Synopsis
The aim of this study was
to understand whether amide proton transfer (APT) contrast on brain tumor
patient will be impacted by applying three different imaging sequences, spin-echo EPI,
single-shot FSE, and a recent developed 3D FSE spiral. Although our finding on APT
contrast appears to be similar among various sequences, careful consideration may be required when choosing
the appropriate CEST readout sequences for your own applications.Purpose
Chemical
exchange saturation transfer (CEST) MRI can detect low-concentration compounds
with exchangeable protons via saturation transfer to water
1,2. One
of the CEST contrasts, amide proton transfer (APT), was developed to detect the
exchange of amide protons, which resonate at 3.5 ppm downfield from the bulk
water protons of endogenous mobile proteins and peptides in tissue. It has been successful applied to many pathological
studies such as stroke, tumor grading in clinical patient
3,4. Experimental
measurement of the APT effect is complex, and depends on not only amide proton
concentration and exchange rate, saturation scheme, but also possibly pulse sequence
readout. A variety of imaging sequences have been used for detecting APT effect,
including echo planar imaging (EPI), fast spin-echo (FSE), and gradient echo
5.
To date, many studies have been conducted on the design and optimization of saturation
scheme. However, little literature is available on the effects of varied readout
sequences. In this study, three imaging sequences, spin-echo EPI (seEPI),
single-shot FSE (ssFSE), and a recent developed 3D FSE spiral (3Dspiral), were
employed for comparing APT effect and imaging quality on tumor patients.
Material & Methods
MRI acquisition was performed on a 3T clinical scanner
(Discovery MR750, GE Healthcare, Milwaukee, USA) using a 32-channel brain coil
as the signal detection and whole body coil for RF transmission. APT imaging were
acquired with three different pulse sequences (seEPI, ssFSE, 3Dspiral) with
identical TR (2.5 s) and saturation scheme. The parameters for saturation
scheme were as follows: saturation pulse= 400 ms × 4 fermi pulses, B
1=1.5 μT, 37
saturation frequencies with S
sat(w) (0, ±25, ±50, ±75, ±100, ±150,
±200, ±250, ±300, ±350, ±375, ±400, ±425, ±450, ±475, ±500, ±525, ±550, ±600 Hz),
and 2 S
0 (without saturation pulse). The imaging parameters were as
follow: FOV= 22 cm; matrix size=128×128; slice thickness=5 mm; and TE=25.3 ms,
30.24 ms, and 10.1 ms for seEPI, ssFSE, and 3Dspiral, respectively. In the data
analysis, the APT effect was quantified using the magnetization transfer ratio
asymmetry (MTRasym) at 3.5 ppm with respect to the water resonance as
the formula of (S
sat(-3.5ppm)-S
sat(+3.5ppm))/S
0
with pixel-by-pixel B
0 correction.
Result & discussion
Gd-enhancing T1-weighted
image (T1WI) and APT images generated by three pulse sequences in brain tumor
patient with cavernous hemangioma were shown in Fig. 1. Enhanced signal on
post-contrast T1WI is observed (Fig. 1a), implying the tumor location is in suprasellar
cistern with extension to the basal ganglion and thalamic region. Hyperintense signal
was noted on APT imaging (Fig. 1b-d) within Gd-enhancing tumor area,
suggesting increased content of protein and peptides. APT images generated by 2D
seEPI (Fig. 1b) and ssFSE (Fig. 1c) appear to be similar, while APT image showed
the blurring in 3Dspiral (Fig. 1d). For acquiring APT data on whole brain with
reasonable acquisition time (6 min with 39 saturation frequencies in this case), the spiral arm was reduced for 3Dspiral
acquisition and consequently, low resolution APT image was found at 3Dspiral. Z-spectrum
and MTR
asym within tumor area and gray matter were shown in
Fig. 2. Z-spectrum was found to be slightly broader at seEPI (Fig.2). The possible
reason is that seEPI could involve longer readout and means the chemical
exchange duration is prolonged. More exchangeable saturated protons, including
MT pool and amide proton, could exchange with bulk water during the whole EPI readout,
thus slightly broadening the Z-spectrum. APT quantitative values among the sequences
within tumor area (Fig. 2a) are slightly varied (4.6%, 5.2%, and 3.7% for
ssFSE, seEPI, and 3Dspiral, respectively) but more consistent at gray matter
region (Fig. 2b).
Conclusion
We have demonstrated that varied readout sequences with
the same saturation scheme showed the similar APT and Z-spectrum. Careful
consideration may be required when choosing the appropriate CEST readout
sequences for your own applications
5, though it appears like among
various sequences readout. For example, although FSE-based CEST sequence produces
exquisite images with less sensitive to field inhomogeneity and may be suitable
to neck region for detecting nasopharyngeal carcinoma in comparison with EPI,
the additional refocusing pulses can create concerns of energy deposit on
clinical scanners. When considering doing whole brain study with voxel-based
analysis, 3Dspiral would be good candidate since limited slice number are
acquired at 2D sequence due to possible saturation inference on neighboring
slices.
Acknowledgements
No acknowledgement found.References
1. J. Zhou, et al., PNMRS, 48:109-136, 2006.
2. P. van Zijl et al., MRM, 65:927-948, 2011.
3. A. Tietze, et al., NMR in Biomed, 27:163–174, 2014.
4. O. Togao, et al., Neuro-Oncology, 16(3): 441-448, 2014.
5. G. Liu, et al., NMR in Biomed, 26:810-828, 2013.