Chien-Yuan Eddy Lin1,2, Jianxun Qu2, Ai-Chi Chen1, Yen-Chien Wu3, David Yen-Ting Chen3, Ying-Chi Tseng3, and Chi-Jen Chen3
1GE Healthcare, Taipei, Taiwan, 2GE Healthcare MR Research China, Beijing, People's Republic of China, 3Department of Radiology, Taipei Medical University - Shuang Ho Hospital, New Taipei City, Taiwan
Synopsis
Pseudo-continuous arterial spin labeling (pCASL) has
been recently used for investigating cerebral hemodynamic change on the patient
receiving carotid artery stenting (CAS) because it permits repeated measurement
of absolute cerebral blood flow in a short interval without MR contrast agent
or radioactive material. However, labeling efficiency of pCASL has been proved
to be dependent on B0 and B1 inhomogeneity. The aim of
this study was to understand how inhomogeneous of the B0 and B1
at labeling position of pCASL and find the remedies of the pCASL measurement for
the CAS patient.
Purpose
Carotid
artery stenting (CAS) is being increasingly used as an alternative treatment to carotid
endarterectomy for carotid
artery stenosis1. Variable imaging modalities have been applied to
investigate cerebral hemodynamic change after CAS2. However, it remains unclear which hemodynamic changes
occur in certain areas of the brain following CAS. Pseudo-continuous arterial spin labelling (pCASL) is an emerging MRI method for
studying cerebral perfusion using radiofrequency (RF) pulses for the noninvasive labeling of endogenous water protons in the blood3 instead of injecting
exogenous contrast agent or radioactive material. This technique is capable of
detecting absolute cerebral blood flow (CBF) at the brain tissue level (ml/100g per minute) permits repeated measurement of CBF in a short interval, which is useful in patients
receiving CAS4. However, the
labeling process of pCASL is not strictly an adiabatic inversion and the
labeling efficiency may be dependent on B0 and B1 inhomogeneity
or other factors5, which are especially concerns for CAS patient. The
aim of this study was to understand how heterogeneous of B0 and B1
field caused by stent at labeling region of pCASL and find the solution without
compromising the pCASL measurement in the CAS patients.Methods
Ten patients with symptomatic internal carotid artery
stenosis receiving CAS were included in the study. Two stent types (Boston
Wallstent® and Cordis Precise®) were
used in these CAS treatment patients. All MRI acquisitions were performed on a
3T clinical scanner (Discovery MR750, GE Healthcare) using an 8-channel brain
coil as signal detection and whole body coil for RF excitation. Perfusion study
was conducted using a pCASL with a TR=5327 ms, an TE=10.5 ms, FOV=24×24 cm, labeling duration=1.5 s, post labelling
delay=2525 ms, matrix=128×128,
NEX=2, slice thickness =4
mm. In addition, labelling plane was 3.35-mm thick and placed at 2.18 cm inferior to the lower edge of the scanning coverage. The
CBF maps were generated on an Advantage Windows workstation
(version 9.4, GE Healthcare). For identifying stent position, time-of-flight magnetic
resonance angiography (TOF-MRA) was acquired. Coronal B0 map of
the tagging region was acquired by two gradient echo images with a TE
difference of 1.5 ms, while B1 map was acquired by gradient echo
Bloch-Siegert sequence with a TR of 19 ms, an TE of 12.8 ms, a matrix of 128×128, and a pair of Fermi pulses (8 ms duration)
having off-resonace +/-4 kHz6. To determine the optimal labeling position, the
distance between stent and labeling plane was varied to be 2.5, 3, 3.25, 3.5, 4
cm.Results
Stent position can be identified
by coronal gradient-echo images with hypointensity (Fig. 1a). B0 and
normalized B1 maps were shown in Fig. 1b and Fig. 1c, respectively.
Quantitative measurement of B0 and B1 value at each
patient was summarized at Tab. 1. Part of data was excluded due to the bad
quality from motion or other reason. B0 field at stent region
appeared rather inhomogeneous according to the B0 map and its quantitative
data with high standard deviation, ranging from ±53 to ±212 Hz. B1 measurement by acquiring the
Block-Siegert phase shift between two scans is independent of B0. Normalized
B1 was calculated by a ratio of actual nominal flip angle (Fig. 1c
and Tab. 1) and it is found to be higher than desired (140%) on stenting side
and close to actual flip angle (101%) on contralateral side. The estimated CBF
map (Fig. 2) showed the lower CBF at ipsilateral hemisphere and back to normal compared
to contralateral side as the labeling position of pCASL away from stent.
CBF-cut-off distance (Tab.1) suggested that the CBF recovered to normal level at
3.25 cm of the distance between stent and labeling position.Discussion and Conclusion
Noncontrast pCASL
method is very useful for evaluating cerebral hemodynamic change on the patient
after CAS. However, prominent frequency incoherence and B1
inhomogeneity due to the presence of stent (Fig. 1 and Tab. 1) would substantial
reduce the labeling efficiency and thus cause quantification error for pCASL if
the labeling plane at or close to the stent position. The quantification error
caused by the combination of B0 and B1 inhomogeneity
could not be easily compensated. Alternatively, we demonstrated that perfusion
signal would not be compromised when labeling position is 3.25 cm away from
stent position (Tab. 1 and Fig. 2). It is advised that the distance may vary
with different type of stent materials7. Nonetheless, once the optimal
labeling distance has been determined in the first time of pCASL experiment for
the material, the same acquisition condition can be applied to CAS patient with
the same stent.Acknowledgements
No acknowledgement found.References
1.
Brott TG, Hobson 2nd RW, Howard G, et al., “Stenting versus endarterectomy for
treatment of carotid-artery stenosis,” N Engl J Med, 363(1):11-23, 2010
2.
Chang TY, Liu HL, Lee TH, et al., “Change in cerebral perfusion after carotid angioplasty
with stenting is related to cerebral vasoreactivity: a study using dynamic
susceptibility-weighted contrast-enhanced MR imaging and functional MR imaging
with a breath-holding paradigm,” AJNR Am J Neuroradiol, 30:1330–1336, 2009.
3. Wang JJ, Alsop DC, Li L, et al., “Comparison of quantitative
perfusion imaging using arterial spin labelling at 1.5 and 4.0 tesla,” Magn
Reson Med, 48(2):242-54, 2002
4. Chen YT, et al., “Loss of labelling efficiency caused by carotid
stent in pseudocontinuous arterial spin labelling perfusion study,” Clinical
Radiology, 71:e21-e27, 2016.
5. Jahanian H, et al., “B0 field inhomogeneity considerations in pseudo-continuous
arterial spin labeling (pCASL): effects on tagging efficiency and correction
strategy,” NMR in Biomed, 24:
1202–1209, 2011
6.
Sacolick L, et al., “ B1 Mapping by Bloch-Siegert Shift,” Magn Reson Med, 63(5):1315-22,
2010.
7. Lin CY, et al., “Experimentally optimizing
labeling position in pseudo-continuous ASL in the presence of carotid artery
stenting,” The proceeding of ISMRM, p4111, 2016