to yield simultaneous T2 and T2* mapping.
Results: Numerical simulations and in vivo rat brain and kidney experiments were conducted to validate the proposed method.
Impact: We developed an ultrafast technique to
simultaneously obtain T2 and T2* mapping in 150 ms,
potentially facilitating the use of T2 and T2*
mapping in scenarios requiring high time
resolution.
Introduction
Quantitative magnetic resonance imaging is a valuable diagnostic
tool that has gained significant importance in various research and clinical applications.1 In general, traditional T2
and T2* mapping involve the acquisition of several images at various
echo times, resulting in relatively long scan times and increased
susceptibility to subject motion. Single-shot spatiotemporally encoded (SPEN)2 is an ultrafast MRI technique
that provides comparable imaging speed to traditional echo-planar imaging
(EPI), along with distinctive advantages such as increased resilience to B0
inhomogeneity, a fully refocused mechanism, and flexible field-of-view (FOV)
imaging. Previous studies have demonstrated that SPEN MRI can provide ultrafast
real-time T2 mapping.3 Here, a biaxial SPEN
sequence with multi-spin-echo trains and spiral
out-in-out-in trajectory was developed to simultaneously obtain T2
and T2* mapping with flexible FOV and further reduced scan time.Methods
The proposed SPEN sequence with multi-spin-echo trains and spiral out-in-out-in trajectory is shown in Fig 1(a). Due to the biaxial frequency-swept excitation strategy with Chirp pulses, the acquired signal $$$S(t)$$$ can be modeled as:
$$S(t)=\iint\rho(x,y)exp(i\phi_a(x,y,t)dxdy\cdot exp(-\frac{t}{T_{2}})\cdot exp(-\frac{\triangle}{T_2^\prime})$$ $$\phi_a(x,y,t)=\phi_e(x,y,t)+\gamma\int_{0}^{t} G_x(t)dt\cdot x+\gamma\int_{0}^{t} G_y(t)dt\cdot y$$ $$\triangle=|t-\tau|$$ $$\frac{1}{T_2^*}=\frac{1}{T_2}+\frac{1}{T_2^\prime}$$
where $$$\rho(x,y)$$$ denotes
the spatial profile of spin density, $$$\tau$$$ refers
to the nominal echo time of multi-spin-echo trains, and $$$T_2^\prime$$$ accounts
for contributions from magnetic susceptibility. $$$G_x(t)$$$ and $$$G_y(t)$$$ epresent the decoding
gradients, which are used to decode a flexible FOV with a pre-defined
trajectory. In this study, a spiral out-in-out-in trajectory was adopted. As
shown in Fig 1(b), single-shot acquisition yields a series
of flexible FOV images with varying echo times due to their variable contrast. Fitting
multiple contrast images with different effective echo times yields T2
and T2*. The flowchat of the
proposed method is shown in Fig 1. The numerical simulations were carried out
with the MRiLab software.4 The in vivo rat experiments were
performed on a 7T Varian MRI scanner.Results and Discussion
Fig 2 shows T2 and T2*
mapping for the numerical simulation, with a flexible FOV targeting the
centered seven tubes while discarding the peripheral circle. Despite exciting
the peripheral circle with a biaxial chirp pulse, the reconstructed images were
unaffected by interference from the peripheral circle due to the special
selective properties of SPEN MRI. As shown in Fig 3(e), the error in T2
is within ± 1.5 ms, and the error in T2* is within ± 2.5 ms.
Fig 3 demonstrates in vivo rat experiments
targeting brain T2 and T2* mapping, along with
reconstructed images at different echo times. The results show that
satisfactory reconstructed images were obtained with a reduced FOV, free of
aliasing artifacts. The T2 and T2* mapping obtained by
SPEN MRI is consistent with that obtained by the SE method and MGRE (multi-echo
gradient-echo) method.
Fig 4 shows T2 and T2* mapping for the in
vivo rat kidney, which is more challenging compared to brain experiments due to
severe B0 inhomogeneity and respiratory motion. The results indicate that
satisfactory T2 and T2* mapping can be obtained using
SPEN MRI. T2 values is 62.5 ± 4.1 ms in medulla, and 47.6 ± 7.4 ms
in cortex. T2* values is 47.2 ± 8.4 ms in medulla, and 29.4 ± 8.2 ms
in cortex.The values are consistent with previous studies.3, 5, 6
Compared
to the previous study,7 the
proposed method can obtain additional T2* mapping and further reduce
the scan time by utilizing flexible FOV scheme and spiral trajectory with high
sampling efficiency.Conclusions
Ultrafast T2 and T2*
mapping can be simultaneously obtained using non-Cartesian single-shot SPEN MRI
with flexible FOV and satisfactory resilience to B0 inhomogeneity.
The proposed method can facilitate the applications of T2 and T2*
mapping in experiments with high time requirements.Acknowledgements
This work is supported by the National
Natural Science Foundation of China, Grant/Award Number: 82302151, 12175189,
22161142024; Shenzhen Science and Technology Program, Grant/Award Number: JCYJ20220818101213029;
Fujian Province Science and Technology Project, Grant/Award Number: 2022J05013;
Xiamen University Nanqiang Outstanding Talents Program.References
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