Jon O Cleary1, Bao Nguyen2, Rebecca Glarin1, Scott C Kolbe1, Bradford A Moffat1, Rishma Vidyasagar1, Bang Bui2, Allison McKendrick2, and Roger J Ordidge1
1Melbourne Brain Centre Imaging Unit, Department of Anatomy and Neuroscience, University of Melbourne, Parkville, Australia, 2Department of Optometry and Vision Sciences, University of Melbourne, Parkville, Australia
Synopsis
While optical eye
imaging techniques are available for examining anterior and retinal
structures, they are limited in making 3 dimensional assessments of the whole eyeball. MRI is the
preferred modality in these areas but fine eye structures are difficult to
resolve on clinical systems. Ultra high field magnets offer increased signal-to-noise,
providing higher resolution, but there have been only a limited number of studies so far. We performed an initial study to assess achievable resolution, the anatomy visible
on differing image weightings and MR parameter measurements, in eyes of healthy
subjects on a 7 Tesla system.
Introduction
Optical eye imaging techniques (such as optical coherence tomography) are excellent, widely available methods for examining
anterior and retinal structures. However, these have a limited role in 3D assessments
of the whole eyeball and related orbital and retrobulbar structures. Magnetic
resonance imaging is the preferred non-invasive modality for these regions but
fine structures such as extraocular muscles, blood vessels and the optic nerve can
be difficult to resolve on conventional clinical systems. Ultra high field
magnets offer superior signal-to-noise, which may be ideal for providing the
increased resolution needed to visualise these areas, but there have been a limited
number of studies thus far[1,2,3]. We performed a preliminary
assessment of achievable resolution, anatomy visible on differing image
weightings and MR parameter measurements, in eyes of healthy subjects at ultra
high field. This forms part of ongoing work seeking to optimise our imaging for
future patient studies.Methods
Subjects: All human
imaging was conducted with Research Ethics Committee approval. Healthy volunteers (5M/2F,
29-47yrs) with normal acuity were imaged using a Siemens 7 Tesla
research MRI scanner and dedicated 6-channel eye coil[3] (MRI.TOOLS GmbH, Berlin, Germany).
Subjects performed a visual attention task in the system to maintain eye fixation.
Select subjects underwent higher resolution scanning of one eye taped comfortably
to reduce susceptibility and blink artefacts[2,4,5]. Imaging: Axial and sagittal 2D T2-w
fast spin echo sequence (TEeff/TR/ETL/FA/NSA/TAcq: 11ms/5.4sec/18/170°/1/2mins) 0.26mm in-plane, 0.7mm slices. 3D
gradient-echo (GRE) images were acquired one eye at a time (TE/TR/FA/GRAPPA/NSA/TAcq:10ms/4ms/12°/2/1/2or4mins) 0.2x0.2x0.4 or 0.9mm. One subject
had 3D-GRE imaging at multiple flip angles (5-30°) and an additional TE. B1
maps were collected. Image processing: Images
were N4 bias field corrected (Advanced Normalisation Tools) prior to anatomical
viewing. Estimated T1 maps calculated from registered (NiftyReg, TIG, University College London UK) multiple FA 3D GRE datasets using JIM v5.0 (Xinapse Systems Ltd., West Bergholt UK). Results
As seen in Fig. 1, the T2-w
protocol produced detailed images with and without fat suppression.
Fig. 2 shows the effect of varying
flip angle on eye structure SNR in the 0.9mm 3D GRE images. These acquired
images enabled voxel-by-voxel T1 estimates to be calculated.
Shown in Fig. 3, imaging a taped
eye, combined with effective fixation, allowed high-resolution T1-w
images (voxel volume 0.016mm3) with low motion and susceptibility
artefact and high SNR (mean whole-eye SNR = 37).Conclusion
This initial work demonstrates high
resolution images of the eye on both T2 and T1-w sequences,
with excellent anatomical detail including: the lens, ciliary body, optic nerve,
ophthalmic vessels and arachnoid space CSF. For the GRE sequence in particular,
we achieved a voxel volume of 0.016mm3 – lower than previous studies2,3
– which readily allowed volumetric structural segmentation. Further continued
optimisation of these sequences may allow higher resolution, potentially
increasing sensitivity to structural pathology in future patient studies.Acknowledgements
J.C. is a University of Melbourne McKenzie
Fellow. This project and B.N. are supported by Melbourne Neuroscience Institute
Seed Grant and Fellowship. S.K. is an Australian National Medical and Health
Research Council Peter Doherty Fellow. Our 7T system is supported by the
Australian National Imaging Facility (NIF). High-performance computing provided
by the Multi-modal Australian ScienceS Imaging and Visualisation
Environment (MASSIVE).References
1. Beenakker, J. W. M., et al. (2013) Highâresolution MRI of uveal melanoma using a
microcoil phased array at 7 T. NMR Biomed, 26(12), 1864–1869.
2.
Richdale, K., et al. (2009). 7 Tesla MR imaging of the human eye in vivo. JMRI, 30(5),
924–932.
3.
Graessl, A., et al. (2014). Ophthalmic magnetic resonance imaging at 7 T using a
6-channel transceiver radiofrequency coil array in healthy subjects and
patients with intraocular masses. Investigative Radiology, 49(5),
260–270.
4.
Bert, R. J., et al. (2006). High-resolution MR imaging of the human eye (2005). Academic
Radiology, 13(3), 368–378.
5.
Berkowitz, B. A., et al. (2001). Measuring the human
retinal oxygenation response to a hyperoxic challenge using MRI: Eliminating
blinking artifacts and demonstrating proof of concept. Mag Reson Med, 46(2),
412–416.