Ute Goerke1, Eze Ahanonu2, Mahesh Keerthivasan3, Ali Bilgin2,4,5, Vibhas Deshpande6, and Maria Altbach4,5
1Siemens Healthcare USA, Tucson, AZ, United States, 2Department of Electrical Engineering, University of Arizona, Tucson, AZ, United States, 3Siemens Healthineers USA, New York, NY, United States, 4Department of Biomedical Engineering, University of Arizona, Tucson, AZ, United States, 5Department of Medical Imaging, University of Arizona, Tucson, AZ, United States, 6Siemens Healthineers USA, Austin, TX, United States
Synopsis
In the inversion-recovery Look-Locker T1-mapping, the
use of slice-selective inversion recovery pulse is explored to map the long
T1-values of the spleen with as many slices as possible. The optimal slice gap
in combination with interleaving the slices was determined. Artifact-free
T1-maps of the spleen were obtained after parameter optimization with double
the number of slices than using the standard approach in a single breath-hold. This
new approach is an important step towards achieving complete coverage of
abdominal organs within a single breath-hold.
Introduction
The measurement of T1 in the abdomen plays a role in
the characterization of chronic liver disease1, kidney function2,
mild chronic pancreatitis3, and tumor malignancy4, 5.
Cartesian MOLLI is used in the clinic for cardiac and
abdominal T1 mapping due to its robustness to B1 and capability of T1 mapping
within a breath-hold. However, MOLLI is slice inefficient, typically yielding
one slice per breath-hold, and T1 mapping is based on a limited number of TIs. Recently,
a radial Look-Locker (LL) technique was proposed for rapid T1 mapping of the
abdomen taking advantage of the undersampling properties6 of radial
MRI. This rapid technique only requires 2-3 seconds per slice opening the
possibility of improving slice efficiency within a breath-hold.
The LL pulse sequence is typically performed with a non-selective
inversion-recovery (IR) pulse. To avoid T1-saturation effects, a wait time is needed
which reduces the number of slices acquired in a breath-hold. In this work, we
explore the use of a slice-selective IR pulse to maximize the number of slices
within a breath-hold while maintaining T1-mapping accuracy through the slices. Methods
The LL T1 mapping sequence (Fig. 1) consists of an IR-pulse
followed by a series of radial GRE readouts sampling the IR-curve. For each
slice, this module is repeated after wait time WT. The IR-pulse can
be slice-selective (ss) or non-selective (ns). To ensure optimal inversion, the
slice thickness of the IR-pulse is set to 200% of the α-pulse nominal slice
thickness.
Phantom experiments were performed on 2% agarose NiCl2
(0.28, 0.74, 1.19, 2.1mM)7 vials to modulate T1. Experiment 1 was
designed to assess the effect WT and slice gap on T1 estimation when
using a ssIR pulse. Experiment 2 was designed to compare nsIR and ssIR T1-mapping
based on results from experiment 1. The
following acquisition schemes were used in experiment 2 using a slice gap 50%,
with interleaved slice acqusition: “ssIR, WT=100ms” “nsIR, WT=2s”,
“nsIR, WT=4s”. T1-values were calculated from voxels within the four
vials.
For abdominal T1-mapping, five subjects were consented
according to the IRB regulations of the University of Arizona. The same imaging
parameters as in phantom experiment 2 were used. In addition, data were
acquired with “nsIR, WT=100ms”.
All experiments were performed at 3T (Magnetom Skyra,
Siemens Healthcare, Erlangen, Germany) with FOV=40cm, readout points=256, slice
thickness (α-pulse)=6mm, TE=1.7ms, TR=5ms, α=10°, radial views per slice=640.
Images were reconstructed using the local low rank
algorithm8 by grouping 16 radial views per TI set yielding 40 TI
images along the 2.8s recovery curve (temporal resolution=80ms). T1 fitting was
performed using the ABT1-model9.Results and Discussion
In phantom experiment 1, the effect of T1-saturation from
the ssIR-pulse was investigated by choosing two slices (Fig. 2a) and varying slice
gap and WT between them. Fig. 2b displays the relative T1-error for
various T1-values. T1-error increases with shorter WT with T1-values
becoming stable at slice gaps≥200% even for the longest T1s indicating cross
talk between ssIR-pulses. From
this experiment, we concluded that a “ssIR, WT=100ms” parameter set -
for highest slice duty cycle, that is, minimal WT - required a 50%
gap given an odd/even slice interleaving scheme.
Fig. 3 shows phantom T1-maps for (a) “nsIR, WT=2s”,
(b) “nsIR, WT=4s’’, and (c) “ssIR, WT=100ms”. For “nsIR, WT
= 2s” the vial with longest T1 (vial “1”) shows T1-attenuation with increasing
slice number; the T1-error relative to the reference slice is shown in Fig. 3d.
This T1-saturation effect is reduced when WT=4s at the expense of reduced
number of slices within a breath-hold (Fig. 3b). T1-values obtained with “ssIR,
WT=100ms” remain constant across slices (Fig. 3c) and 6 slices can
be acquired in one breath-hold compared to three slices with “nsIR, WT=4s’’
(Fig. 3b).
A similar experiment was performed in vivo for abdominal
data (Fig. 4). In this experiment we also added a “nsIR, WT=100” acquisition
as a direct comparison to the slice efficient “ssIR, WT=100” (Fig.
4c). The effect of T1-saturation in the spleen (arrow), an organ with T1-value
of ~1.3s, is seen in slices after the first acquired slice for “nsIR, WT=2s”
and “nsIR, WT=100ms”. In contrast, the T1-maps for the “nsIR, WT=4s”
and the “ssIR, WT=100ms” are not deteriorated. The advantage of “ssIR,
WT=100ms” is the 50% increase in slice efficiency. Another advantage
of using a ssIR-pulse is that signal from blood vessels appears dark in the
T1-maps due to flow (while these appear bright in the nsIR T1-maps). This reduces
the confounding vessel effect when assessing anatomy (e.g., focal liver lesions).
To test reproducibility the imaging scans were
repeated for all subjects after re-running the calibration scans. The correlation
plot for liver and spleen ROIs from T1-maps for the optimized “ssIR, WT=100ms”
is displayed in Fig. 5. The coefficient-of-variation is 4.1%.Conclusion
A ssIR-pulse allows to minimize the WT and
therefore doubles the number of slices per breath-hold in a T1-mapping
experiment. Attenuation-free T1-maps are obtained with an optimized slice gap
and slice interleaving, an important step towards efficient coverage of
abdominal organs within a single breath-hold.Acknowledgements
The authors would like to acknowledge the support by NIH (R01CA245920), the Arizona Biomedical Research Commission (CTR056039), and the Technology and Research Initiative Fund (TRIF) Improving Health Initiative.References
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