Andreas Wetscherek1, Brigid A McDonald2, Ernst S Kooreman3, Angus Z Lau4,5, Ramesh Paudyal6, Amita Shukla-Dave6,7, Liam SP Lawrence4,5, Petra J van Houdt3, and Uulke A van der Heide3
1Joint Department of Physics, The Institute of Cancer Research and The Royal Marsden NHS Foundation Trust, London, United Kingdom, 2Department of Radiation Oncology, The University of Texas MD Anderson Cancer Center, Houston, TX, United States, 3Department of Radiation Oncology, The Netherlands Cancer Institute, Amsterdam, Netherlands, 4Physical Sciences Platform, Sunnybrook Research Institute, Toronto, ON, Canada, 5Department of Medical Biophysics, University of Toronto, Toronto, ON, Canada, 6Department of Medical Physics, Memorial Sloan Kettering Cancer Center, New York, NY, United States, 7Department of Radiology, Memorial Sloan Kettering Cancer Center, New York, NY, United States
Synopsis
Measuring the detectable effect size is crucial for setting
up clinical trials involving quantitative MRI for
treatment
adaptation, response assessment and outcome prediction in MR-guided radiotherapy. For four different tumor sites (brain, head and neck, prostate and rectum) diffusion-weighted MRI protocols were optimized for intravoxel incoherent motion imaging based on minimizing the mean relative error of the IVIM parameters. For full IVIM model fits, 4-5 b-values were found optimal, while a fit with fixed D* was best performed with 3 b-values. MR-Linac systems currently have limitations regarding gradient performance and number of coil channels and qMRI techniques
require careful optimization.
Purpose
Measuring the detectable effect size is crucial for setting
up clinical trials involving quantitative MRI (qMRI) biomarkers and for
adequate interpretation of daily qMRI measurements in the context of treatment
adaptation, response assessment and outcome prediction. The aim of this study
is to suggest a data-driven approach to characterize and optimize
diffusion-weighted (DW) magnetic resonance imaging (MRI) for intravoxel
incoherent motion (IVIM) analysis on hybrid MR-Linacs. Introduction
The IVIM model1 introduces a perfusion
compartment, which contributes the perfusion fraction f to the unweighted
signal. In addition to the tissue diffusion coefficient D, a pseudo-diffusion
coefficient D* is used to describe perfusion-related signal attenuation. All
IVIM parameters have shown promise as biomarkers for assessing tumor cellularity
and early response to radiation therapy2,3,4,5, but variability in estimates of quantitative imaging biomarkers (QIBs) in longitudinal studies can lead to uncertainty in detecting post-treatment
changes. In particular for multi-center
trials, repeatability tests are essential to identify sources of
errors across clinical sites. Substantial differences
in the design of an MR-Linac6 compared to conventional MRI scanners make it
challenging to optimize DW MRI protocols5,7. Here we
propose a data-driven strategy based on a set of calibration scans to optimize
the acquisition, such that uncertainty in the IVIM parameter estimates is
minimized and quantified to facilitate robust interpretation regarding clinical
end-points.Methods
DW data were acquired using single-shot EPI in 6 patients (1 head & neck cancer, 3 glioblastoma multiforme (GBM), 1
prostate carcinoma and 1 rectal carcinoma) across different 1.5T MR-Linac (Elekta
AB, Stockholm) sites. Patients consented to participate in clinical studies
approved by local IRBs. Calibration scan parameters (Table 1) followed consensus guidelines for DWI on the Unity system7 and consisted of
single-average trace-weighted DW images for a wide range of b-values and were repeated
five times within one session.
Monte-Carlo simulations were performed using the average
per-pixel standard deviation of the signal intensity within the delineated ROI. To limit search space, allowed b-values were restricted to 0, 2, 5, 10, 15, 20, 25, 30, 35, 40, 45, 50, 60, 70, 80, 90, 100, 125, 150, 175, 200,
250, 300, 350, 400, 450 and 500 s/mm2. Starting from 25 averages for
each of the 27 allowed b-values, in each step one of the following two actions
was performed: Either one average was removed from one b-value or one b-value
was removed completely and its averages minus one were distributed randomly among other b-values. For each of these possibilities
2500 IVIM fits were performed on data simulated according to $$$S(b)=S_0[(1-f)e^{-bD}+fe^{-bD^*}]$$$ by drawing ground truth signal
intensity S0, D, f and D* randomly from $$$S_0\in[0.4,5]$$$, $$$f\in[0.01, 0.4]$$$, $$$D\in[0.8, 3.0]\times10^{-3}mm^2/s$$$ and $$$D^{*}\in[4.0,100.0]\times10^{-3}mm^2/s$$$ and applying the relative signal variation from the calibration scans. At each step the action that resulted in the
lowest average relative fit error with
respect to the drawn ground truth was chosen. One exception was that the number of averages for b-values 0, 150 and 500 s/mm2 was not allowed to reach zero to enable baseline ADC calculations7. Four
different scenarios were investigated: pixel-wise fitting vs fitting to the average values within an ROI of size 25 pixels, combined with either a full 4-parameter IVIM fit or a fit where D* was fixed to
40x10-3mm2/s.Results
Fig. 1 shows exemplary diffusion-weighted calibration scan
images and corresponding contours. The per-pixel standard deviation was
calculated across the five repetitions and averaged within the ROI, resulting
in the input for the Monte-Carlo simulations (Fig. 2). Fig. 3 displays the
dependence of the mean relative error (MRE) on the total number of averages for the different IVIM
parameters and anatomical sites. For all anatomical sites MRE D < MRE f < MRE D*. The MRE is strongly reduced for
fitting the model to ROI-averaged data, compared to pixel-wise fitting. Table
2 lists the optimal b-values and simulated mean relative errors for a 5
min acquisition, which is acceptable for integration into a clinical MR-Linac
treatment workflow.Discussion
Fitting of the full IVIM model for an ROI is possible, but
one should consider that the MRE and the variation of the QIBs might depend heavily on the used
protocol, when setting up clinical studies. For the range of protocols
investigated here, pixel-wise D* mapping led to higher errors than fixing D* to
a pre-determined value and could explain why only population average results showed
a significant trend in5.
For full IVIM model fits, the simulation identified 4-5
different b-values as optimal, while a fit with fixed D* is optimally performed
with 3 b-values. MR-Linac systems currently have limitations in terms of
gradient performance and qMRI
techniques require careful optimization.
Lower resolution could reduce the impact of
signal variation but could introduce Gibbs-ringing artifacts and
partial volume effects. Deep learning9 or denoising
techniques10 could potentially overcome the current limitations regarding
D* mapping on MR-Linacs.
The here described technique based on calibration scans could potentially be extended to other QIBs. Future work will investigate repeatability of the optimized IVIM protocols to inform clinical trials.Conclusion
Application of data-driven techniques for standardizing IVIM
protocols is the first step towards reliable estimation of IVIM-derived QIBs in
the clinical context of treatment adaptation, response assessment and outcome
prediction.Acknowledgements
No acknowledgement found.References
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