Sina Straub1, Mark E. Ladd1,2, Paul Chang3, and Sahar Nassirpour3
1Division of Medical Physics in Radiology, German Cancer Research Center (DKFZ), Heidelberg, Germany, 2Faculty of Physics and Astronomy, Faculty of Medicine, University of Heidelberg, Heidelberg, Germany, 3MR Shim GmbH, Reutlingen, Germany
Synopsis
A 14-channel local array of shim coils
was used to improve B0 homogeneity and reduce artifacts in quantitative
susceptibility mapping at 7T. Using the local array of shim coils in addition
to the standard 2nd order spherical harmonic shims, the B0 shim quality was
improved by an average of 16% across all volunteers. Local inhomogeneities
were significantly reduced and could be correlated to reduced artifacts in
QSM.
Introduction
Quantitative susceptibility
mapping strongly benefits form ultra-high field MRI due to the higher available
signal-to-noise ratio allowing for higher resolutions and the larger phase
effects providing better contrast-to-noise ratios1. However, also
local B0 field inhomogeneities can become too steep to be
accounted for during pre-processing of the used gradient echo phase data
leading to artifacts in susceptibility maps. Arrays of small local shim coils have been used in multiple
MRI applications to reduce B0 inhomogeneity, since they provide
more flexibility over spherical harmonics2,3. As of yet, to the
best of our knowledge, this method has not been used in QSM. Therefore, in this study, we
investigate improving the B0 shim quality for brain QSM at 7T using
a 14-channel local array of shim coils.Methods
Data acquisition
Data were acquired in accordance
with the Declaration of Helsinki from three healthy volunteers (mean age
28.0±7.5 years, one female) who provided written informed consent at a 7 Tesla
whole-body system (Magnetom 7 Tesla, Siemens Healthineers) with a
8Tx/32Rx-channel head coil (Nova Medical Inc., Wakefield, MA, USA) using an
in-house-constructed butler matrix.
B0 shimming with a
local array of shim coils was performed using the system provided by MR Shim
GmbH (Reutlingen, Germany) which included: 14 channel local array of shim coils
(Elara) driven by shim amplifiers (Jupiter) with maximum currents of +/-
2.5 A per channel connected directly to the control PC over Ethernet.
Reference field maps for each
shim channel were acquired on a standard Siemens phantom by applying 1.5A to
each coil and acquiring a 2D dual-echo gradient echo (GRE) B0 field
map (sequence parameters Table 1).
For QSM, three-dimensional
multi-echo GRE sequences were acquired with the sequence parameters given in
Table 1 using two different shim settings: 1) with 2nd order scanner-only B0
shimming, and 2) with 2nd order and local shim coil B0 shimming.
Data processing and evaluation
Single-channel data were combined
on the scanner using the computationally efficient combination of multi-channel
phase data from multi-echo acquisitions (ASPIRE)4, and each echo was unwrapped with Laplacian-based phase
unwrapping5-7. For background field removal a
brain mask was generated with FSL Brain Extraction Tool8 on each echo of the gradient echo
data. Background field removal was performed with the variable-kernel
sophisticated harmonic artifact reduction for phase data (V-SHARP)6,7 method with kernel size up to 12 mm, and all
echoes were averaged9. The susceptibility maps were
calculated from local phase data using the streaking artifact reduction for QSM
(STAR-QSM) algorithm10.
As subjects had moved between
measurements, data was registered to the scan for which the local shimming was
performed using FSL-FLIRT11. A small region of interest, in which artifacts were
visible in QSM, was drawn for each volunteer using Medical Imaging Interaction
Toolkit (MITK)12,13 and mean as well as standard deviations were
calculated.Results
The RMS of the shim currents for
the local shim coils were: 1.1A, 1.25A and 1.7A, for Subjects 1, 2 and 3,
respectively. The standard deviation of the frequency shifts was 36.65 Hz/ 29.59 Hz for scanner shim only/ for local
shimming for Subject 1, 33.82 Hz/ 27.51 Hz for Subject 2, and 40.55 Hz/ 36.50
Hz, respectively for Subject 3.
Figure 1 shows that for all volunteers, histograms of the
frequency are broader for the scanner-only shim compared to when the local B0
shimming was used.
In Figure 2, representative sagittal (Volunteers 1 and 3)/ axial
(Volunteer 2) slices of
susceptibility maps as well as field map/ susceptibility map overlays are
shown. Strong field inhomogeneities can be observed above the sphenoidal sinus
(arrow heads) which are mitigated by the applied local shim. For Volunteer 3,
for which a smaller slab was acquired, inhomogeneities are more severe. In QSM,
artifacts (arrow heads) in the vicinity of these local field inhomogeneities
can be observed such as artificially bright regions. This is also depicted in
the quantitative results provided in Table 2, e.g. standard
deviation of susceptibility values in the depicted region decreases as well as
in Volunteer 3, the susceptibility itself is 33% lower.Discussion
It has been shown that some of
the most severe artifacts regularly observed in QSM can be mitigated with improved B0
shimming using a local
array of shim coils. In future, it should be highly beneficial to not
only use static local shimming but dynamic shimming. Real-time shimming has
already been shown to compensate for respiration induced B0
fluctuations and to improve the image quality of gradient echo data14.Acknowledgements
Authors Sahar Nassirpour and Paul Chang
are employees of MR Shim GmbH.References
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