Synopsis
This teaching presentation will attempt to demonstrate the power and existing present limitations of Chemical Exchange Saturation Transfer (CEST)-based MRI and its most prominent applications.Highlights
·
Chemical Exchange Saturation Transfer: The
physical/chemical effect and how to measure it
·
Endogenous contrasts and applications
·
Exogenous contrasts and applications
TARGET AUDIENCE
Researchers, clinicians and basic scientists, who want to learn about
this very versatile new technology.
OUTCOME/OBJECTIVES
Upon completion of this course, participants
should be able to:
· Get a glimpse of fundamental concepts and
methods used in CEST MRI
· Learn about the state-of-the-art applications, and
the ones closest to ‘clinical practice’.
· Understand the power of potentially important new contrast agents and
the challenges necessary to bring those to the clinics.
PURPOSE
What is Chemical Exchange Saturation Transfer? What are its boundary
conditions and its limits? The purpose of this presentation will be to show
what are the general characteristics of this versatile, albeit difficult MRI
method to understand.
METHODS
In vivo CEST-based imaging is a variant of magnetization
transfer (MT) imaging (1), in which the selective saturation
of the magnetization of amide protons is detected indirectly through chemical
exchange with bulk water protons. Selective irradiation is possible because
there are composite proton resonance between 1ppm and 4ppm downfield from the
water resonance. Among the most widely assessed exchangeable proton groups are amide protons, exchanging with bulk
water at a rate of about 30 times per second, amine groups, exchanging at a rate of 1000-2000 Hz, and finally hydroxyl groups, exchanging at rates of
2000 Hz and above. Such exchange rates falls within the slow to intermediate
exchange rate on the NMR time scale (2). Finally, NOE effects, thought to originate from protons in the
aliphatic region, 3 to 5 ppm upfield from water can also lead to a detectable
exchange of protons. Even though
the underlying mechanisms are not fully understood, the effect is considered to
be initially mediated by the cross relaxation via dipole-dipole interaction of
the backbone protons in medium-size molecules.
Most of these exchangeable proton
pools are small (mM concentration range), but continuous saturation leads to a
measurable decrease by a few percent of the large water signal due to a sensitivity
enhancement mechanism. Indeed, by continuously saturating protons at the right
off-resonance frequency, and letting them exchanging with the surrounding bulk
water, one would achieve complete saturation of the latter, without the
counterbalancing effect from the spin-lattice relaxation of the water T1. Note
that this off-resonance saturation can be performed either in a continuous or
pseudo-continuous mode. In humans, pulsed methods have been generally used (e.g.
(3)), analogous to the pulsed MT
techniques used in clinical MT imaging. In general, a CEST image is
calculated based either on the subtraction of a single off-resonance pulse
up-field and down-field from the water line, or as the integral under the curve
created by the subtraction of both parts of the Z spectrum, obtained by
continuous sweep of the off- resonance saturation frequency across typically ±
5-10 ppm around the water peak (2).
Many imaging pulse sequences and
post-processing methods have been developed to measure and assess the CEST
effects, and it is beyond this syllabus to describe them all in details.
Suffice to say that most of the necessary information can be found in two very
good review papers: (2) for the CEST effect in general and (4) for a review on image processing
methods.
The main applications of most CEST
methods have been for the assessment of pH changes, as the exchange rate of
most of the above-mentioned moieties is based-catalyzed (2). As such, some of the most
important uses of this method have been in stroke (5, 6) using endogenous CEST contrast
(i.e. looking at changes in the signal from amide protons due to an
acidification of the tissue) and the imaging of pH in tumours using exogenous
contrast agents such as iopamidol (7).
In addition, some of the early work
has also been focusing on the use of the amide proton signal mainly for the
assessment of tumour aggressiveness based on the increased protein turnover
from high-metabolic cancerous cells (3, 8, 9).
Finally, a whole series of
applications based on the amide and hydroxyl groups have been demonstrated,
from glutamate (10) to glucose (11, 12). Some of its advantages and issues
will also be highlighted in this presentation.
CONCLUSION
CEST and its variants are very
versatile and possibly very useful techniques, but, as often at the early
stages of development of novel MRI techniques, currently suffer from a lack of
harmonization in both sequences and processing techniques. In addition, there
are remaining issues and ongoing debates on the source of some of the
endogenous CEST applications, and much more work is needed before
quantification of the exchangeable pool is possible.
Acknowledgements
No acknowledgement found.References
1. Wolff SD,
Balaban RS. Magnetization transfer imaging: practical aspects and clinical
applications. Radiology. 1994;192(3):593-9.
2. van
Zijl PC, Yadav NN. Chemical exchange saturation transfer (CEST): what is in a
name and what isn't? Magnetic resonance in medicine : official journal of the
Society of Magnetic Resonance in Medicine / Society of Magnetic Resonance in
Medicine. 2011;65(4):927-48.
3. Jones
CK, Schlosser MJ, van Zijl PC, Pomper MG, Golay X, Zhou J. Amide proton
transfer imaging of human brain tumors at 3T. Magnetic resonance in medicine :
official journal of the Society of Magnetic Resonance in Medicine / Society of
Magnetic Resonance in Medicine. 2006;56(3):585-92.
4. Zaiss
M, Bachert P. Chemical exchange saturation transfer (CEST) and MR
Z-spectroscopy in vivo: a review of theoretical approaches and methods. Physics
in medicine and biology. 2013;58(22):R221-69.
5. Tee
YK, Harston GW, Blockley N, Okell TW, Levman J, Sheerin F, et al. Comparing
different analysis methods for quantifying the MRI amide proton transfer (APT)
effect in hyperacute stroke patients. NMR in biomedicine. 2014;27(9):1019-29.
6. Zhou
J, Payen JF, Wilson DA, Traystman RJ, van Zijl PC. Using the amide proton
signals of intracellular proteins and peptides to detect pH effects in MRI.
Nature medicine. 2003;9(8):1085-90.
7. Longo
DL, Busato A, Lanzardo S, Antico F, Aime S. Imaging the pH evolution of an
acute kidney injury model by means of iopamidol, a MRI-CEST pH-responsive
contrast agent. Magnetic resonance in medicine : official journal of the
Society of Magnetic Resonance in Medicine / Society of Magnetic Resonance in Medicine.
2013;70(3):859-64.
8. Zhou
J, Lal B, Wilson DA, Laterra J, van Zijl PC. Amide proton transfer (APT)
contrast for imaging of brain tumors. Magnetic resonance in medicine : official
journal of the Society of Magnetic Resonance in Medicine / Society of Magnetic
Resonance in Medicine. 2003;50(6):1120-6.
9. Zhou
J, Tryggestad E, Wen Z, Lal B, Zhou T, Grossman R, et al. Differentiation
between glioma and radiation necrosis using molecular magnetic resonance
imaging of endogenous proteins and peptides. Nature medicine. 2011;17(1):130-4.
10. Cai
K, Haris M, Singh A, Kogan F, Greenberg JH, Hariharan H, et al. Magnetic
resonance imaging of glutamate. Nature medicine. 2012;18(2):302-6.
11. Chan
KW, McMahon MT, Kato Y, Liu G, Bulte JW, Bhujwalla ZM, et al. Natural D-glucose
as a biodegradable MRI contrast agent for detecting cancer. Magnetic resonance
in medicine : official journal of the Society of Magnetic Resonance in Medicine
/ Society of Magnetic Resonance in Medicine. 2012;68(6):1764-73.
12. Walker-Samuel
S, Ramasawmy R, Torrealdea F, Rega M, Rajkumar V, Johnson SP, et al. In vivo
imaging of glucose uptake and metabolism in tumors. Nature medicine.
2013;19(8):1067-72.