Xinpei Wang1, Jichang Zhang1, and Chengbo Wang1
1Faculty of Science and Engineering, University of Nottingham Ningbo China, Ningbo, China
Synopsis
Plenty of studies have reported
correlations between the tissue pathological changes and abnormal T1 value. However, T1 mapping pulse sequences often
suffer from the B1 inhomogeneity and long scan time. To improve the time efficiency
without leading to the worse robustness to B1 inhomogeneity, we develop an accelerated MPRAGE-based 3D T1 mapping
method by using SPGR steady state. Our proposed method is demonstrated in
phantom experiments and the preliminary in-vivo brain scan.
Introduction
T1 relaxation time is one of the most important quantitative
parameters in MRI. Many different MPRAGE-based T1 mapping techniques have been
developed and investigated. MP2RAGE1, can perform T1 mapping with self-correction of receive
magnetic field ( B1- ) and a first-order
correction of transmit magnetic field ( B1+ ) by two T1-weighted images. However, imperfect inversion recovery and a small amount of B1 error still degrade the
accuracy of T1 measurement2,3. Liu et al.4 proposed 3-TI MPRAGE to estimate T1 accurately from several T1-weighted images by varying the inversion time based
on a 3D MPRAGE sequence while keeping the sum of the inversion time and time
recovery constant, which results in a lot of waiting time for the recovery of
the longitudinal magnetization3. In this study, by
using SPGR steady state, we develop a modified 3-TI MPRAGE pulse sequence for 3D T1 mapping which does not need B1 correction
and can significantly reduce the imaging time. We demonstrate the
feasibility of the proposed T1 mapping method in phantoms and healthy human
subjects. Methods
In our approach, the spoiled
gradient echo (SPGR) sequence is implemented at the beginning and in the
following data acquisitions to achieve the steady state5, which will be
used as the reference point before every inversion pulse cycle. The
proposed MRI pulse sequence is shown in Figure 1. At the beginning, sufficient
dummy scans are implemented once to achieve the steady-state condition as the reference
point. T1-weighting preparation block
consists of an adiabatic inversion pulse and spoiler gradients followed with a
variable inversion time delay (TI). After the center-out SPGR acquisition, the steady-state
preparation block 2 is optional to make sure the steady-state SPGR condition is
fulfilled at the end of every inversion pulse cycle. These blocks are repeated Ny (number of 2D phase encoding) times like 3D MPRAGE
to produce one T1-weighted image.
The center-out SPGR sequence
in the slice direction (3D) phase encoding direction is used to sample the 3D
images.
Since the inversion time
is primarily defined by the center of k-space, the measured
signal $$$S$$$can be expressed by: $$ S = a + be^{-TI/T_{1}},$$ where $$$a = M_{0} sin(\theta)e^{-TI/T_{2}^{*}}$$$ and $$$b = -M_0(1+\frac{1-e^{-TR/T_1}}{1-cos(\theta)e^{-{TR}/T_1} } )sin(\theta)e^{-TI/T_{2}^{*}}$$$ with $$$M_{0}$$$ represents the thermal equilibrium
magnetization, $$$\theta$$$ is the flip angle. Three T1-weighted images are acquired
with different inversion times to estimate T1 using a reduced-dimension nonlinear least
square (RD-NLS)6 fit. Five water-containing tubes
(diameter 2.5 cm, height 10 cm) doped with Gdcl and agarose were used to perform phantom T1 mapping studies. All scans were performed at a
1.5 T scanner (Superscan-1.5 T, XGY Medical Equipment, Ningbo, China) with an 8-channel head coil. For the phantom experiments, IRSE
method was implemented as a T1 mapping reference: TR/TE = 1550/10 ms, slice
thickness = 4 mm, TI = [30 530 1030 1530] ms, with the resolution of 1.27×1.27 mm2. The scan time was 23.5
mins per slice. The parameters of the proposed method were: TR/TE = 5.8/2.5 ms,
TI = [6 686 1506] ms, with the resolution of 1.27×1.27×2.81 mm3. The scan time of the
proposed method was 9.1 mins. Two healthy volunteers (Male, Age: 26, 33) were
scanned by the proposed T1 protocol, with all parameters same as these used
in the phantom study. The study was approved by the local ethics committee, and written informed consent was obtained from both subjects.
Results
Figure 2 shows the
histograms of T1 maps obtained for 5 phantoms and Table 1
presents the corresponding T1 values. Linear regression analysis indicated that the T1 measurements from both methods are highly similar with a very small relative
difference (0.41% ± 0.58%, r=0.9999, P<1E-5). Figure 3 shows T1 maps of one
example slice for each subject with cerebrospinal fluid (CSF) filtered out. The
results from an ROI analysis on the two healthy subjects were shown in Table 2 compared with T1 values reported in the literature. Discussion
As demonstrated in the phantom experiments, the proposed method achieves similar
accuracy, but less precision compared with IRSE method. In
vivo brain analysis, T1 values of the white matter and grey matter
were found to be 674 ±
38 and 1209 ± 170 ms, which are in close agreement with the T1 values reported at 1.5 T7-10. Our method has two advantages over other
MPRAGE based T1 mapping methods. Prior knowledge of flip angle is not required
in our method compared with MP2RAGE, avoiding the additional B1 correction.
Compared with 3-TI MRRGAE, our method saves about 50% of the time because no recovery time
is needed for each inversion cycle. Preliminary results suggest that the
proposed method can achieve similar time efficiency as MP2RAGE, much faster
than 3-TI MPRAGE.Conclusion
In this study, we proposed an accelerated MPRAGE-based 3D T1 mapping method by using
SPGR steady state. Furthermore, we demonstrated the feasibility of the proposed
method in phantom and human experiments, which estimated T1 values comparable
to reported literature values.Acknowledgements
No acknowledgement found.
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