Yuanyu Shen1, Gang Xiao2, Zhiwei Shen1, Xiaolei Zhang1, Wei Hu1, Xiangyong Tang1, Zhiyan Zhang1, Jitian Guan1, and Renhua Wu1
12nd Affilicated Hospital, Shantou University Medical College, Shantou, China, People's Republic of, 2Hanshan Normal University, Chaozhou, China, People's Republic of
Synopsis
Our aim was to demonstrate
the feasibility of nuclear Overhauser enhancement (NOE) imaging to detect the
characteristic of patients with brain tumors. Six healthy volunteers and eleven
patients with brain tumors were recruited for undergoing MRI scan at 3T. As a
result, we found NOE value was greater in white matter compared to gray matter.
However, in human brain tumors, NOE value was slightly hypointense in glioma
and little difference in meningioma. NOE imaging may help to distinguish the
heterogeneity of benign or malignant tumors, and it is important in diagnosis
and treatment planning for patients with brain tumors.Background
Chemical exchange saturation transfer (CEST) is a type of
magnetization transfer (MT) which employs the saturation transfer from low
concentration endogenous and exogenous pools of exchangeable protons to the
bulk water proton pool. There have two CEST effects apparent in vivo which are
attributed to protons of mobile proteins: amide proton transfer (APT) and nuclear
Overhauser enhancement (NOE). The NOE signals originate from
mobile macromolecular components with a spectral range upfield
relative to water. Glioma and meningioma, as the most common malignant and
benignant tumors in human brain, which imaging diagnosis and the boundary
description are significant to clinical treatment. NOE has been attributed to increased mobile protein
concentrations in malignant cells. In
our study, we evaluated the difference between glioma and meningioma in NOE
signals to explore whether NOE* imaging can identify the
differentiation of benign and malignant in human brain tumor.
Methods
All MR imaging was acquired on a 3T MR imaging
system. CE-T1 weighted images were performed. In addition, MT-prepared
GRE MRI sequence was used for CEST imaging. The MT saturation pulse
was chosen as a 20 ms width Fermi pulse with B1 of 0.6 μT.
Forty-nine equidistant frequency offsets between 6 and -6 ppm and the
additional S0 image were acquired. Z-spectra were corrected for B0
inhomogeneity employing a water saturation shift referencing map (WASSR).
Images
were processed using the Matlab. Z-spectra were calculated from the normalized
images for ROI. For NOE image mapping, three offset frequencies were selected:
one at the center frequency of the NOE* peak, while the other two were
at the upper and lower bounds of the peak. In addition to the S0 was
the signal intensity without irradiation. Then NOE map can be
obtained as equation: NOE*=S{[(-2.5ppm)+S(-5ppm)]/2-S(-3.5ppm)}/S0.
Results
Eleven patients with recently diagnosed and histopathologically
confirmed brain tumors and six normal controls were included in this
prospective study.
Fig.
1A is a T2WI of brain from a healthy volunteer. To quantitatively
compare the NOE effect in the human brain, regions of interest (ROI) were
analyzed. The ROIs enclosing the white matter and the gray matter were
carefully drawn on the T2WI images. The average z-spectrums were
drawn in Fig. 1B at B1 = 0.6 μT. Both white matter and gray matter
showed a board peak at -2.5 ppm to -5 ppm due to NOE effect.
Figure
2A-D show a patient with a grade-III astrocytoma in the left temporal
lobe. In this case, the tumor core signal is enhanced area in the
Gd-enhanced T1-weighted image (Fig. 2A). In Fig. 2B, we can observe
that the tumor core is hyperintense while the NOE* is hypointense.
In Fig. 2C and 2D, the average Z-spectrum and a linear fitting of date points were
measured from tumor and contralateral normal-appearing white matter (CNAWM). We
observed a drop in NOE signal strength (about 0.3 %) at -2.5 ppm to -5 ppm in
tumor core region.
Figure
2E-H show an example of a patient who had a pathologically proven transitional
meningioma in the right parietal lobe. The tumor core, as identified by the
signal enhancement in the post-contrast T1WI images (Fig. 3E). In
the Fig. 3F, we can see there is no significant difference between tumor core
and CNAWM in the NOE* image. However, we also can obtain the similar
results in the average Z-spectrum and a linear fitting of date points was
measured with the tumor core and CNAWM regions (Fig. 3G and H). NOE*%
is not significantly different between the tumor and CNAWM.
NOE*
contrast at -3.5 ppm was different in two types of human brain tumors, when we
compared tumor core with CNAWM. Results demonstrated a positive NOE*%
at -3.5ppm in glioma (p <
0.001) but an insignificant NOE*%
in meningioma (p = 0.112).
Conclusions
We
investigated NOE signals in healthy human brain and human brain tumors at 3T. The
NOE signals (-2.5 ~ -5 ppm) were found to peak around the B
1 of 0.6 μT,
and were more abundant in the white matter than in the gray matter. However, in
human brain tumors, we found that NOE signals were attenuated in glioma and not
in meningioma. These findings may have implication for future NOE studies in
the human brain tumors in clinical application. NOE imaging may help to
distinguish the heterogeneity of benign or malignant tumors, and these
capabilities of NOE imaging may be very important in diagnosis and treatment
planning for patients with brain tumors.
Acknowledgements
This work was supported
in part by the National Natural Science Foundation of China (Grant No.
81471730), the National High Technology Research and Development Program (863
Program) of China (Program No. 2014AA021101).References
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