Natsuko Onishi1, Masako Kataoka1, Shotaro Kanao1, Mami Iima1, Makiko Kawai1, Akane Ohashi1, Katsutoshi Murata2, Benjamin Schmitt3, and Kaori Togashi1
1Dept of Diagnostic Imaging and Nuclear Medicine, Kyoto University Graduate School of Medicine, Kyoto, Japan, 2Research & Collaboration Dpt., Siemens Japan K.K., Tokyo, Japan, 3Healthcare Sector, Siemens Ltd, Melbourne, Australia
Synopsis
Amide proton transfer (APT) imaging is the representative endogenous
chemical exchange saturation transfer (CEST) imaging that has been applied to
some clinical cancer studies. However, little is known about the clinical
usefulness of APT imaging in breast cancer. In this study, 3T MRI studies
including APT imaging were performed for 24 breast cancer lesions, and the possible
utility of APT imaging in evaluating biochemical information induced by breast
cancer was demonstrated. APT CEST imaging is a potentially useful MRI technique
for breast cancer.Purpose
Chemical exchange saturation transfer (CEST) MRI is a novel
molecular MRI technique that can detect subtle chemical changes by detecting
interactions of protons between metabolite and bulk water. Amide proton
transfer (APT) imaging is the representative endogenous CEST imaging that has
been applied to some clinical cancer studies. Especially in brain, previous
reports have demonstrated the usefulness of APT imaging in tumor detection and
characterization(1-3). However,
little is known about the clinical usefulness of APT imaging in breast cancer. The
aim of this study were to determine the possible utility of amide proton
transfer (APT) MR imaging in breast cancer.
Methods
Approval for this study was obtained from
the Institutional Review Board of our institution, and informed consent was
waived due to retrospective study design. Twenty-three female patients with
pathologically confirmed invasive breast cancer underwent breast MRI. All
examination was performed at a 3T scanner (MAGNETOM Trio, A Tim System,
Siemens
GmbH) with 16ch breast coil. Axial bilateral breast APT CEST imaging were
obtained using a
proto-type 3D gradient-echo pulse sequence with the following settings: TR/TE,
6.3/1.78ms; Flip angle, 12°; voxel size, 1.8×1.8×3.0mm3; 16slices.
Pre-saturation pulses consisted of 5 consecutive RF pulses of 99-ms duration
with 60-ms inter-pulse delays and 1.2 μT time-average amplitude. First,
baseline images were acquired without pre-saturation pulse (S0 image). And
then, images with pre-saturation pulses at different offsets (0, ±0.6, ±1.2,
±1.8, ±2.4, ±3.0, ±3.6, ±4.2, and ±4.8 ppm) from the bulk water resonance were
acquired (SSat). Selective
excitation of water was used to avoid signal from lipid resonance. Total
scan time was 4min 49s.
The asymmetry of the magnetization transfer
rate (MTRasym) at 3.5ppm (APTasym) was calculated by integration of the
attenuated signal (SSat) between +3.2 and +3.8 ppm and subtracting
that from the integrated SSat between –3.2 and –3.8 ppm, normalized
against S0. SSat(Δω) was obtained after interpolation
of the originally
sampled points to a resolution of 0.05 ppm and subsequent correction for inhomogeneity of the static
magnetic field by Z-spectrum shifting similar to a previously described method by Schmitt et al (4).
Obtained APTasym maps (APT images) were evaluated in comparison with
B0 (to rule out uncorrectable
confounding B0 inhomogeneities post shimming), dynamic
contrast-enhanced (DCE) T1-weighted, T2-weighted and T1-weighted images. Tumor
size was determined using DCE T1-weighted images. One lesion without DCE
T1-weighted images was evaluated using diffusion-weighted images instead.
Results
In total, 23 patients with 46 breasts were investigated and 24
cancer lesions were identified. In APT images, no lesions presented
intratumoral hyperintensity compared with normal breast tissue and 6 lesions
presented hyperintensity in peritumoral breast tissue (named peritumoral
hyperintensity; PT-HI) compared with contralateral breast tissue. Two representative
cases of PT-HI are shown in Fig 1 and 2a. Fig 2a&b shows the disappearance of PT-HI
through neoadjuvant chemotherapy (NAC). Table
1 shows the characteristics
of all lesions, lesions with PT-HI (PT-HI group) and lesions without PT-HI (non
PT-HI group).
Discussion & Conclusion
It
is noteworthy that no breast cancer lesions presented
intratumoral hyperintensity, which was different from previous reports in brain
tumors demonstrating intratumoral hyperintensity compared with normal tissue. For
now, we are not sure what contribute to the difference, but the difference in
amide concentration and tissue physicochemical properties (pH and temperature)
between breast cancer and brain tumors may exist. Also, PT-HI in breast cancer has not been
reported before, as far as we know. Considering the disappearance of PT-HI through NAC treatment demonstrated in Fig 2a&b, we speculate PT-HI may reflect the
change in microenvironment induced by cancer (e.g., interstitial protein
accumulation, lymph stasis), though our data didn’t indicate the specific
characteristics to PT-HI group. Further studies in larger number of lesions are
needed.
We demonstrated a pilot study of APT imaging of breast cancer. Providing biochemical information non-invasively, APT CEST
imaging is a potentially useful MRI technique for breast cancer.
Acknowledgements
This work was supported by JSPS KAKENHI Grant Number 15K09921.References
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