Guruprasad Krishnamoorthy1,2, Jacinta Browne2, Aiming Lu2, David A. Woodrum2, and James G. Pipe2
1MR R&D, Philips Healthcare, Rochester, MN, United States, 2Department of Radiology, Mayo Clinic College of Medicine and Science, Rochester, MN, United States
Synopsis
Keywords: New Trajectories & Spatial Encoding Methods, Thermometry
This study assessed the
feasibility of thermometry of frozen tissue during MRI-guided cryoablation at
1.5T using a novel 3D spiral staircase UTE sequence (SSCUTE). MRI data using the
SSCUTE sequence were continuously acquired along with temperature measurements
during several freeze-thaw cycles in ex-vivo porcine specimens. A calibration
curve was obtained using temperature measurements and corresponding MRI data. MRI-estimated
temperature maps were generated with high accuracy using the calibration curve
on a validation dataset. Our work demonstrated the feasibility of thermometry
of frozen tissue using SSCUTE sequence at 1.5T, which could be an essential
step in clinical adoption of this technique.
Introduction
MRI-guided percutaneous cryoablation
is a promising technique for treating lesions in the prostate, liver, and other
body sites1-3. Standard T1/T2-weighted sequences are used to
visualize the edge of frozen tissue (< 0⁰C), commonly referred to as an iceball6.
However, the iceball itself does not represent the lethal ablation margin (<
-20⁰C). Therefore, non-invasive thermometry inside the iceball is clinically desired
to ensure treatment efficacy. Using ultrashort echo time (UTE) sequences, recent studies have demonstrated thermometry of frozen tissue at 0.5T and 3T7-11.
This study investigates the feasibility of thermometry of frozen tissue at 1.5T
using a novel 3D spiral staircase UTE sequence. Methods
Imaging sequence: The
proposed 3D spiral staircase UTE (SSCUTE) is based on a spiral staircase
trajectory12 modified to achieve UTE by adapting a variable-duration
slice encoding similar to the acquisition weighted stack-of-spiral technique
(AWSOS)13. SSCUTE has several advantages: 1) high sampling & SNR
efficiency due to spiral readout along the Kxy axis; 2) adaptability
to anisotropic FOV and resolution; and 3) an in-coherent through-plane aliasing
artifact pattern. The latter is beneficial in minimizing through-plane aliasing
artifacts caused by the short RF pulses typical in UTE sequences. Figure 1a
shows the pulse sequence diagram of the proposed SSCUTE method, and Figure 1b
compares AWSOS and SSCUTE trajectories. Phantom images were acquired to compare
the through-plane aliasing artifact pattern of AWSOS and SSCUTE sequences using
identical sequence parameters and RF pulse, as detailed below.
Cryoablation experiment: Two
ex-vivo porcine muscle specimens (A&B) procured from different vendors were
used to perform four experiments (two experiments on each specimen). In each
experiment, an MR-compatible cryoneedle (Visual-ICE, Boston Scientific, USA)
was inserted into the ex-vivo specimens at room temperature. Four fiber-optic
sensors (OSENSA, Canada) were inserted at different distances from the tip of
the cryoneedle for temperature reference. A baseline dataset was acquired at
room temperature before cryoablation. And two freeze-thaw cycles of 15:00 mins were
performed, during which MRI data at a clinical 1.5T Ingenia scanner (Philips,
The Netherlands) were dynamically acquired with interleaved multi-echo SSCUTE
sequence. The sequence parameters are: TE1, TE2, TE3/TR = 160, 220,
600µs/3.4msec (TE as inner loop); Flip angle = 9⁰; Acq. FOV/voxel = 325 x 325 x
140mm3/1.7 x 1.7 x 6mm3; spiral readout duration =
0.68msec; Volume selective excitation; Scan orientation = Axial; Temporal
resolution = 60sec. The image
reconstruction was performed immediately on the scanner using a gridding and inline
temperature map generation algorithms implemented in Recon 2.0 (Philips, The Netherlands).
MRI data of the following three methods were correlated with the temperature
measurements from the sensors: 1) Magnitude of TE1 normalized to the baseline TE1
magnitude (Normalized uteMag); 2) T2* map computed by the exponential fitting
of TE1, TE2, and TE3 data (T2*); and 3) T2* normalized to the baseline T2*
(Normalized T2*). A calibration curve was obtained by fitting the data points
below -5⁰C to an exponential function. The obtained fit was validated on a
separate validation set to estimate temperature, and statistical analysis was
performed to determine the accuracy of the results.Results and Disucssion
Phantom images obtained with AWSOS
and SSCUTE are compared in Figure 2. SSCUTE visibly minimized the through-plane
aliasing artifacts caused by the imperfect excitation profile of the short RF
pulse used in this study. In the ex-vivo experiments, the average T2* obtained
with SSCUTE from the baseline scans in porcine specimens A and B differed
substantially (3.57±9.3 vs. 8.29±15.96). Figure 3 shows the MR images
obtained with SSCUTE during a freeze-thaw cycle from specimen A along with the
temperature measurements from sensors and MRI measurements from ROIs drawn
around the sensors. All three methods (Normalized uteMag, T2*, and Normalized
T2*) exhibited a similar trend as the temperature measurements in both
specimens, while the T2* and Normalized T2* measurements were noisier for
temperatures > -10 ⁰C. Figure
4a show plots of MRI measurements as a function of temperature. T2* showed
large deviations between the two specimens, even in sub-zero temperatures, which
differed from the previous work9. However, Normalized
uteMag and Normalized T2* decayed similarly in both specimens, resulting in a
calibration curve with a high correlation coefficient (R2 ~0.9). Figure
4b show plots of MRI estimated temperature as a function of the measured
temperature. While the Normalized uteMag and Normalized T2* methods exhibited
good agreement between the estimated and measured temperature, the Normalized
uteMag method may be preferred because it requires only one-third of the scan
time required by the Normalized T2* method. A plot of the measured and the MRI
estimated temperature, along with overlayed temperature maps using Normalized
uteMag, is shown in Figure 5. Conclusion
The feasibility of thermometry of
frozen tissue at 1.5T using the SSCUTE sequence is demonstrated. Based on the preliminary
results, thermometry with a 20-30 sec temporal resolution can be achieved using
the Normalized uteMag method. The accuracy of the proposed method needs to be
evaluated invivo on patients.Acknowledgements
No acknowledgement found.References
1. Morrison,
P.R., Silverman, S.G., Tuncali, K. and Tatli, S. (2008), MRI-guided
cryotherapy. J. Magn. Reson. Imaging, 27: 410-420. https://doi.org/10.1002/jmri.21260
2. Woodrum
DA, Kawashima A, Karnes RJ, et al. Magnetic resonance imaging-guided
cryoablation of recurrent prostate cancer after radical prostatectomy: initial
single institution experience. Urology. 2013;82(4):870-875.
doi:10.1016/j.urology.2013.06.011
3. Welch
BT, Ehman EC, VanBuren WM, et al. Percutaneous cryoablation of abdominal wall
endometriosis: the Mayo Clinic approach. Abdom Radiol (NY).
2020;45(6):1813-1817. doi:10.1007/s00261-019-02379-4
4. Baust, J.G. and Gage, A.A. (2005), The
molecular basis of cryosurgery. BJU International, 95: 1187-1191. https://doi.org/10.1111/j.1464-410X.2005.05502.x
5. Gage
AA, Baust J. Mechanisms of tissue injury in cryosurgery. Cryobiology.
1998;37(3):171-186. doi:10.1006/cryo.1998.2115
6. Tacke, J., Adam, G., Haage, P., Sellhaus, B.,
Großkortenhaus, S. and Günther, R.W. (2001), MR-guided percutaneous cryotherapy
of the liver: In vivo evaluation with histologic correlation in an animal
model. J. Magn. Reson. Imaging, 13: 50-56. https://doi.org/10.1002/1522-2586(200101)13:1<50::AID-JMRI1008>3.0.CO;2-A
7. Butts, K., Sinclair, J., Daniel, B.L.,
Wansapura, J. and Pauly, J.M. (2001), Temperature quantitation and mapping of
frozen tissue. J. Magn. Reson. Imaging, 13: 99-104. https://doi.org/10.1002/1522-2586(200101)13:1<99::AID-JMRI1015>3.0.CO;2-O
8. Wansapura JP, Daniel BL, Vigen KK, Butts K. In
vivo MR thermometry of frozen tissue using R2* and signal intensity. Acad
Radiol. 2005;12(9):1080-1084. doi:10.1016/j.acra.2005.06.006
9. Kaye
EA, Josan S, Lu A, Rosenberg J, Daniel BL, Pauly KB. Consistency of signal
intensity and T2* in frozen ex vivo heart muscle, kidney, and liver tissue. J
Magn Reson Imaging. 2010 Mar;31(3):719-24. doi: 10.1002/jmri.22029. PMID:
20187218; PMCID: PMC2832094.
10. Overduin, C.G., Fütterer, J.J. and Scheenen,
T.W. (2016), 3D MR thermometry of frozen tissue: Feasibility and accuracy
during cryoablation at 3T. J. Magn. Reson. Imaging, 44: 1572-1579. https://doi.org/10.1002/jmri.25301
11. Tokuda
J, Wang Q, Tuncali K, Seethamraju RT, Tempany CM, Schmidt EJ. Temperature-Sensitive
Frozen-Tissue Imaging for Cryoablation Monitoring Using STIR-UTE MRI. Invest
Radiol. 2020 May;55(5):310-317. doi: 10.1097/RLI.0000000000000642. PMID:
31977600; PMCID: PMC7145748.
12. Anderson AG 3rd, Wang D, Pipe JG. Controlled
aliasing for improved parallel imaging with a 3D spiral staircase
trajectory. Magn Reson Med. 2020;84(2):866-872.
doi:10.1002/mrm.28154
13. Qian, Y. and Boada, F.E. (2008),
Acquisition-weighted stack of spirals for fast high-resolution
three-dimensional ultra-short echo time MR imaging. Magn. Reson. Med., 60:
135-145. https://doi.org/10.1002/mrm.21620