Synopsis
In this presentation the audience will be guided through the theory and applications of Arterial Spin Labeling MRI in an interactive manner. Emphasis will be put on the pitfalls of the acquisition, post-processing and interpretation of perfusion measurements by ASL.Introduction
Arterial
spin labeling (ASL) MRI is based upon inversion (or saturation) of the
magnetization of arterial blood in the neck region (see Figure 1)
1. After a delay-time of
approximately 1.5-2 seconds, to allow the blood to travel to the brain tissue,
a proton-density weighted scan is made: the label image. Subsequently the same
procedure is repeated, but without inverting the inflowing blood: the control
image. Subtraction of the label from the control image will cancel out signal
from static tissue, leaving only the signal from the labeled spins, i.e. the
blood that has flown into the brain tissue.
Acquisition
Traditionally,
two different types of ASL are recognized: pulsed ASL that labels a large
region below the imaging slices with a short (≈15 ms) inversion module and (pseudo-)continuous
ASL that labels for a longer time (≈2 s) all blood that flows through an
inversion plane. In the consensus paper of 2015, pseudo-continuous ASL (pCASL)
was designated as workhorse technique for ASL imaging
4,5. Main reasons for favoring this
implementation of ASL are the easy implementation on clinical MR scanners, easy
quantification because of the well-defined temporal width of the labeling
bolus, the higher SNR due to the continuous approach, and the easy post-processing/interpretation
of the data. Throughout this abstract and presentation, pCASL will be the
assumed method except when explicitly stated otherwise. Relatively recently, a
third category of ASL (spatially non-selective (SNS) ASL) was proposed with
velocity selective ASL being the most-applied example
6,7. In SNS-ASL, labeling is not performed
below the imaging slice, but based on the flow properties of blood by means of
motion-sensitizing gradients. This results also in creation of label within the
imaging volume and thus much closer to the tissue, thereby shortening the time
for the label to travel towards their end destination in tissue.
Quantification
Important
for understanding the quantification of ASL is the fact that the non-invasively
created tracer (the labeled blood) are in fact the water-molecules in blood,
which both quickly exchange magnetization between blood plasma and blood cells,
as well as between the intra- and extravascular compartment in brain tissue at
the capillary level2,3. The tracer employed in ASL is therefore
not only an endogenous, but also an (almost) freely diffusible tracer (i.e.
when arriving in the microvasculature the magnetization will almost immediately
exchange with the extravascular compartment). This provides the basis for the
quantification approach: after creating a bolus of labeled spins with a
pre-determined temporal width, the label will be transported to the supplied
brain tissue, extravasate into the tissue and accumulate (for the largest
part) in the brain tissue until it will be detected, i.e. the local cerebral
blood flow is proportional to the amount of label accumulated in a voxel. Three
main processes need to be taken into account when quantifying the blood flow:
1. The efficiency of labeling: pCASL does provide on average a
high labeling efficiency, but the labeling efficiency can be affected by the
velocity of the blood and B0-inhomogeneities resulting in low or
even negative signal on the CBF-maps. Normally, a constant labeling efficiency
is taken into account as obtained from simulation studies of the ideal
situation. This will of course not correct for artefactual low labeling
efficiency, due to for example off-resonance effects. Solutions that have been
proposed include the measurement of the blood velocity by quantitative phase
contrast MRI and using this as input to the simulations8, by equating the total cerebral
blood flow to a reference flow measurement9, or by direct measurement of the
labeling efficiency in a separate scan10. When no further corrections are
employed, it is at least essential to realize when interpreting pCASL-scans
that sub-optimal labeling might have occurred.
2.
Decay of the label: Labeling is performed by inversion of the magnetization and therefore
label will be lost via longitudinal relaxation processes. Because of the
relatively long time between labeling and detection of the label in the brain
tissue (typically longer than 2 seconds), one needs to correct the detected
signal for the T1-relaxation of the label during this delay-time. Since
the label will be located for the longest time in arterial blood, the consensus
paper proposed to assume that the label was exclusively located in blood and
therefore only to correct with the T1 of blood (approximately 1.65 s
at 3 Tesla). However, several factors can influence the T1 of blood
with main magnetic field strength, hematocrit and oxygenation as the three most
important factors11,12. Hematocrit is known to be
different between males and females and in several diseases changes in
hematocrit have been reported. When observing differences in quantitative
ASL-values between two groups of subjects, it is therefore important to
consider whether differences in hematocrit (and thus T1 of blood)
might explain the observed differences or that a difference in CBF is a more
likely explanation. Secondly, in most subjects the label will at some point in
time (approximately 1.5 – 2.0 s after labeling) move from the intra- to the
extravascular compartment and from that time onward the label will relax
quicker, i.e. with the T1 of tissue (approximately 1.2 s).
Differences in the time that it takes for the label to travel through the
vascular tree and to exchange magnetization with the extravascular compartment,
might therefore also introduce differences in observed ASL-signal.
3. Normalization of ASL-signal: MRI is traditionally a qualitative
imaging modality, and the obtained signal after subtracting label from control
images, needs therefore to be calibrated. In principle, calibration should be
performed to the magnetization of a voxel containing pure arterial blood, i.e.
the maximum ASL-signal that could be observed. In practice such a voxel is not
available and it has therefore been proposed to use a minimum contrast reference
scan obtained with the same readout parameters as the ASL scan, but a TR of 2-4
s4. The use of a reference image
instead of a signal value, opens-up the possibility to perform a voxel-wise
normalization of the signal-intensity that will also correct for most signal-variations
due to local differences in T2(*) or coil sensitivities.
Artefacts
Two main artefacts
should be expected when working with ASL13. The first is the occurrence of
motion artefacts, which do result in strong artefacts because ASL is a
subtraction technique. Motion correction in post-processing can alleviate some
of the artefacts, but typically one would still see some ringing around the
brain when the subject moved a lot. Optical tracking and prospective motion
correction techniques have been proposed as solutions to minimize motion
sensitivity. Moreover, probably an equally important solution is the use of
background suppression in the ASL-sequence, which was also included in the
consensus statement as part of the suggested standard implementation of ASL. By
lowering the signal intensity in the brain tissue, the effect of a mismatch in
static brain tissue after motion is lowered, thereby improving image quality.
The second
important artefact is known under the names “transit time artefacts” or “vascular
artefacts” (see Figure 2). These artefacts occur in subjects with delayed blood
flow, resulting in the presence of label in the major arteries during readout
of the signal instead of the label being present in the microvasculature or
brain tissue. This is a violation of the assumption that all labeled blood has
arrived in the brain tissue and will lead to an underestimation of the
tissue-perfusion and hyperintense signal within the arteries. One solution to
avoid such artefacts is to prolong the delay-time between the end of labeling
and the readout (i.e. increased post-labeling delay time (PLD)), but this will
automatically decrease the SNR of the resulting ASL-image, since the label will
have had more time to relax than for a shorter PLD. Whereas one could also use
flow-crushers to get rid of the signal in the large vessels, this would also
obscure information, i.e. the fact that label could have been observed in the
large arteries, tells us that label was still on its way to feed the brain
tissue and tells us to take this into account in our interpretation of the ASL
scan. One should therefore refrain of interpreting an ASL-scan just as an perfusion
scan, but keep reminding oneself that one is looking at an “ASL-scan” of which
transit time artefacts are an important indicator of impaired large vessel
transport.
Aim of the presentation
The
audience will be taken in an interactive way through the acquisition,
post-processing and interpretation of ASL scans. Many examples will be
discussed.
Acknowledgements
-References
1.
Detre JA, Leigh JS, Williams DS,
Koretsky AP. Perfusion imaging. Magn Reson Med 1992;23(1):37-45.
2.
Parkes LM, Tofts PS. Improved accuracy
of human cerebral blood perfusion measurements using arterial spin labeling:
accounting for capillary water permeability. Magn Reson Med 2002;48(1):27-41.
3.
Zhou J, Wilson DA, Ulatowski JA,
Traystman RJ, Van Zijl PC. Two-compartment exchange model for perfusion quantification using arterial
spin tagging. J Cereb Blood Flow Metab 2001;21(4):440-455.
4.
Alsop DC, Detre JA, Golay X, Gunther M,
Hendrikse J, Hernandez-Garcia L, Lu H, MacIntosh BJ, Parkes LM, Smits M, van
Osch MJ, Wang DJ, Wong EC, Zaharchuk G. Recommended implementation of arterial
spin-labeled perfusion MRI for clinical applications: A consensus of the ISMRM
perfusion study group and the European consortium for ASL in dementia. Magn
Reson Med 2015;73(1):102-116.
5.
Dai W, Garcia D, de BC, Alsop DC.
Continuous flow-driven inversion for arterial spin labeling using pulsed radio
frequency and gradient fields. Magn Reson Med 2008;60(6):1488-1497.
6.
Wong EC, Cronin M, Wu WC, Inglis B,
Frank LR, Liu TT. Velocity-selective arterial spin labeling. Magn Reson Med
2006;55(6):1334-1341.
7.
Schmid S, Ghariq E, Teeuwisse WM, Webb
A, van Osch MJ. Acceleration-selective arterial spin labeling. Magn Reson Med
2014;71(1):191-199.
8. Gevers
S, Nederveen AJ, Fijnvandraat K, van den Berg SM, van OP, Heijtel DF, Heijboer
H, Nederkoorn PJ, Engelen M, van Osch MJ, Majoie CB. Arterial spin labeling measurement of cerebral
perfusion in children with sickle cell disease. J Magn Reson Imaging
2012;35(4):779-787.
9.
Aslan S, Xu F, Wang PL, Uh J, Yezhuvath
US, van OM, Lu H. Estimation of labeling efficiency in pseudocontinuous
arterial spin labeling. Magn Reson Med 2010;63(3):765-771.
10.
Chen Z, Zhang X, Webb AG, Zhao X, and Van Osch MJ. A novel method to estimate
labeling efficiency for pseudo-continuous arterial spin labeling imaging. 2015.
2953.
11.
Hales PW, Kirkham FJ, Clark CA. A
general model to calculate the spin-lattice (T1) relaxation time of blood,
accounting for haematocrit, oxygen saturation and magnetic field strength. J Cereb Blood Flow Metab
2016;36(2):370-374.
12.
Zhang X, Petersen ET, Ghariq E, De Vis
JB, Webb AG, Teeuwisse WM, Hendrikse J, van Osch MJ. In vivo blood T(1) measurements at 1.5 T, 3 T, and 7 T.
Magn Reson Med 2012.
13.
Grade M, Hernandez Tamames JA, Pizzini
FB, Achten E, Golay X, Smits M. A neuroradiologist's guide to arterial spin
labeling MRI in clinical practice. Neuroradiology 2015;57(12):1181-1202.