Maria Sedykh1, Stefano Casagranda2, Patrick Liebig3, Christos Papageorgakis2, Laura Mancini4,5, Sotirios Bisdas4,5, Manuel Schmidt1, Arnd Doerfler1, and Moritz Zaiss1
1Institut of Neuroradiology, University Clinic Erlangen, Friedrich-Alexander Universität Erlangen-Nürnberg, Erlangen, Germany, 2Department of R&D Advanced Applications, Olea Medical, La Ciotat, France, 3Siemens Healthcare GmbH, Erlangen, Germany, 4Lysholm Department of Neuroradiology, University College of London Hospitals NHS Foundation Trust, London, United Kingdom, 5Institute of Neurology UCL, London, United Kingdom
Synopsis
Keywords: Tumors, CEST & MT
Fluid suppression has an inestimable value
in improving the readability of Amide Proton Transfer weighted imaging in the
neuro-oncological field, by removing contamination effects in the fluid
compartments. With this work we wanted to justify the derivation of this metric
and to show different clinical examples. Our new fluid-suppressed APTw metric
for 3T MR imaging, based on the principles of Spillover Correction for CEST
imaging, can be then derived through the Bloch McConnell Equations.
Introduction
Amide Proton
Transfer weighted MRI is a molecular imaging technique nowadays available on 3
Tesla MRI scanner1. Despite
its valuable clinical added value, especially in neuro-oncology field2,3, its signal is known to be contaminated by
different effects such as T1,T2 and Magnetic Transfer Contrast (MTC) signal.
This contamination is high in the fluid compartments (such as necrosis, cyst,
hemorrhage) leading to false positives in reading the APTw images4, generating a real problem of clinical
interpretation of the results. Early on, so-called spillover corrections5 were suggested to improve CEST imaging
based on multi-Lorentzian-pools at 7T and 3T fields 6,7, but still not used for APTw imaging based on
Magnetic Transfer Ratio Asymmetry1 metrics at 3T.
The most likely reason for this was that the
spillover correction changed the value scaling and thus the colormap limits of
APTw imaging, making it difficult to compare APTw maps before and after this
correction.
Recently, so-called fluid suppression approaches
for APTw imaging were suggested4,8,that also could suppress highlights in areas
of long T1/T2 and low MTC (typical characteristics in fluid compartments), but
had the benefit that the tissue APTw values (solid compartments) were almost
unchanged and the same colorbar limits could be used.
However the fluid-suppression formulas were
heuristic and could never be properly derived from Bloch-McConnell (BMC)
equations. Herein we show that fluid suppression can actually be understood as
spillover correction, and we provide an adjusted version that can be properly
derived, and used with the same colormap for the traditional APTw imaging.Methods
Formula
derivation:
The fluid-suppression that was proposed in4 introduced an additional weighting factor
following the heuristic condition:(i) this factor must be 1 for tissue to keep
the same colormap, (ii) and close to 0 for liquid tissue. Assuming that the
vales for Z-Spectrum-Reference at Δω=-3.5ppm (Zref) and Z-Spectrum-Label at
Δω=3.5ppm (Zlab) in tissue are typically ≈0.5, and in liquids ≈1, the factor
(2-Zref-Zlab) fulfills this condition.
FSheuristic-MTRasym=(Zref−Zlab)⋅(2−Zref−Zlab)=MTRasym⋅(2−Zref−Zlab) [1]
If we
compare this to a spillover corrected metric, it does not fulfill conditions
(i+ii),but regions with high Z-Spectrum values will be upscaled using the
formula from1
MTRRex=1/(Zlab−Zref)=(Zref+Zlab)/(Zref∙Zlab)=MTRasym/(Zref∙Zlab) [2]
To achieve the same conditions (i+ii) we can
transform this equation back to standard tissue with Zref = Zlab=0.5
generating a spillover corrected fluid suppression (FS).
FS-MTRasym=(0.5⋅0.5) ⋅MTRasym/(Zref∙Zlab) [3]
Now, condition (i) is directly fulfilled, and the factor of condition (ii) is
not 0 but 0.25/1. Eq.[3] thus has similar features as Eq.[1], but is based on
the BMC equations and thus theoretically justified.
Magnetic Resonance Imaging Acquisitions and
post-Processing:
APTw/MRI data were acquired in 3 glioblastoma
patients on a 3T MRI scanner (MAGNETOM Prisma, Siemens, Erlangen, Germany) with
a 64-channel head and neck coil. The APTw protocol (C2P-MPI04, 3 min, 2x2x5mm3,
12 slices) was performed with a 3D snapshot-GRE sequence9, setting a B1 root mean of square of 2μT and a
Duty Cycle of 90%. The WASAB1 protocol10 (C2P-MPI04, 2 min) was performed for
simultaneous B0-B1 mapping. T1w sequences after contrast injection were also
acquired.
Olea Sphere 3.0 software (Olea Medical, La
Ciotat, France) was used to post-process APTw maps.Results
Figure 1 shows that the heuristic fluid-suppression
factor, and the spillover-correction-based fluid-suppression factor have
similar course plotted over Zref, which explains their similar effect on the data and on (liquid)
regions with high Z-values. The property of Eq. [1] to kill all effects at Zref=1
is clinically unrealistic to achieve, while the depletion to only 25% by Eq.
[3] is both theoretical correct and clinically plausible. Figure 2 shows differences of the original and newly proposed
fluid-suppressed APTw method in tumor case at 3T: (first-row) cyst and
liquefied necrosis hotspots are suppressed by Eq. [1] and even more by Eq. [3];
(second-row) both metrics suppress the signal from microfluid environment of an
IDH mutant tumor; (third-row) only the hotspot in the liquefied necrotic part
is removed by fluid-suppression.Discussion
Spillover
correction is asking ‘how high would CEST effects in tissue be without
spillover dilution’. On the other hand, fluid-suppression is asking ‘how low
would CEST effects in liquid areas be if we transform them to similar
conditions as in tissue’. Thus, both make CEST effects of tissue and liquefied
tissue comparable. The novelty here, to bring the spillover correction back to
tissue values, allows to use the same colormap and makes MTRasym-based metrics
and spillover-corrected/fluid-suppressed- based metrics for APTw directly
comparable on the same colormap. In tumor cases with clearly identified liquid
regions, the new fluid-suppressed metric shows similar (and even improved)
features as the previous heuristic one, and clearly removes hotspots of liquid
areas, such as cysts, necrosis and microfluid environments. If this liquid-artifact
or spillover-artifact is removed, the generated contrast might be better
correlated to the actual exchange effects and has potentially higher diagnostic
value, as first studies indicate11,12.Conclusion
Fluid suppression has an inestimable value in improving the readability
of APTw maps in the neuro-oncological field. With this work we wanted to
justify the derivation of this metric from a theoretical point of view, to
reassure the scientific and medical field about its use.Acknowledgements
Department
of Health’s NHR-funded Biomedical Research Centre at University College London.
German
Research Foundation DFG ZA 814/5-1 References
1-
Zhou J,
Payen JF, Wilson DA, Traystman RJ, van Zijl P. Using the amide proton signals
of intracellular proteins and peptides to detect pH effects in MRI. Nature
medicine. 2003 Aug;9(8):1085-90.
2-
Bisdas
S, Demetriou E, Topriceanu CC, Zakrzewska Z. The role of APT imaging in gliomas
grading: a systematic review and meta-analysis. European Journal of Radiology.
2020 Dec 1;133:109353.
3-
Nichelli
L, Casagranda S. Current emerging MRI tools for radionecrosis and
pseudoprogression diagnosis. Current Opinion in Oncology. 2021 Nov;33(6):597.
4-
Togao O., Keupp J., 2018.
Magnetization Transfer Ratio based Metric for APTw or CESTw MRI Suppressing
Signal from Fluid Compartments - Initial Application to Glioblastoma
Assessment. Abstract for ISMRM 2018.
5-
Zaiss
M, Xu J, Goerke S, Khan IS, Singer RJ, Gore JC, Gochberg DF, Bachert P. Inverse
Z‐spectrum analysis for spillover‐, MT‐, and T1‐corrected steady‐state pulsed
CEST‐MRI–application to pH‐weighted MRI of acute stroke. NMR in biomedicine.
2014 Mar;27(3):240-52.
6-
Zaiss
M, Windschuh J, Goerke S, Paech D, Meissner JE, Burth S, Kickingereder P, Wick
W, Bendszus M, Schlemmer HP, Ladd ME. Downfield‐NOE‐suppressed amide‐CEST‐MRI
at 7 Tesla provides a unique contrast in human glioblastoma. Magnetic resonance
in medicine. 2017 Jan;77(1):196-208.
7-
Goerke
S, Soehngen Y, Deshmane A, Zaiss M, Breitling J, Boyd PS, Herz K, Zimmermann F,
Klika KD, Schlemmer HP, Paech D. Relaxation‐compensated APT and rNOE CEST‐MRI
of human brain tumors at 3 T. Magnetic resonance in medicine. 2019
Aug;82(2):622-32.
8-
Casagranda S, Mancini L, Gautier G, Peter
P, Lopez B, Brandner S, de Vita E, Golay X, Bisdas S. Fluid suppression in CEST
imaging affects predominantly IDH-mutant 1p/19q retained gliomas with T2-FLAIR
mismatch. Abstract #0500 In ISMRM 29th Annual Meeting 2020.
9-
Liebig P, Sedykh M, Herz K, Fabian MS,
Mennecke A, Weinmüller S, Schmidt M, Dörfler A, Zaiss M. snapshot CEST++: the
next snapshot CEST for fast whole-brain APTw imaging at 3T. arXiv preprint
arXiv:2207.00261. 2022 Jul 1.
10-
Schuenke
P, Windschuh J, Roeloffs V, Ladd ME, Bachert P, Zaiss M. Simultaneous mapping
of water shift and B1 (WASABI)—application to field‐inhomogeneity correction of
CEST MRI data. Magnetic resonance in medicine. 2017 Feb;77(2):571-80.
11-
Mancini
L, Casagranda S, Gautier G, Peter P, Lopez B, Thorne L, McEvoy A, Miserocchi A,
Samandouras G, Kitchen N, Brandner S. CEST MRI provides amide/amine surrogate
biomarkers for treatment-naive glioma sub-typing. European journal of nuclear
medicine and molecular imaging. 2022 Jan 14:1-5.
12-
Nichelli L, Jacob J, Leclerq D, Benbelkacem F, Lehéricy S, and
Casagranda S. Predicting radionecrosis and recurrent disease through Amide
Proton Transfer weighted imaging in brain metastases. Abstract #7682 In ISMRM 31th Annual
Meeting 2022.