Abstract
Purpose.:
To determine the degree of correlation between spatial characteristics of the retinal nerve fiber layer (RNFL) birefringence (Δn RNFL) surrounding the optic nerve head (ONH) with the corresponding anatomy of retinal ganglion cell (RGC) axons and their respective organelles.
Methods.:
RNFL phase retardation per unit depth (PR/UD, proportional to Δn RNFL) was measured in two cynomolgus monkeys by enhanced polarization-sensitive optical coherence tomography (EPS-OCT). The monkeys were perfused with glutaraldehyde and the eyes were enucleated and prepared for transmission electron microscopy (TEM) histologic analysis. Morphologic measurements from TEM images were used to estimate neurotubule density (ρRNFL), axoplasmic area (A x) mode, axon area (A a) mode, slope (u) of the number of neurotubules versus axoplasmic area (neurotubule packing density), fractional area of axoplasm in the nerve fiber bundle (f), mitochondrial fractional area in the nerve fiber bundle (x m), mitochondria-containing axon profile fraction (m p), and length of axonal membrane profiles per unit of nerve fiber bundle area (L am/A b). Registered PR/UD and morphologic parameters from corresponding angular sections were then correlated by using Pearson's correlation and multilevel models.
Results.:
In one eye there was a statistically significant correlation between PR/UD and ρRNFL (r = 0.67, P = 0.005) and between PR/UD and neurotubule packing density (r = 0.70, P = 0.002). Correlation coefficients of r = 0.81 (P = 0.01) and r = 0.50 (P = 0.05) were observed between the PR/UD and A x modes for each respective subject.
Conclusions.:
Neurotubules are the primary source of birefringence in the RNFL of the primate retina.
Glaucoma is a progressive optic nerve disease characterized by a loss of retinal ganglion cell (RGC) axons and thinning of the retinal nerve fiber layer (RNFL). Axon loss can be as much as 50% before the disease is clinically detectable.
1 Imaging devices have been developed to quantitatively measure RNFL thinning and birefringence loss. For example, optical coherence tomography (OCT) produces cross-sectional images of the retina allowing measurement of RNFL thickness.
2 Polarization-sensitive OCT (PS-OCT)
3 and scanning laser polarimetry (GDx; Carl Zeiss Meditec, Inc. Dublin, CA)
4 measure phase retardation in the RNFL that arises from anisotropic structures in the RNFL.
5 Changes in RNFL birefringence may precede RGC death.
Birefringence (Δ
n) is a dimensionless measure of the anisotropy of the refractive index (
n) of a material and is given by the difference between the extraordinary index (
n e) and ordinary index (
n o), where
n o and
n e are the refractive indices for polarization perpendicular and parallel to the axis of anisotropy respectively (Δ
n =
n e −
n o). Phase retardation is proportional to birefringence according to the expression Δ
n = λ
0PR/360°Δ
Z where λ
0 is the free-space wavelength, PR is the phase retardation, and Δ
Z is the thickness of the material.
6 In general, Δ
n of the RNFL is weakly wavelength dependent across visible and near infrared wavelengths.
7 The RNFL demonstrates form birefringence that originates from anisotropic cylindrically shaped cellular structures in the RGC axons.
8,9 The major cylindrical structures of the RGC axonal cytoskeleton are neurotubules (NT), neurofilaments, and neurotubule-associated proteins.
10 Huang and Knighton
5 identify neurotubules as the source of birefringence from the RNFL. Theoretical analysis has attributed RNFL reflectance to the cylindrically shaped mitochondria and axonal membranes.
9
It is postulated that either changes in neurotubule density of RNFL bundles or neurotubule packing densities within the axons themselves are responsible for the differences in birefringence surrounding the ONH.
11 Neurotubule density (ρ
RNFL) is defined in this report as a scalar estimate of the number of neurotubules per unit area of RNFL tissue (NT/μm
2). There is strong evidence that the regional characteristic ρ
RNFL surrounding the optic nerve head (ONH) is a source of birefringence,
5,12,13 but it has not been clear whether ρ
RNFL is the only source of birefringence.
9 RNFL birefringence has been investigated as a possible diagnostic to detect early subcellular changes in glaucoma before there is any measurable change in RNFL thickness.
5,12,13 Fortune et al.
13 injected colchicine into the vitreous of nonhuman primate eyes and observed neurotubule disruption with a reduction of RNFL birefringence without any accompanying change in RNFL thickness. These results show that decreases in the number of neurotubules occur before thinning of the RNFL, and in situ measurement of ρ
RNFL can be used as a diagnostic for cytoskeletal changes in RGC axons.
13 In this study, we compared the measured birefringence signal in the peripapillary retina with the corresponding measured anatomic features to explore the origin of the RNFL birefringence.
The retinas of two healthy 6-year-old female, 5.9 and 7.7 kg, cynomolgus monkeys (subjects 1853 and 57204) were imaged over a period of 62 days. Intraocular pressures and subjective visual function were normal. All experimental procedures were approved by The University of Texas at Austin Institutional Animal Care and Use Committee (IACUC, Protocol 05021401) and conformed to all United States Department of Agriculture (USDA), National Institutes of Health (NIH) guidelines, and the ARVO Statement for the Use of Animals in Ophthalmic and Vision Research. A combination of IM ketamine (10 mg/kg) and xylazine (0.25 mg/kg) was used to anesthetize the monkeys, and anesthesia levels were monitored by a certified veterinary technologist. A retrobulbar injection of 0.5% xylocaine and 0.375% marcaine was given to immobilize the eye that was imaged. Pupils were dilated by using 1 drop of 1% cyclopentolate and 1 drop of 1% tropicamide. One drop of 10% methylcellulose, to prevent dehydration, was placed in the eye to be imaged, and a contact lens was placed on that eye. A contact lens that rendered the monkey slightly myopic was used to ensure that light was focused on the internal limiting membrane (ILM).
The peripapillary RNFL thickness (
Z RNFL) and single-pass phase retardation maps of the two cynomolgus monkeys were measured by using an enhanced polarization-sensitive optical coherence tomography (EPS-OCT) system described previously.
11,14 EPS-OCT consists of a PS-OCT instrument combined with a nonlinear fitting algorithm to determine PR and Δ
n with high sensitivity in weakly birefringent tissues. The system utilizes a mode-locked Ti:Al
2O
3 laser source (λ
0 = 830 nm, Δλ = 55 nm) linearly polarized at 45°. The
Z RNFL and PR maps are used to construct phase retardation per unit depth (
PR/
UD) area maps given in units of degrees of retardation per 100 μm of RNFL thickness (degrees/per 100 μm) by dividing local PR by
Z RNFL.
The PR map was measured in an area and ring scan configuration. Each area map consisted of 24 evenly spaced (15°) radial scans containing 2, 6, or 8 clusters distributed uniformly between 1.4 and 1.9 mm from the center of the optic nerve head. A cluster comprised 36 or 64 A-scans individually acquired over a respective 0.9- or 1.6-mm2 area. Ring scans are derived from sector scans spread 5° apart. The right eye of each subject was imaged twice on separate days, to assess reproducibility of retinal birefringence measurements.
A single peripapillary map was acquired in approximately 45 minutes. Laser power incident on the cornea was 2.8 mW during lateral scanning and 1.7 mW while stationary for both scan configurations. Approximate laser spot size at the retinal surface was 30 μm. Axial resolution was 5 μm (determined by the coherence length of the laser source in air).
Two days after EPS-OCT imaging was completed, both monkeys were anesthetized and transcardially perfused with a fixative solution (pH 7.4) consisting of 2.5% glutaraldehyde and 2% paraformaldehyde in 0.1 M sodium phosphate buffer. Each animal was first brought down to a surgical level of anesthesia with a combination of IM ketamine (10 mg/kg) and xylazine (0.5 mg/kg). Pentobarbital sodium (10 mg/kg) was given first for surgical anesthesia and then an IV overdose was administered.
After each perfusion was complete, all four eyes were enucleated and immersed in 180 mL of the primary fixative solution from 1 to 3 hours before dissection from the periorbital tissue and removal of the posterior hemisphere of the eye. A 360° incision was made at the ora serrata, and the anterior eye structures including the ciliary body, iris, lens, and cornea were removed from the posterior eye cup. A notch and suture placed in the nasal sclera before enucleation remained visible throughout the specimen preparation process to maintain proper orientation. All posterior eye cups were then simultaneously immersed in 180 mL of the primary fixative solution for approximately 1.5 hours.
Eye cups were washed in three 30-minute changes of 0.1 M sodium phosphate buffer (180 mL each, pH 7.4) and postfixed in 90 mL of 2% osmium tetroxide (aqueous) solution for 1 hour. They were washed again two times for 30 minutes per wash in 0.1 M sodium phosphate buffer (180 mL each, pH 7.4) and then one more time in 180 mL of distilled water for 30 minutes. The eye cups were then dehydrated through a series of increasing ethanol concentration solutions (50% for 14 hours, 75% for 1 hour, 100% for 1 hour, and 100% for 1 hour, all in 180 mL) followed by two immersions in acetone (50 mL 100% acetone for 1 hour each). The posterior eye cups were then infused with 1:3 low-viscosity resin (EMBed-812; Electron Microscopy Sciences, Hatfield, PA) in acetone for 1 hour, after which they were covered and left in 2:3 resin for 19 hours overnight. The following day, the eye cups were placed into fresh solutions of 100% resin and left in uncovered containers for approximately 5 hours. They were then placed anterior side down into cubical embedding molds. The molds were put into a 60°C oven for 21 hours overnight, during which the resin solution polymerized, and the eye cups were removed the following day.
Superficial lines intersecting at the center of the ONH profile were used to divide the cube mold of the embedded eye into wedge-shaped angular sections. Each sample wedge was carefully carved from the cube to prevent excess tissue removal surrounding the ONH. Glass knives were used to create a flat rectangular block face (500 × 300 μm).
Ultrathin and semithin sections were sampled 1.6 to 1.9 mm from the ONH in regions (Ultracut UCT Ultramicrotome; Leica Microsystems GmbH, Ernst-Leitz-Strasse, Germany). Semithin sections (0.5 μm) were cut and stained with toluidine blue before ultrathin sections (60 nm) to ensure that the block's orientation on the microtome would result in transverse cuts. Several ultrathin sections were placed on copper, α-numeric–indexed grids (Electron Microscopy Sciences) and stained with 2% uranium acetate and 0.3% lead citrate before TEM analysis.
Gray-scale digital images were captured on a transmission electron microscope (EM208 TEM; Phillips, Eindhoven, The Netherlands) equipped with a digital camera system (Advantage HR 1 MB; AMT, Danvers, MA). Each bundle was photographed at low (2,200×–2,800×), medium (11,000×–14,000×), and high (28,000×–44,000×) magnification.
Nonsparse Axons.
Sparse Axons.
Radial area and ring scan
PR/
UD measurements falling within an angular section were averaged, resulting in an equal number of
PR/
UD values for every mean ρ
RNFL. The averaged
PR/
UD measurements for subjects 1853 and 57204 resulted in ±22.5° and ±11.25° of angular error, respectively. Average
PR/
UD measurement positions were optimally registered with angular RGC axon organelle mean measurements to compute the correlation between them (
Fig. 5). The shift was used to avoid
PR/
UD and ρ
RNFL measurement positions taken at angular boundaries between sections in both subjects.
Two approaches were used to find a correlation between PR/UD and RGC organelles. The first approach was a Pearson product moment correlation. Correlation coefficients and significance values were computed (SAS ver. 9; SAS, Cary, NC).
A multilevel modeling technique was used for the second approach, since it allows PR/UD and RGC organelles to be correlated on two levels so that finer angular resolution of PR/UD measurements could be preserved. Multilevel modeling was implemented through the procedure PROC MIXED within the statistical analysis software. The model accounts for the random effect of angular position of PR/UD measurements.
Subject 57204 had a correlation coefficient of 0.67 (
P = 0.005) between
PR/
UD and ρ
RNFL (
Table 4), and the multilevel model resulted in standardized regression coefficients of 0.50 (
P = 0.04). The averaged pattern of
PR/
UD is shown superimposed on respective ρ
RNFL for both subjects in
Figure 9.
Table 4. Correlation between PR/UD and ρRNFL in Subject 57204
Table 4. Correlation between PR/UD and ρRNFL in Subject 57204
Statistical Model | r | P |
Pearson's correlation | 0.67 | 0.005 |
Multilevel model | 0.5 | 0.04 |
Morphologic measurements from TEM images were used to estimate mean values of axoplasmic area (A x) mode, axon area (A a) mode, slope (u) of neurotubule number versus axoplasmic area (neurotubule packing density), fractional area of axoplasm in the nerve fiber bundle (f x), mitochondrial fractional area in the nerve fiber bundle (x m), mitochondria-containing axon profile fraction (m p), and length of axonal membrane profiles per unit nerve fiber bundle (L am/A b).
Pearson product moment correlation coefficients of the morphologic parameters with
PR/
UD are summarized in
Table 5. Correlation coefficients of
r = 0.81 (
P = 0.01) and
r = 0.5 (
P = 0.05) were observed between
PR/
UD and mean
A x mode in subjects 1853 and 57204 (
Fig. 10), respectively. Mean
A x mode values were similar in the superior and inferior portions of both eyes and were larger than temporal and nasal portions. Mean
A a and
PR/
UD yielded a significant correlation coefficient of
r = 0.79 (
P = 0.01) in subject 1853 (
Fig. 10B).
Table 5. RGC Morphologic measurements Correlated with Phase Retardation Per Unit Depth (PR/UD, Proportional to Birefringence) for Subjects 57205 and 1853
Table 5. RGC Morphologic measurements Correlated with Phase Retardation Per Unit Depth (PR/UD, Proportional to Birefringence) for Subjects 57205 and 1853
RGC Axon Morphologic Measurement | Abbreviation | 57204 OD | 1853 OS |
r | P | r | P |
Least-squares linear slope (number of NTs per unit Ax area), NT/μm2 | Mean u | 0.70* | 0.0028 | 0.68 | 0.0941 |
Mean RGC axoplasmic area mode, μm2 | Mean A x | 0.50* | 0.0500 | 0.81* | 0.0145 |
Mean axon area mode, μm2 | Mean A a | 0.47 | 0.0600 | 0.79* | 0.0184 |
Neurotubule density (number of NTs per unit RNFL area), NT/μm2 | Mean ρRNFL | 0.67* | 0.0050 | 0.61 | 0.1077 |
Axoplasmic fractional area (per unit RNFL bundle area), % | Mean f | 0.34 | 0.1924 | 0.51 | 0.1934 |
Mitochondrial fractional area (per unit RNFL bundle area), % | Mean x m | 0.02 | 0.9500 | — | — |
Mitochondria-containing axon profile fraction (per unit RNFL bundle area), % | Mean m p | — | — | 0.24 | 0.5708 |
Axonal membrane length (per unit RNFL bundle area), μm−1 | Mean L am/A b | 0.24 | 0.3670 | 0.23 | 0.5811 |
In subject 57204, a significant correlation coefficient of
r = 0.7 (
P = 0.002) was observed between section averaged
PR/
UD and the
k versus
A x regression fit slope (
u) that is used as a measure of neurotubule packing density (
Fig. 11). Arcuate bundle regions had the highest packing density, followed by the nasal region, and last the papillomacular region.
Our findings further support the hypothesis that neurotubules are the primary source of birefringence in the RNFL. The strongest correlation between Δn and PR/UD (P = 0.0028) for all the morphologic parameters studied was the slope (u) of the regression fit of neurotubule number (k) versus axoplasmic area (A x), which represents the neurotubule packing density.
Supported by Grant R01EY016462-01A1 from the National Eye Institute at the National Institutes of Health and Long Term Full Time Program Grant BV0700313000. Any opinions, interpretations, conclusions, and recommendations are not necessarily endorsed by the U.S. Air Force.
Disclosure:
G.M. Pocock, None;
R.G. Aranibar, None;
N.J. Kemp, None;
C.S. Specht, None;
M.K. Markey, None;
H.G. Rylander III, None
The publication costs of this article were defrayed in part by page charge payment. This article must therefore be marked “
advertisement” in accordance with 18 U.S.C. §1734 solely to indicate this fact.
The authors thank Matt Hersh and the Graduate Student's Fellows Program run by The University of Texas at Austin's Division of Statistics and Scientific Computation for their review of the manuscript and Maura Boyle for technical assistance.