Paddy J. Slator1,2, Luke Pleva3,4, Lucy Higgins5,6, Edward Johnstone5,6, Alexander Heazell5,6, Daniel C. Alexander7, Josephine H. Naish3,4, and Kate Duhig5,6
1Cardiff University Brain Research Imaging Centre, Cardiff University, Cardiff, United Kingdom, 2School of Computer Science and Informatics, Cardiff University, Cardiff, United Kingdom, 3BHF Manchester Centre for Heart and Lung Magnetic Resonance Research, University of Manchester, Manchester, United Kingdom, 4Division of Cardiovascular Sciences, Faculty of Biology, Medicine and Health, University of Manchester, Manchester, United Kingdom, 5Maternal and Fetal Health Research Centre, Institute of Human Development, University of Manchester, Manchester, United Kingdom, 6St. Mary's Hospital, Manchester University Hospitals NHS Foundation Trust, University of Manchester, Manchester, United Kingdom, 7Centre for Medical Image Computing and Department of Computer Science, University College London, London, United Kingdom
Synopsis
Keywords: Placenta, Placenta
Motivation: The intravoxel incoherent motion (IVIM) model can separately assess diffusion in tissue and perfusion in vasculature. However, anisotropic extensions to IVIM that model coherently orientated vasculature are complex and difficult to fit.
Goal(s): Enhance the IVIM model to account for macroscopic anisotropy in vascular structures, while minimizing the increase in model complexity.
Approach: We model perfusion and diffusion compartments using constrained tensors and estimate the tensor parameters via the spherical mean.
Results: Our spherical mean anisotropic IVIM approach quantifies and maps anisotropy in perfusion and diffusion compartments and captures microstructural and microcirculatory alterations in the placenta during pregnancy.
Impact: Existing anisotropic IVIM models are complex and clinically impractical. We demonstrate a spherical mean approach that simplifies the disentanglement of perfusion- and diffusion-related anisotropy. This can enable rapid quantification of biomarkers for detecting microcirculatory and microstructural changes in anisotropic tissue.
Introduction
The intravoxel
incoherent motion (IVIM) model separates diffusion- and perfusion-related
components of the diffusion MRI (dMRI) signal. However, the IVIM model assumes isotropic signal attenuation, whereas macroscopic
anisotropy can occur in diffusion-related components and perfusion-related components (e.g. in coherent vasculature in
muscles1).
Extensions to IVIM additionally
accounting for macroscopic anisotropy in diffusion- and perfusion-related signal
components have been demonstrated in muscle1, brain2–4, heart5, kidney6–8, prostate9, and placenta10. Separating perfusion- and
diffusion-related anisotropy in dMRI offers the opportunity for new imaging
biomarkers, for example separate perfusion- and diffusion-related fractional
anisotropy (FA).
However, these anisotropic
IVIM models are complex. For instance, some extend IVIM by incorporating
full tensors for the diffusivity, perfusion-related diffusivity, and perfusion
fraction, yielding an 18 parameter model7. Even when full tensors are only used
for some of these, models involve numerous parameters.
Spherical mean techniques
can calculate quantitative microstructural metrics whilst factoring out orientation
dependence11, meaning fewer model parameters that are
easier to fit whilst still accounting for anisotropy. Here we introduce simplified anisotropic IVIM
using spherical mean (SM) techniques and demonstrate its application in
placental MRI.Methods
Pregnant participants
gave informed consent to undergo dMRI of the placenta (22-37 weeks’ gestation),
DAPHNE study (REC 22/YH/0144). Here,
we include data from 19 participants with normal pregnancy outcome (defined as normotensive
pregnancy, and term delivery of normal birthweight baby).
We scanned on a Siemens Vida scanner
at 3T using the Body 18 coil, utilising a previously published dMRI protocol
that was optimised for the placenta12. The protocol has $$$b= [5,10,18,25,36,50,100,200,400,600,800,1200,1600]\;$$$s mm-2 with
multiple gradient directions optimised for maximal angular coverage13. Other imaging parameters were TE$$$=83\;$$$ms, TR$$$=3300\;$$$ms,
Grappa 2, partial Fourier 6/8, voxel size = $$$3\times3\times15\;$$$mm, image
matrix $$$128\times128\times9$$$, acquisition time = 3:07.
Data were
pre-processed with MP-PCA denoising14,
Rician bias correction15, and Gibbs ringing removal16. We manually defined a
region-of-interest (ROI) containing the placenta and basal plate as previously
described10.
We fit the diffusion tensor (DT) with weighted
linear least squares17 utilising all measurements, and
calculated downstream metrics, using MRTrix18. We fit IVIM in dmipy19.
We introduce two
anisotropic IVIM spherical mean approaches, based on stick-zeppelin and
zeppelin-zeppelin models that were previously suggested for placental dMRI10. These are two-compartment models made
up of stick20 and zeppelin21 components.
The spherically
averaged stick signal is
$$\bar{S}_S(d_{par})=\frac{\sqrt{\pi}\;\mbox{erf}\left({\sqrt{bd_{par}}}\right)}{2\sqrt{bd_{par}}}$$
where erf() is the
error function, $$$d_{par}$$$ is the parallel diffusivity, $$$\bar{S}_S$$$ is the spherically averaged
signal and $$$b$$$ is the b-value.
The spherically
averaged zeppelin signal is11
$$\bar{S}_Z(d_{par},d_{perp})=\exp(-bd_{perp})\frac{\sqrt{\pi}\;\mbox{erf}\left({\sqrt{b(d_{par}-d_{perp})}}\right)}{2\sqrt{b(d_{par}-d_{perp})}}$$
where dperp is the
perpendicular diffusivity.
The signal for
SM-zeppelin-zeppelin is
$$\bar{S}=f\bar{S}_Z(d_{par}^*,d_{perp}^*)+(1-f)\bar{S}_Z(d_{par},d_{perp}).$$
The signal for
SM-stick-zeppelin is
$$\bar{S}=f\bar{S}_S(d_{par}^*)+(1-f)\bar{S}_Z(d_{par},d_{perp}).$$
We fit SM-stick-zeppelin
and SM-zeppelin-zeppelin using dmipy19. We calculated FA for the tissue- and
perfusion-related zeppelin compartments separately.
Figure 1 gives the
parameter constraints when fitting, and Figure
2 schematically represents each model. Results
Figure 3 displays all
maps for one participant. DT and IVIM
maps are akin to previous studies10. For example,
diffusivities, FA, and perfusion fraction are higher at placental margins. SM-stick-zeppelin
perfusion-related diffusivity is high in the basal plate whereas
diffusion-related diffusivity is high in the chorionic plate. Both
SM-stick-zeppelin and SM-zeppelin-zeppelin tissue-related FA maps show intra-placental
contrast.
Figure 4 plots the ROI-averaged
parameter values against gestational age for each participant, showing
that these parameters capture diffusion- and perfusion-related changes over
gestation. SM-stick-zeppelin
has the two parameters with highest correlation with gestation.Discussion
Our novel approach maps diffusivity and anisotropy related to
microcirculation and microstructure. Maps reveal consistent patterns across 19 scanned participants,
illustrated in Figure 5 for perfusion fraction, and capture
changes across gestation (Figure 4). The SM-stick-zeppelin perfusion fraction and
perfusion-related parallel diffusivity have the highest correlation with
gestational age, suggesting that an anisotropic IVIM SM approach better captures microstructural and microcirculatory changes than DT and IVIM models, and has potential for accurately capturing such alterations in dysfunctional
placentas.
DT-derived
diffusivities decrease over gestation (Figure
4), in agreement with previous literature22. However, whilst the SM-stick-zeppelin
perfusion-related $$$d_{par}$$$ decreases over gestation, both
SM-stick-zeppelin tissue-related diffusivities increase over gestation (Figure 4). This suggests that SM-stick-zeppelin can disentangle different sources
of attenuation in placental dMRI data, and that perfusion- and
diffusion-related components may evolve differently over gestational age.
We used a straightforward signal direction-averaging method although our protocol, with multiple
b-shells, is not ideally suited for this. Future work will explore using
rotational invariants to more accurately estimate the spherical mean23.Conclusion
We introduce an
anisotropic IVIM SM approach to disentangle perfusion- and tissue-related
diffusivity and anisotropy. This approach captures
changes across gestation in placental MRI better than baseline models. Perfusion- and tissue-specific metrics are potential
biomarkers for various diseases.Acknowledgements
We thank all pregnant
participants, midwives, obstetricians, and radiographers who played a key role
in obtaining the datasets. This work was funded by the Wellcome Leap In Utero
programme project “Multi-modal studies to understand pregnancy and prevent
stillbirth”.References
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