Gunther Helms1 and Hampus Olsson1
1Medical Radiation Physics, Clinical Sciences Lund, Lund University, Lund, Sweden
Synopsis
Fitting
the inversion recovery (IR) at multiple TI provides T1 estimates of high
accuracy if performed in a single slice with full relaxation. We present an isotropic
3D variant based on MP-RAGE, where a T1-weighted driven equilibrium is prepared
prior to inversion by a second RAGE readout. This abolishes the need for long
recovery times and provides volumes of similar contrast for co-registration.
The method was tested at 3T on a small cohort and compared to 3D IR-TSE and 3D
variable flip angle mapping.
Introduction
Fitting
the exponential inversion recovery (IR) at multiple TI at full relaxation provides T1 estimates of high
accuracy since this excludes bias by inhomogeneous B1+1. Since this is typically performed in a single slice and due to time requirements, this is mainly used to validate other T1 mapping methods. A driven equilibrium (DE) is reached much faster than M0 by relaxation, thus accelerating IR measurements when combined with non-equilibrium rapid acquisition of gradient echoes (RAGE). By using the second volume of MP2RAGE2 to establish a DE, isotropic three-dimensional (3D) IR fitting of T1 becomes possible.Theory
At
the n+1-th readout by flip angle α during RAGE at TR, Mz has converged on the DE at M0(1-exp(R1TR))/(1-exp(R1*TR)) by exp(-R1*nTR) = exp(-R1nTR)*cosnα, featuring a relaxation and a driving term3. While small α and small n partially maintain the dynamic range of the IR-prepared Mz, a large enough α are required to reach
the DE for a given turbo-factor. These conflicting demands can be met by exploiting the two read-out trains of MP2RAGE. Methods
Measurements were performed on a 3T MAGNETOM Prisma using a 20
channel head-neck coil (Siemens Healthcare, Erlangen, Germany) on informed
consenting healthy adults (3m/2f, 26-53years).
Sagittal non-selective volumes of 1.25 mm3 isotropic resolution
(FoV 240x232x180 mm3) were acquired using an MP2RAGE at TE/TR/α1/α2 =2.6/5.6ms/5°/20° while varying TI through 300ms, 600ms, 1000ms,
1600ms, 2500ms and 4000ms. The turbo-factor was 144. At 20°, Mz converges by more than 1% (for a typical lower B1+=75%). With 6/8
partial Fourier acquisition (n=48) and α1=5° more than 75% of the dynamic
range from IR-preparation are preserved (driving term only, at upper B1+=125%). The additional
time to establish DE was 850ms. Without delay between the second RAGE and the inversion,
the measurement time per volume was between 2:22 and 7:32 minutes. Volumes were
co-registered using the T1-w DE volumes. T1 was obtained by fitting an
exponential transition to the first MP-RAGE volumes. For comparison, T1 was also mapped at five variable flip angles (4°,
6°, 8°, 12° and 16° at constant B1= 8.16uT, TR = 10ms)4, corrected by the scanner's default
saturation recovery B1+ maps5 in one subject and by fully relaxed 2D IR-TSE in
another.Results
For
different TI, the first MP-RAGE volumes showed a strong dependence on TI (Figure 1). The similar contrast of the other volume (not shown) indicated convergence onto the
T1-weighted DE. Thus, Mz was positive even at the shortest TI. Fit to ROI
signals (Fig. 2) resulted in small residues with R close to 1 as typical for
IR. At TI=4000ms, the endpoint was attained only in white matter.
For
the standard locations in splenium, caudate and lateral ventricle, values obtained
from 3D MP-RAGE and 2D TSE agreed well: 866±44ms/870±51ms, 1337±52ms/1417±16ms
and 4179±1265ms/3858±317ms. Corresponding cohort means±SD from 3D MP-RAGE were 871±43ms, 1432±80ms, and 4294±171ms, respectively.
The
poorer definition of the endpoint with increasing T1 explains the loss of precision
as seen in the scatterplot (Fig. 3). This could be ameliorated by increase the longest TI value (and omitting some shorter TI). Here, VFA and DE-MP-RAGE yielded T1 of similar precision. Linear regression revealed a slight
underestimation of T1 by VFA (as explained by inverse magnetization transfer)6. Discussion
By
turning MP2RAGE into a DE-IR-prepared measurement, we obtained 3D T1 maps in
only slightly more time than by the (gold-)standard 2D IR-prepared TSE. This is
possible due to the RAGE readout and the preparation of DE taking less time than
restoring M0 by relaxation. This comes at a cost of reducing the dynamic range
of the IR-prepared state.
Details
of our implementation depended on the MR system’s MP2RAGE sequence, 20° being
the highest possible α2. Complete saturation of Mz can be
efficiently achieved by replacing RAGE by additional 90° pulses. Although α2
= 5° was the Ernst angle in GM, higher SNR may be achieved by increasing α1,
but at a cost of dynamic range.
The method is applicable at 7T (data not shown). The
DE-IR-prepared T1 maps are intended to serve as reference for 3D T1 mapping methods that may be subject to spatial bias, e.g. to validate the reduced B1+ sensitivity of T1 mapping by MP2RAGE.2 Conclusion
Preparing
a DE prior to inversion with an MP2RAGE sequence allows for isotropic T1 mapping of
the whole brain, thus providing a B1+-independent, IR-based T1 reference to validate T1 quantification methods. Acknowledgements
Funding
by the Swedish Research Council (NT-2014-6193) and support by Dr. F. Testud,
Siemens Healthcare Sweden, is gratefully acknowledged. References
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