Lukas Mario Gottwald1, Rainer Schneider1, and Josef Pfeuffer1
1MR Application Development, Siemens Healthcare, Erlangen, Germany
Synopsis
In clinical 3T imaging,
gradient-echo-based sequences often suffer from signal loss induced by patient-specific susceptibility artifacts. To tackle this problem, a proposed local
signal recovery z-shim method using parallel transmission was implemented for a
clinical setup. The approach was further extended by an automated slice-specific delay-time calculation to ensure user-friendly operation as well
as maximal signal gain in artifact regions. Studies in humans were carried out
using commonly used GRE and EPI sequences. Signals could be nearly fully recovered
in artifact regions; tSNR gain maps for EPI time series showed an increase up
to 148%.Purpose
At higher field strengths (3T and
above), T2*-weighted images acquired with gradient-echo (GRE)-based sequences,
e.g. FLASH, SWI and BOLD EPI, are often impaired by local signal loss induced
by susceptibility effects. In the human brain, these artifacts typically appear
near the orbital frontal and inferior temporal cortex and affect the imaging of
brain activity with fMRI or the diagnosis of diseases, e.g. stroke or
hemorrhage. The effect worsens with increasing echo time (TE) and slice thickness,
and is often dominated by the through-plane signal loss. Proposed methods (1,
2) mitigate through-plane dephasing using parallel transmission without
increasing scan time or changing the slice coverage.
In this work, we implemented the
pTX z-shim including B1 inhomogeneity correction (2) on a clinical 3T scanner
equipped with two whole-body transmit channels. Furthermore, slice-specific
delay-times were calculated automatically inline to ensure user-friendly
operation as well as maximal signal gain in artifact
regions. Finally, human studies were performed to demonstrate the potential
benefit for clinical GRE and fMRI imaging.
Methods
To summarize the methods (1, 2), the
excitation pulse is applied on separate transmit channels with a time shift to
impose a linear “prewinding” phase to compensate the phase cancellation induced
by the through-plane susceptibility. Our prototype sequences included an inline
pTX pulse optimization (2) to mitigate the B1 inhomogeneity.
Five human subjects were studied on
a 3T MAGNETOM Skyra (Siemens Healthcare, Erlangen, Germany) using prototype gradient-echo
(FLASH) and EPI-based sequences with image resolutions of 0.7x0.7x6 mm3
and 1.7x1.7x6 mm3, respectively. Studies with standard RF excitation
pulses (reference) were compared to slice-specific pTX z-shim pulses, which
were calculated fully automatically from inline B0 and B1 maps and designed for
maximal signal gain in artifact regions.
For both gradient-echo and EPI images,
difference images (corrected vs. reference) were calculated in % of the
reference mean intensity. Temporal-signal-to-noise ratio (tSNR) maps were
generated from EPI time series of 100 repetitions (ratio of the mean signal
intensity to the standard deviation of the noise: $$$ tSNR =\overline{S}_{d}/\sigma_{N}
$$$). tSNR provides information on the detection ability for fMRI and is particularly
suitable to highlight the benefit for fMRI applications. In all series, noise regions
were masked and time series were detrended voxelwise by a second-order
polynomial. To evaluate the actual signal or tSNR gain, respectively, artifact
regions-of-interest (ROI) were defined in affected slices, and mean or maximum values
were calculated.
Results and Discussion
Exemplary signal gain in FLASH studies
is shown in Fig. 1. Some image slices acquired with the standard excitation
pulse suffered from strong subject-induced susceptibility artifacts (left) in
the frontal orbital and temporal cortex. Commonly, only few slices were affected
(e.g. slices 7-11 of 20) and corrected by the pTX z-shim, and the rest remained untouched.
In contrast, images with a slice-specific correction showed significantly signal
gain in artifact regions at the cost of global SNR penalty. Difference images (right)
revealed that a gain relative to the reference mean could be achieved up to 102%
in the areas suffering from through-plane susceptibility. Fig. 2 summarizes the
signal gain in GRE studies for all subjects. On average over all subjects, the
frontal (temporal) orbital cortex had a maximal signal gain of 88+-13% (74+-21%)
and a mean signal gain of 31+-11% (31+-12%).
Exemplary signal gain in
gradient-echo EPI time series is shown in Fig. 3. A similar signal recovery in
artifact regions compared to GRE could be achieved. In addition, tSNR maps from
EPI time series (Fig. 4) show a remarkable increase with the pTX z-shim. A mean
tSNR increase up to 121% in artifact regions can be seen from difference maps. Fig.
4 summarizes the tSNR gain for all subjects. On average, the frontal (temporal)
orbital cortex had a mean tSNR gain of 88+-38% (86+-43%).
In the slices with signal and
tSNR gains in artifact regions (ROI), a reduced SNR and fMRI detection power is
visible outside the ROI (unaffected areas). In order to be able to adapt
gains/losses for specific application protocols, an additional user factor to
scale the pTX z-shim correction was implemented (data not shown).
Conclusion
The proposed method and
implementation on a clinical scanner enables an easy-to-use and automated compensation for slices with local signal loss induced by susceptibility
effects. Moreover, significant tSNR gain could be achieved in susceptibility-induced artifact regions in fMRI image series. Hence, this application is of
high interest to enhance the visualization of brain activity and the diagnosis of
diseases in former dark artifact regions.
Acknowledgements
N/AReferences
[1] Deng, W., Yang, C., Alagappan, V., Wald, L. L., Boada, F. E., & Stenger, V. A. (2009). Simultaneous z-shim method for reducing susceptibility artifacts with multiple transmitters. Magnetic Resonance in Medicine, 61(2), 255-259.
[2] Schneider, R., Ritter, D., Haueisen, J., & Pfeuffer, J. (2014). B0-informed variable density trajectory design for enhanced correction of off-resonance effects in parallel transmission. Magnetic Resonance in Medicine, 71(4), 1381-1393.