Near the end of the diffuser-rearing period (approximately 150 days of age), magnetic resonance imaging (MRI) was performed on 11 representative animals with a horizontal bore scanner (7T Bruker Biospec USR 70/30; Bruker, Karlsruhe, Germany). A 155-mm inner-diameter volume coil supplied by Bruker was used for radiofrequency transmission and signal reception.
To obtain the MRI scans, the monkeys were initially anesthetized with 4% to 5% isoflurane in an air/oxygen mixture (7:3). To stabilize the animals during the recording session, the monkeys were intubated and maintained on 2% isoflurane gas anesthesia administered through an anesthesia system (ventilator, Inspira asv [Harvard Apparatus, Holliston, MA]; vaporizer, VMS Anesthesia Machine [MDS Matrix, Orchard Park, NY]). Body temperature was kept at 36.5C° ± 1C° with a feedback-controlled warm air system (SA Instruments, Stony Brook, NY). Throughout the MRI procedures, respiration rate and rectal temperature were measured using a small-animal monitoring system (SA Instruments). Blood oxygen saturation and heart rate were monitored with an MRI-compatible pulse oximeter (NONIN, Plymouth, MN). The monkey’s head was fixed on a custom-designed head holder, and petrolatum ophthalmic ointment was applied topically to prevent the ocular surfaces from drying during MRI scans.
The initial tripilot scan was used to localize the positions of the monkey’s eyes. Magnetic field homogeneity was then optimized using localized shimming with a point-resolved spectroscopy procedure. Anatomic images were acquired with a three-dimensional (3D)-rapid acquisition paradigm with a relaxation enhancement sequence. Image signals were enhanced with a 3D method by which all scan slices were acquired simultaneously, in contrast to conventional 2D methods by which scan slices are acquired separately. Scan parameters of the axial images were as follows: field of view (FOV) varied from 50 × 50 × 20 mm to 50 × 50 × 30 mm, depending on eye size; acquisition matrix varied correspondingly from 256 × 256 × 40 to 256 × 256 × 60 to ensure that a slice thickness of 0.5 mm was maintained. Spatial resolution of the axial images was 0.195 × 0.195 × 0.5 mm. T2-weighted images were obtained with long repetition (TR, 1500 ms) and effective echo times (TE, 96 ms) to enhance the contrast between the fluids and tissues of the eye. Average scan time per session was approximately 40 minutes.
Acquired axial MR images were reconstructed with the use of in-house software developed with numerical computing environment and programming language (MATLAB; Mathworks, Natick, MA), which allowed the MR images to be viewed from axial, sagittal, and coronal orientations. The software interpolated between the axial image slices to produce uniform resolution of 0.195 mm in the 3D matrix. To ensure that measurements of the ocular dimensions were obtained from the appropriate image plane, the 3D volumes were rotated so that in the sagittal orientation, the line connecting the equatorial poles of the lens was vertical. The rotation angle was in the range of 4° to 29°. A Canny edge detection algorithm was applied to the horizontal plane of the rotated volumes to determine the boundaries between ocular structures. The approximate optical axis was defined as the perpendicular through the midpoint of the line connecting the equatorial poles of the lens. Lens thickness was determined as the distance along this axis from the anterior to the posterior lens surface. The horizontal image slice that contained the greatest lens thickness in the interpolated stack was used for all further measurements. The intersection of the presumed optical axis and the posterior lens surface was considered the approximate position of the second nodal point.
36 The primary measure of interest was the vitreous chamber depth, which was defined as the distance between the approximate position of the second nodal point and the retina. Vitreous chamber depth was determined as a function of eccentricity from 45° nasally to 45° temporally in 15° intervals along the horizontal meridian. To assess the overall shape of the globe, we also measured the eye’s axial length and the equatorial diameter in the horizontal plane. Axial length was defined as the distance from the anterior corneal surface to the retina along the presumed optical axis. Equatorial diameter was defined as the greatest distance between the nasal and the temporal retinas measured along a line perpendicular to the presumed optical axis.