Jianxun Qu1, Tianye Lin1,2, Priti Balchandani3, M. Dylan Tisdall1, and John A. Detre1,4
1Radiology, Perelman School of Medicine, University of Pennsylvania, Philadelphia, PA, United States, 2Chinese Academy of Medical Sciences, Peking Union Medical College, PUMCH, Beijing, China, 3Icahn School of Medicine at Mount Sinai, New York, NY, United States, 4Neurology, Perelman School of Medicine, University of Pennsylvania, Philadelphia, PA, United States
Synopsis
Inflow blood during the
post labeling delay is a significant source of physiological noise in arterial
spin labeling. This study utilized a novel inflow saturation method to address
this issue. Compared to traditional inflow saturation approach where a 90o
thick saturation slab is used to null blood within the interval of background
suppression inversion pulses, the proposed method employs serial of thin slab
sub-bolus saturations, with the saturation strength planned adaptively to
return the blood to nulling point at the excitation point. The proposed method
reduces the inflow artifacts markedly and mitigates global signal fluctuations.
Introduction
Inflow of unlabeled
blood during post labeling delay (PLD) is a significant source of physiological
noise in continuous arterial spin labeled (ASL) perfusion MRI. Although cardiac
gating can reduce inflow fluctuations1, it requires extra
preparations and lengthens acquisition time. Vessel suppression is an
alternative strategy, but it introduces T2 weighting and reduces SNR2.
Inferior saturation bands are typically used to suppress inflowing blood. In
background suppressed (BS) 3D ASL, an inflow saturation band is typically inserted
between BS inversion pulses to suppress inflowing blood after the labeled bolus.
With the help of inversion pulses, longitudinal relaxation then returns
saturated blood to the nulling point at the initial excitation pulse of the
image acquisition (Fig.1a). In ideal circumstances, a single thick inferior
saturation band should suppress all signal from inflowing blood. However, due
to RF field inhomogeneity, the optimal saturation region is often more limited,
compromising the saturation module’s efficacy. In this work, we replace the
thick saturation band with serial thinner saturation bands to achieve more
robust inflow saturation. The saturation RF strength of sub-bolus saturation
bands is adjusted independently to match the recovery curve of blood in an
ideal situation.Method
Figure.1
illustrates sequences without saturation, with standard thick slab saturation,
and with the improved serial saturation for comparison. The labeling duration
and PLD were 1.8s, following the consensus paper2. Two slice
selective inversion pulses, placed at 493ms, and 1771ms before the acquisition,
are used for background suppression, achieving a moderate suppression
efficiency of 90%. In the standard approach, the inferior saturation band was
placed at 700 ms before the last inversion pulse. For the serial saturation
approach, two and three saturation modules are evenly placed within the
interval of saturation to inversion and inversion to acquisition. The
saturation slab thickness for the traditional approach was 250mm, while for the
serial saturation approach, the saturation thickness was 120mm, chosen to
optimally saturate blood with a mean velocity of 50 cm/s. Parameter details for
inflow saturation are shown in Fig.1a. The acquisition utilized a single-shot
accelerated 3D stack-of-spirals fast spin echo (SoS-FSE) readout with the
following parameters: FOV 240mm, 40 slices, isotropic resolution 3.75 mm, and
rate-2 GRAPPA acceleration in the Kz direction3. ASL measurements
were performed on two healthy volunteers with: 1) no inflow saturation; 2)
traditional saturation; and 3) proposed serial saturation on a 3T whole-body
system (MAGNETOM Prisma, Siemens Healthcare, Erlangen, Germany). In total,
thirty interleaved phases of labeling and control were acquired for each inflow
saturation approach. The M0 normalized standard deviation (SD) of perfusion-weighted
(PW) images were calculated for comparison. Results
Figure 2a illustrates
the normalized standard deviation map for each subject. Fig2b plots the average
value of the SD within the brain parenchyma. For both subjects, the SD is high
for measurements without inflow saturation, which is most prominent in regions
around the middle cerebral arteries (MCA, white arrows) and anterior cerebral
arteries (ACA, orange arrows). The standard saturation approach reduced these
artifacts, but with the serial saturation approach, signal fluctuation around
MCA and ACA were further suppressed. Neither approach effectively attenuated
signal fluctuations in CSF (blue arrows). Global signal fluctuations were also
reduced (Fig 2b). For the first subject, the average SD dropped from 0.155 to
0.149 (4.1%) and 0.140 (9.5%) for standard and serial approaches, respectively.
For subject two, the average SD dropped from 0.228 to 0.201 (11.8%) and
0.179(21.5%) for standard and serial approaches, respectively. Conclusions
Inflow artifacts in
BS 3D ASL artifacts are incompletely attenuated by single slab inflow
saturation, while the serial saturation approach completely eliminated
conspicuous inflow artifacts in the MCA and ACA regions. This approach is more
straightforward and more time-efficient compared to the cardiac-gated method.
In designing the sub-bolus saturation band thickness, the sequence assumed a mean
blood velocity of 50 cm/s, whereas in instances where proximal flow velocity
deviates from this value, there remains a chance of compromised saturation or
potentially double saturation. The tolerance to both fast and slow flow is not
addressed in the current study and waits to be explored later. There exists a
difference in the fluctuation reduction rate for the two subjects, which might
be a result of varying hemodynamics, such as arterial transit time. The
proposed method could also be extended to BS planning involving more than two
inversion pulses. Additional evaluation of saturation efficiency tolerance to
serial slab saturation number and thickness across the inflow velocity values
will be explored in future work.Acknowledgements
This
work was supported by NIH grant P41 EB015893References
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