MATTHEW TARASEK1, Eric Fiveland1, Chitresh Bhushan1, Goutam Ghoshal2, Tamas Heffter2, Katie Gandomi3, Paulo Alberto Carvalho3, Christopher Nycz3, Teresa Maiette4, Zahabiya Campwala4, Erin Jeannotte4, Michael Staudt4, E Clif Burdette2, Gregory Fischer3, Julie Pilitsis4, and Desmond Yeo1
1GE Global Research, Niskayuna, NY, United States, 2Acoustic MedSystems Inc., Savoy, IL, United States, 3WPI, Worcester, MA, United States, 4Neurosurgery, Albany Medical College, Albany, NY, United States
Synopsis
In this work we evaluate a newly developed catheter-based therapeutic ultrasound (US) probe used for interstitial MR-guided high intensity focused US (iMRgFUS) procedures. Specifically, we optimize and down-select MR thermal imaging protocols in
order to achieve maximum temperature measurement precision and volume
coverage in the presence of image artifacts arising from the iMRgFUS probe
design and operation.
Purpose
Thermotherapy-based interventional technologies have
rapidly developed as means to treat several pathologies. Ablative therapies have
become especially useful in the treatment of movement disorders and brain
tumors.[1-3] These
procedures are typically monitored by magnetic resonance temperature imaging
(MRTI), using the proton resonance frequency (PRFS) method.[4] The PRFS method
is very sensitive to image phase artifacts, and therefore much care must be
given to ablation probe design to minimize susceptibility-induced image artifacts.
Interstitial MR-guided focused ultrasound (iMRgFUS) probes contain metal wires,
piezoelectric material and water flow lines for cooling, all of which have the
potential to cause drastic MRTI degradation. Here we (i) perform quantitative ΔB0,
SNR, B1+ phantom tests on a recently developed catheter based iMRgFUS probe [5]
in various orientations and power states, and (ii) perform phantom MRTI heating
validation tests at multiple sonication power levels using 4 different MRTI
sequences. The
goal of this work is to evaluate, optimize and down-select MRTI protocols in
order to achieve maximum temperature measurement precision and volume coverage in
the presence of image artifacts arising from the iMRgFUS probe design and
operation.Methods
Phantom
imaging tests were performed on a 3T GE Architect scanner (GE Healthcare,
Waukesha, WI). Body coil transmit was used with a single channel (15 cm ID)
loop coil for receive signal. Phantoms were 3% Agar solution doped with copper
sulfate to mimic the relaxivity of brain tissue at 3T. Two separate phantoms
were used for testing: one phantom containing only the probe in Agar as
depicted in Fig. 1 (phantom 1), and
one containing multiple fiber optic temperature probes for MRTI validation
testing seen in Fig. 3a (phantom 2). The
iMRgFUS probe (Acoustic Medsystems, Savoy, IL) was constructed with a multielement
10mm long tubular piezoelectric transducer mounted on a hollow polyimide
tubular structure. It was inserted into the Agar phantom as can be seen in Fig.
1a. Quantitative imaging tests were performed to assess (i) ΔB0,
(ii) B1+, and (iii) basic SNR tests using a gradient-echo (GRE) sequence. All
imaging tests were performed at 0°, 45°, and 90° orientations of the axis of
the catheter based therapeutic US probe with respect to the main magnetic field
(B0). Figs. 1c-d depicts the parallel (0°) and orthogonal (90°) orientation
examples. Phantom MRTI tests were performed using phantom 2 depicted in Fig. 3a with three fiber optic temperature
probes (Neoptix) distributed in-plane, at different radial distances from the
US transducer element. Four sequences were tested using the PRFS MRTI method: a
spoiled gradient echo (SPGR), echo-planar imaging -GRE, fast SPGR, and multi-echo fast-SPGR. The precision and accuracy of MRTI
measurements are defined as the standard deviation of the temperature
measurements averaged within a 20-pixel diameter region centered on the probe, and
the absolute difference between the temperature probe readings and the MRTI
reading at the T-probe locations respectively.Results and discussion
Phantom 1 was constructed with only the US probe and Agar in order to minimize
any potential confounding artifacts during ΔB0, SNR, B1+ measurements. These imaging measurements
were repeated with phantom 2, and no new
imaging artifacts were noted when the temperature probe was inserted. The
table in Fig. 2 summarizes the results of the orientation dependence study for phantom 1. The standard deviation of ΔB0 is
reduced by a factor of 2 in the parallel (0°) orientation. SNR likewise
increases within the 20-pixel diameter averaging region in the parallel
position, indicating that ΔB0 effects primarily contribute to MR signal
drop in the immediate vicinity of the US probe. B1+ maps remain largely
unchanged in the different orientations. The table in Fig. 3 indicates the
precision, accuracy, and maximum volume coverage in a 10 second window for the
multiple MRTI methods tested in phantom 2.
Overall, single-echo SPGR provided the highest temperature precision and
accuracy, although it performs worst in terms of volume coverage. Relative to
SPGR, EPI-GRE provides a factor of 3 increase for volumetric coverage yet
underperforms in terms of MRTI temperature precision and accuracy (over 40%
reduction). Fast-SPGR, and multi-echo fast-SPGR perform similarly well, and
give similar MRTI metrics with an approximate 2-fold increase in volumetric
coverage relative to SPGR.Acknowledgements
This
work was funded in part by NIH 2R01CA166379References
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