Ludger Starke1, Thoralf Niendorf1, and Sonia Waiczies1
1Berlin Ultrahigh Field Facility (B.U.F.F.), Max Delbrück Center for Molecular Medicine in the Helmholtz Association, Berlin, Germany
Synopsis
Labeling cells with 19F
nanoparticles (NPs) continues to elicit interest for non-invasive localization
of inflammation and monitoring immune cell therapy. Systematic overestimation
in low SNR MRI of 19F-NPs has been previously described which needs
to be corrected for valid quantitative conclusions. We develop a statistical
model which successfully compensates this bias and demonstrate its efficacy for
the correct estimation of signal intensities on neuroinflammation data acquired
in a mouse model of multiple sclerosis. The correction only relies on the image
data itself and promises to be a valuable contribution to the development of
reliable quantitative 19F MRI.
Introduction
Labeling cells with 19F
nanoparticles (NPs) continues to elicit interest for the non-invasive 19F
MR localization of inflammation and monitoring immune cell therapy.1,2 We recently reported strong bias in
conventional, magnitude reconstruction 19F MRI when imaging
inflammation in a mouse model of multiple sclerosis (experimental autoimmune
encephalomyelitis, EAE).3 The effect
occurred despite Rician noise bias correction (RNBC)4 and reduction of the observed bias will
be essential for future quantitative applications of 19F MR. Statistical
characteristics of the experiments were low SNR, no a priori known signal
location, and a heavily skewed distribution of signal intensities (Fig.1). Here
we propose a statistical model which successfully removes the bias without need
for additional calibration experiments.Methods
We examine 11 in vivo datasets from 5 SJL/J mice, partially scanned on multiple
days, and ex vivo datasets from 5
different mice. Perfluoro-15-crown-5-ether rich nanoparticles were administered
daily starting on day 5 following EAE induction5 and in vivo data was
acquired on day 10 to 14. Ex vivo
tissue was fixed and secured in tubes filled with paraformaldehyde.5
A 3D-RARE protocol was employed for 19F-MRI:
TR=800ms, TE=4.4ms, ETL=40, FOV=(45x16x16)mm3, (140x40x40) matrix.
32min and 80min (in vivo) or 128min (ex vivo) measurements are used as test
and reference data, respectively. Signal intensities after RNBC4 are denoted as St and Sr. The noise
level σ was estimated based on a background region.
Images were thresholded at SNR=3.5 and features of less than 3 connected 19F
signal voxels were removed as outliers. For more details on the data, see also
Starke et al., Setup 2 and 3.3
For true, but unknown signal S* and measured signal Sm before RNBC , the
forward model πσ(St|S*) is given by Rician distribution Ri(St;Sm,σ) (Fig.2a). We model S* as drawn iid from prior distribution πθ(S*) with parameters θ and consider three different prior
distributions commonly used for skewed data: exponential, Weibull and
log-normal. We estimate θ for each image individually by maximizing the likelihood of
the measured signal intensities under the marginal distribution πσ,θ(Sm)=∫πσ(Sm|S*)πθ(S*)dS* (Fig.2b). Akaike information criterion (AIC) weights
were computed for all test and reference images to compare the prior
distribution candidates.6 For
all subsequent computations the log-normal prior was used.
Based on prior distribution and forward
model, we computed the corrected signal as the posterior mean following Bayes theorem (Fig.2c).
Analysis was performed by comparison of St and Sc to Sr for single voxels and averaged over complete
features, i.e. separate clusters of connected signal voxels. To evaluate the
effectiveness at different signal levels, a moving average with bin width 0.8σ was computed weighted by the number of voxels
per feature.Results
Marginals based on the Weibull and
log-normal prior provided a good fit of the measured data for datasets with both
small (Fig.3a) and large numbers of signal voxels (Fig.3b), whereas the
exponential prior did not yield a good fit for multiple datasets spanning a
larger range of signal intensities (Fig.3b). The Akaike weights show each of
the candidates as optimal for some of the datasets. The single parameter
exponential prior is favored in small datasets, whereas the Weibull and
log-normal distribution are superior for larger datasets and perform similarly
(Fig.3c).
In an example in vivo dataset, the signal intensity is overestimated at all
signal levels by on average 0.5σ (Fig.4a). The model-based correction successfully
removes this bias without altering the random spread (Fig.4a). The same holds
true when averaging over signal features, except for those close to the
detection threshold. No difference between smaller and larger features is noticeable
(Fig.4b). The example slice (Fig.4c) illustrates these effects: while the
change to the signal level of individual voxels is small, the corrected image
contains a balance of overestimated and underestimated voxels, while the
original nearly exclusively contains overestimated voxels.
The joint analysis of all datasets confirms
these observations (Fig.5). In vivo the
average overestimation in uncorrected data is slightly larger than in the
example at about 0.8σ (Fig.5a) for single voxels and up to 1σ averaged over features (Fig.5c). Again, the average
bias in the corrected data is close to 0 except at St/σ>10, where few
available voxels lead to fluctuations of the moving average. Analysis of the ex vivo data yields similar results
(Fig.5b,d).Discussion & Conclusion
We have shown that systematic
overestimation in low SNR MRI of 19F-NPs can be explained and
corrected by assuming that signal intensities are drawn from a heavily skewed
distribution, e.g. a log-normal. While the effect size is below the random uncertainty
for individual voxels, both the overestimation in uncorrected data and the
effectiveness of model-based correction persist when averaging over ROIs, which
would normally suggest a high degree of certainty. Thus, correction is
essential to achieve quantitatively correct conclusions.
The correction can be applied purely in
post-processing without the need to change data acquisition protocols. A
natural extension of the existing model would be to exploit the spatial
structure of imaging data, e.g. by modelling a hidden Markov random field. It
remains to be investigated whether similar effects occur in other 19F
MRI applications, such as the imaging and quantification of fluorinated drugs,7 or in different low SNR MR
measurements.Acknowledgements
This study was funded in part by the Deutsche Forschungsgemeinschaft to Sonia Waiczies (DFG WA2804). Thoralf Niendorf was supported by an advanced grant from the European Research Council (EU project 743077 - ThermalMR).References
1. Darçot E, Colotti R, Pellegrin M, et
al. Towards Quantification of Inflammation in Atherosclerotic Plaque in the
Clinic - Characterization and Optimization of Fluorine-19 MRI in Mice at 3 T. Scientific reports. 2019;9(1):17488.
2. Chapelin F, Capitini CM, Ahrens ET.
Fluorine-19 MRI for detection and quantification of immune cell therapy for
cancer. J Immunother Cancer. 2018;6(1):105.
3. Starke L, Pohlmann A, Prinz C,
Niendorf T, Waiczies S. Performance of compressed sensing for fluorine-19
magnetic resonance imaging at low signal-to-noise ratio conditions. Magn Reson Med. 2020;84(2):592-608.
4. Henkelman RM. Measurement of signal
intensities in the presence of noise in MR images. Med Phys. 1985;12(2):232-233.
5. Waiczies S, Millward JM, Starke L,
et al. Enhanced Fluorine-19 MRI Sensitivity using a Cryogenic Radiofrequency
Probe: Technical Developments and Ex Vivo Demonstration in a Mouse Model of
Neuroinflammation. Scientific reports. 2017;7(1):9808.
6. Wagenmakers EJ, Farrell S. AIC model
selection using Akaike weights. Psychon
Bull Rev. 2004;11(1):192-196.
7. Prinz C, Starke
L, Millward JM, et al. In vivo detection of teriflunomide-derived fluorine
signal during neuroinflammation using fluorine MR spectroscopy. In Press. Theranostics 2020. Doi:10.7150/thno.47130