Deb Rivera1,2,3, IML van Kalleveen3, Catalina Arteaga de Castro4, Hanneke Laarhoven3, Dennis Klomp1,4, Wybe van der Kemp4, Jaap Stoker3, and Aart Nederveen3
1MR Coils BV, Zaltbommel, Netherlands, 2Spinoza Centre, Amsterdam, Netherlands, 3Academic Medical Center, Amsterdam (AMC), Amsterdam, Netherlands, 4University Medical Center Utrecht (UMCU), Utrecht, Netherlands
Synopsis
At 7T 31P spectroscopy becomes possible on clinically relevant scales. Here
we tackle the greatest challenge in multi-parametric imaging at high-field –
creating localizers and radiological-grade images in the body in the absence of
a bore body coil. By using antennas rather than loop coils, we image the full
extent of the liver (n=10). Combining antennas with parallel transmit, allows
radiological-grade images. Although technically feasible, it is not yet
possible to obtain multi-nuclear spectra and parallel transmit images within
the same scan session. We combine the methods by rebooting the scanner mid-exam,
and demonstrate the method can be used for imaging patients.
Introduction
Phosphorus spectroscopy is a marker for treatment response in hepatic cancers,1,2 and at 7 Tesla clinically-relevant
spatial resolutions (<18mL) and time scales (<30min) become feasible,
allowing differentiation of relevant metabolites and clinical treatment-response
tracking.3 There is no body coil in the bore of the 7T, nor receive loops in the bed. At 7T (~300MHz) collecting a radiological-grade
anatomical image of the liver presents a challenge due to poor penetration depth4 and destructive interference.5 Although incapable of imaging even half of the liver at
300MHz, surface coils are the state-of-the-art for acquiring anatomical (1H)
images for phosphorous spectroscopy, High field 31P spectroscopy in the liver has
been limited to diffuse disease.6,7 Antennas enable improved
penetration depths at 300MHz,8 and when combined with parallel
transmit enable body imaging at 7T (Fig.1). Although technologically feasible, combination of multinuclear spectroscopy (non-proton) and
parallel transmit is not yet available on commercial 7T scanners. This results
in general in poor coverage of the liver. Here we present the use of antennas to improve penetration depth for multi-nuclear spectroscopy, as an improvement over loops for obtaining localizers, and demonstrate the need for the combination of parallel transmit with phosphorus
spectroscopy for ultra-high field multi-parametric imaging of hepatic cancers.Methods
A custom-made liver coil (MR
Coils BV, Zaltbommel) consisting of 8 30-cm dipole antennas tuned to the
proton (298MHz) frequency, and 2 loops (20cm diameter) tuned for 31P (120MHz) were used to transmit
and receive signal. The pairs of elements were combined with a fixed
phase of 90-degrees (quad-hybrid). For power optimization for 31P, we swept the
flip-angle to identify the maximum signal intensity in a phantom and adapted
for a volunteer (maxB1=30μT). Adiabatic pulses were used (adiabatic half-passage with a tanh/tan shape,
2ms pulse duration, and maximum frequency modulation of 5kHz), thus we did not
further optimize the transmit power for the multi-nuclear experiment.
Similarly, the optimal power level was found and written into the coil file for
the proton antennas (maxB1=10μT). Spectra voxels were selected from 3DiCSI and Hamming
filtered, uploaded into JMRUI and filtered with a 40Hz Lorentzian, zero filled
to double the number of points, zero-order phase corrected to maximize the
closest non-split peak to the phospholipid metabolites, and 1st order (0.4ms)
phase corrected.Results
Penetration depth of a single antenna exceeds 20 cm, as
shown in a large phantom (Fig.2). Two antennas with fixed-phase allow the
liver to be visualized in vivo (Fig.3). Aggregate data compare penetration depth (n=9) with liver depth (n=5) for each direction, with A/P penetration approximately equal to liver depth (Fig.3). The liver and full axial slice of the
abdomen can be visualized with 8-transmit/receive antennas (Fig.1). Parallel
transmit with 8-antennas allows for B1-shimming to overcome black-band image
voids (Fig.4). Fig.5 shows results from a patient with 31P MRS projected onto a
DIXON image (same scan parameters as Fig.1). Discussion and conclusions
We have developed a protocol for
imaging hepatic cancer patients using parallel transmit and 31P spectroscopy
sequentially at 7T. The field of view afforded by two antennas is sufficient to
image the boundaries of the liver for CSI planning and region-of-interest-based
B0 shimming for the 31P experiment. With such a setup it is possible to locate
tumors anywhere within the liver in order to optimally position the imaging
matrix of 3D CSI. Additionally, the 2-antennas allow for alignment with
anatomical images collected using parallel transmit. Once 31P
data is acquired using the standard (dual-channel/multi-nuclear) mode of the scanner, the system must be rebooted and changed to parallel-transmit mode for anatomical imaging
using B1+ shimming. To our knowledge,
7T 31P studies have been limited to diffuse liver disease using loops for 1H
imaging with partial coverage of the liver (<50%) and penetration depths of 10cm.6,7
We have demonstrated that with antennas we can achieve nearly full coverage of
the liver, facilitating tumor localization and region-of-interest B0 shimming. The
31P protocol can be improved by B1 calibration, improved penetration depth, T1-saturation
correction (or longer TR), use of a BIR4 adiabatic pulse for uniform phase
across the bandwidth, and acquisition methods to improve SNR (e.g.9,6).
Hardware improvements include the use of a 31P birdcage and an array of 31P receive
coils.10 With the commercially available 7T platforms, it is not
possible to collect multinuclear (non-proton) data and anatomical images using
parallel transmit without rebooting the system. The implications of adapting
treatments to patients with a virtual-biopsy for hepatic cancers using full-radiological
grade images and multi-parametric imaging (31P, DWI), warrants adapting the
commercially available 7T scanner systems to meet the clinical needs. Acknowledgements
Thank you to the Spinoza Centre, Michel Italiaander, and the engineers and staff at MR Coils.References
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