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NIHPA Author Manuscripts logoLink to NIHPA Author Manuscripts
. Author manuscript; available in PMC: 2018 May 1.
Published in final edited form as: J Glaucoma. 2017 May;26(5):450–458. doi: 10.1097/IJG.0000000000000647

Enhanced Diagnostic Capability for Glaucoma of 3-Dimensional versus 2-Dimensional Neuroretinal Rim Parameters Using Spectral Domain Optical Coherence Tomography

Kenneth Chen Fan 1,2, Edem Tsikata 2,3, Ziad Khoueir 2,3,4, Huseyin Simavli 2,3,5, Rong Guo 2,3, Regina DeLuna 2,6, Sumir Pandit 3, Christian John Que 2,3,7,8, Johannes F de Boer 2,3,9,10, Teresa C Chen 2,3
PMCID: PMC5408323  NIHMSID: NIHMS846245  PMID: 28234677

Abstract

Purpose

To compare the diagnostic capability of 3-dimensional (3D) neuroretinal rim parameters with existing 2-dimensional (2D) neuroretinal and retinal nerve fiber layer (RNFL) thickness rim parameters using spectral domain optical coherence tomography (SD-OCT) volume scans

Materials and Methods

Design

Institutional prospective pilot study.

Study population

65 subjects (35 open angle glaucoma patients, 30 normal patients).

Observation procedures

One eye of each subject was included. SD-OCT was used to obtain 2D retinal nerve fiber layer (RNFL) thickness values and five neuroretinal rim parameters [i.e. 3D minimum distance band (MDB) thickness, 3D Bruch’s membrane opening-minimum rim width (BMO-MRW), 3D rim volume, 2D rim area, and 2D rim thickness].

Main outcome measures

Area under the receiver operating characteristic (AUROC) curve values, sensitivity, specificity.

Results

Comparing all 3D with all 2D parameters, 3D rim parameters (MDB, BMO-MRW, rim volume) generally had higher AUROC curve values (range 0.770–0.946) compared to 2D parameters (RNFL thickness, rim area, rim thickness; range 0.678–0.911). For global region analyses, all 3D rim parameters (BMO-MRW, rim volume, MDB) were equal to or better than 2D parameters (RNFL thickness, rim area, rim thickness; p-values from 0.023–1.0). Among the three 3D rim parameters (MDB, BMO-MRW, and rim volume), there were no significant differences in diagnostic capability (false discovery rate > 0.05 at 95% specificity).

Conclusion

3D neuroretinal rim parameters (MDB, BMO-MRW, and rim volume) demonstrated better diagnostic capability for primary and secondary open angle glaucomas compared to 2D neuroretinal parameters (rim area, rim thickness). Compared to 2D RNFL thickness, 3D neuroretinal rim parameters have the same or better diagnostic capability.

Keywords: primary open angle glaucoma, spectral domain optical coherence tomography, 3-dimensional volume scan, minimum distance band, Bruch’s membrane opening-minimum rim width

Introduction

Glaucoma is the leading cause of irreversible blindness in the world, currently affecting over 62.2 million people globally and over 3.3 million in North America.1 Spectral Domain OCT (SD-OCT) has replaced time domain optical coherence tomography (TD-OCT) as the most widely used quantitative structural assessment of the optic nerve head (ONH) and the surrounding retinal nerve fiber layer (RNFL) for glaucoma.2 These structural parameters remain essential in evaluating glaucoma since structural changes such as RNFL thinning often precede visual field deficits.3,4 However, despite the advent of the newer 3-dimensional (3D) technical capabilities of SD-OCT, commensurate 3D software development has lagged behind; and current commercially available SD-OCT 3D software for glaucoma care needs further development.

Perhaps the most common SD-OCT imaging scan in glaucoma is the 2-dimensional (2D) peripapillary retinal nerve fiber layer (RNFL) circle scan centered on the ONH. This methodology has some inherent diagnostic limitations due to ONH anatomical variability, myopia, glaucomatous RNFL reflectivity loss, peripapillary atrophy, and other issues.515 For ONH evaluation, assessment has classically been quantified by the cup-to-disc ratio (CDR), and OCT can assess CDR by using a reference plane 150 microns above the retinal pigmented epithelium (RPE)/Bruch’s Membrane (BM) complex. However, these assessments are often unreliable due to variability of cup anatomy.2,16 Furthermore, CDR assessment by OCT scanning reports can be approximately 0.1 higher than that determined clinically by glaucoma specialists.17 In terms of future directions for OCT structural evaluation, studies have shown that 3D imaging parameters can demonstrate at least the same diagnostic capabilities as 2D RNFL thickness, can improve diagnostic sensitivity of glaucoma at 95% specificity, can track glaucomatous changes of acute intraocular pressure (IOP) elevation in non-human primate models, and can longitudinally evaluate structural changes secondary to glaucoma.1823 Therefore, there is clearly a need to develop and test 3D SD-OCT methods for interpreting glaucomatous neuroretinal rim changes,24 because 3D algorithms may hold better potential than 2D methods for detecting subtle structural changes in the clinic.

Given the diagnostic potential of 3D imaging from past studies,1820,2227 this study investigated five neuroretinal rim parameters to determine the best method of analyzing 3D volume data. This study specifically features 2 newer 3D neuroretinal rim parameters: the Bruch’s Membrane Opening – Minimum Rim Width (BMO-MRW) and the “minimum distance band” (MDB) thickness. Using an SD-OCT radial scan protocol, past studies have defined the BMO-MRW as the neuroretinal rim bound by the shortest distance from BMO to the cup surface19,20 and have demonstrate a stronger structure-function relationship in glaucomatous eyes with the BMO-MRW compared to RNFL thickness and other 2D parameters.28 Using an SD-OCT raster volume scan protocol, our group has previously reported the MDB neuroretinal thickness parameter, which is a circular band that is bound by the shortest distance between the termination of the RPE/BM complex and the closest corresponding points along the cup surface.2,29 Under this same SD-OCT raster volume scan protocol, we were also able to examine older 150 micron reference plane based neuroretinal rim tissue parameters including rim area, rim volume, and rim thickness. We hypothesize that newer 3D neuroretinal rim parameters (e.g. MDB, BMO-MRW) are better at diagnosing glaucoma than the classic 2D parameters used today and that different SD-OCT scanning methods can offer new and additional parameters for ONH evaluation. Therefore, in this study, we evaluated the diagnostic capabilities of 3D and 2D neuroretinal parameters as well as 2D RNFL thickness from SD-OCT imaging in a group of primary and secondary open angle glaucoma (POAG) and normal patients who were imaged with the Spectralis instrument (Heidelberg Engineering, Heidelberg, Germany).

Materials and Methods

Participants and Examinations

All study subjects were recruited from the Glaucoma Service at the Massachusetts Eye and Ear Infirmary between September 2014 and June 2015 as part of a study approved by the Massachusetts Eye and Ear Infirmary institutional review board. All included patients provided informed consent in accordance with the Declaration of Helsinki for research involving human subjects as well as the Health Insurance Portability and Accountability Act Regulations. A glaucoma specialist (T.C.C.) examined all patients. Each patient’s clinic visit documentation included history of present illness, best corrected visual acuity, refraction, slit-lamp examination, Goldmann applanation tonometry, gonioscopy, and dilated ophthalmoscopy. All imaging and diagnostic procedures were performed for all patients on the same day and included Spectralis OCT imaging, stereo disc photography (Visucam Pro NM; Carl Zeiss Meditec, Inc.), and Humphrey visual field (HVF) testing (Swedish Interactive Threshold Algorithm 24-2 test of the Humphrey visual field analyzer 750i; Carl Zeiss Meditec, Inc.). Only one eye per patient was included in the study.

All patients were dilated for imaging (HRA/Spectralis software version 5.4.8.0). We performed three imaging protocols on each subject on the same day including: (1) circle scan for RNFL thickness; (2) 20 × 20-degree raster volume scan of the ONH for MDB thickness, rim volume, rim area, and rim thickness measurements.; (3) radial scan of the ONH for BMO-MRW measurements, with manual correction of the BMO border in the clinic. Scans were only included if images: (1) had a signal strength ≥ 15 (range 0–40);30 (2) had clear visibility of the fundus, optic disc, and RNFL; and (3) were continuous without significant blank areas. The automatic real-time (ART) eye-tracking system of the Spectralis OCT allowed for averaging of multiple scans at the same location.

From the three imaging protocols, we were able to investigate six diagnostic parameters: 2D RNFL thickness, 2D neuroretinal rim area, 2D neuroretinal rim thickness, 3D neuroretinal rim volume, 3D MDB thickness, and 3D BMO-MRW. RNFL thickness was determined by Heidelberg software and was obtained from Heidelberg Spectralis Exam Reports. The neuroretinal rim parameters (i.e. rim volume, rim area, rim thickness) and MDB thickness were calculated from the 3D ONH raster volume scans with software developed at the Massachusetts Eye and Ear Infirmary (Figures 1 & 2). This scan protocol consisted of 193 raster images over a region approximately 6 mm × 6 mm. The RPE/BM complex (Figure 1A, pink dotted circle) and the cup surface (Figure 1B, yellow dotted circle) were reconstructed by segmenting the images. In accordance with previous definitions of the RPE/BM complex, we segmented the RPE/BM complex when we were able to identify either just the RPE, or just the BM, or both the RPE and BM.31 For rim volume, rim area, and rim thickness, the traditional reference surface of 150 microns above the RPE/BM complex was used to calculate the ONH parameters (Figure 1C with 150 micron reference plane represented by yellow letter Z).16,32 Rim volume was calculated by measuring the tissue bounded below by the 150 micron reference surface, above by the ILM, and radially by the RPE/BM complex). The rim area (Figure 2A) was the projection of the rim volume (Figures 2B and 2C) on a transverse plane. The rim thickness was the rim volume divided by the rim area. The MDB thickness was calculated by measuring the shortest distances from 100 points along the RPE/BM complex to the cup surface (Figure 1D) and has been previously described in detail by our group in recent publications.33,34 The BMO-MRW thickness was determined from the 24 radial B-scan protocol, using the Glaucoma Premium Module software (6.0.11) seen in Figure 3. The BMO-MRW is defined by the minimum distance between the Bruch’s Membrane Opening and the ILM.19,35 The Glaucoma Premium Module software is commercially available and is FDA approved. For each of the 6 parameters, we measured a total of 9 regions: global, 4 quadrants (inferior, superior, nasal, temporal), and four 45 degree sectors (inferonasal, superonasal, inferotemporal, superotemporal).

Figure 1.

Figure 1

Depiction of how neuroretinal rim parameters were derived from the raster volume scan protocol. This example is of a normal right eye. After volume scans were obtained with Spectralis optic coherence tomography (OCT) imaging (HRA/Spectralis software version 1.9.1.0, Heidelberg Engineering, Heidelberg, Germany), custom-designed Massachusetts Eye and Ear Infirmary software calculated (1a – 1c) rim area, rim volume, and rim thickness and (1b and 1d) minimum distance band (MDB) thickness. In 1A, the pink dotted circle represents the OCT-based disc border, or retinal pigmented epithelium (RPE)/Bruch’s membrane (BM) complex termination. In picture 1B, the yellow dotted circle represents the cup surface points which are closest to the OCT-based RPE/BM complex border, which defines the outer MDB border (1D pink dotted circle). Picture 1C displays a B-scan, where yellow letter Y represents the RPE/BM complex plane, and yellow letter Z represents the 150μm reference plane which is 150μm above the RPE/BM complex and which divides the neuroretinal rim above from the cup below. 1D depicts the MDB as a 360-degree circumferential blue band, which is bordered above by the cup surface (blue dotted circle) and below by the OCT-based RPE/BM complex (pink dotted circle).

Figure 2.

Figure 2

Depiction of neuroretinal rim parameters derived from the raster volume scan protocol (i.e. neuroretinal rim volume, rim thickness, and rim area). This example is the normal right eye who had volume scans using Spectralis optic coherence tomography (OCT) imaging (HRA/Spectralis software version 1.9.1.0, Heidelberg Engineering, Heidelberg, Germany). Using our custom-designed algorithm, the OCT-based retinal pigmented epithelium (RPE)/Bruch’s membrane (BM) complex border is shown as pink dotted circles in Figure 2 (A–C) and represents the termination of the retinal pigmented epithelium (RPE)/Bruch’s membrane (BM) complex. In 2A, the integrated reflectance image shows the rim area in yellow. 2B and 2C are both 3-dimensional representations of rim volume, which is 150 microns above the OCT-based RPE/BM complex border (pink dotted circles).

Figure 3.

Figure 3

Representative integrated reflectance image (A) and associated B-scan (B) of the Bruch’s membrane opening-minimum rim width (BMO-MRW) scan protocol from Heidelberg Spectralis OCT (HRA/Spectralis software version 1.9.1.0, Heidelberg Engineering GmbH, Heidelberg, Germany). In picture A, the 24 radial B-scan protocol for measuring the BMO-MRW is shown. The highlighted green line represents the radial B-scan shown on the right in picture B. Picture B demonstrates that the BMO-MRW is a measurement of the minimum distance (light blue arrows) between the internal limiting membrane (ILM) and Bruch’s membrane opening (BMO).

The inclusion criteria for this study were as follows: (1) patients who received a dilated eye exam, disc photos, HVF testing, Spectralis RNFL scan, SD-OCT 3D ONH raster volume scan, and Spectralis BMO-MRW scans on the same day; (2) spherical equivalent between −5.0 diopters (D) to +5.0 D inclusive; and (3) reliable HVF test results with ≤ 33% fixation losses, ≤ 20% false-positive results, and ≤ 20% false-negative results. Patients were excluded from the study if there was presence of congenital anomalies of the anterior chamber, corneal scarring or opacities, HVF loss attributable to a non-glaucoma condition, such as central retinal vein or artery occlusion or pan-retinal photocoagulation, dilated pupillary diameter less than 2mm, or severe non-proliferative or proliferative diabetic retinopathy. Only patients with best corrected visual acuity of 20/50 or better were included in this study.

In selecting glaucoma subjects for this study, we included primary and secondary forms of open angle glaucoma. The following types of open angle glaucoma were included: primary open angle glaucoma, normal tension glaucoma, pseudoexfoliation glaucoma, and pigmentary glaucoma. Any patient diagnosed with chronic angle closure glaucoma, traumatic glaucoma, aphakic glaucoma, juvenile open angle glaucoma, or uveitic glaucoma was excluded from the study. All diagnoses were confirmed by a glaucoma specialist (T.C.C.). To qualify for a diagnosis of glaucoma, an abnormal VF was defined by either 3 or more contiguous pattern standard deviation (PSD) test locations depressed by 5 decibel (dB) or more; or 2 or more contiguous PSD test locations with one depressed by 10dB or more and the other by 5 dB or more. Abnormal PSD test locations on the outer rim of the visual field were not considered in the aforementioned criteria in order to account for peripheral rim artifacts.

For normal subjects, patients were included if they satisfied the following criteria: (1) absence of other ocular disease with the exception of mild cataracts; (2) normal HVF test results as defined by hemifield test results within normal limits; and (3) CDR asymmetry ≤ 0.2 between eyes. No patients with physiologic cupping were included, and CDRs for Caucasians were ≤ 0.4 and for African-Americans and Hispanics ≤ 0.6.

For patients where both eyes were eligible for inclusion, one eye was selected at random using the Microsoft Excel 2010 random number generator function “=RANDBETWEEN(min,max).” Defining “min” as “1,” and “max” as “2,” we assigned the value “1” to indicate selection of the left eye and “2” to indicate selection of the right eye.

Statistical Analysis

Results are reported as means +/− standard deviation, unless otherwise stated. Chi-square or two sample t-tests were used for the comparison of demographic variables between normal and glaucoma patients.

For all 9 regions of our 6 parameters (RNFL thickness, MDB thickness, rim area, rim volume, rim thickness, BMO-MRW), we determined area under the receiver operating characteristic (AUROC) curve values. To find the most accurate diagnostic parameter for glaucoma, AUROC curve values were evaluated with pairwise comparisons, and false discovery rates were calculated to adjust for the multiple comparisons. P-values less than 0.05 were considered statistically significant. All statistical analyses were performed using SAS 9.4 (SAS Institute Inc., Cary, NC).

Results

There were 65 patients in our study, 35 glaucoma subjects and 30 normal subjects, with mean age of 67.7 ± 11.0 and 58.5 ± 12.0 years, respectively (p-value < 0.01, Table 1). Statistically significant differences were also found in clinically assessed CDR as well as HVF mean and pattern standard deviation (Table 1). Of the glaucoma subjects, 51.4% (18/35) were categorized as early glaucoma (HVF mean deviation greater than −6 dB, inclusive) and 48.6% (17/35) as moderate to severe glaucoma (HVF mean deviation worse than −6 dB).

Table 1.

Demographics of the Primary Open-Angle Glaucoma and Normal Study Populations

POAG Normal p-value
Number of Eyes 35 30
Number of Right Eyes/Left Eyes 20/15 11/19
Gender (Male/Female) 18/17 13/17 0.515
Age (years) 67.7 ± 11.0 58.5 ± 12.0 0.002
Refractive Error (Spherical Equivalent D) −0.20 ± 1.62 −0.76 ± 1.88 0.202
Cup to Disc Ratioa 0.67 ± 0.17 0.4 ± 0.18 < 0.0001
Visual Fieldb
 Mean Deviation (dB) −8.15 ± 7.35 −1.78 ± 1.88 < 0.0001
 Pattern Standard Deviation (dB) 6.29 ± 3.82 1.78 ± 0.79 < 0.0001
Race 35 30 0.811
 White 4 3
 Black 22 22
 Asian 7 4
 Hispanic 1 0
 Other 1 1

D = diopter, dB = decibel, POAG = primary open-angle glaucoma

a

Cup to Disc Ratio as performed via clinical assessment by trained ophthalmologist

b

Visual field data obtained through Humphrey’s Visual Field testing

”Other” racial group represents a patient of unspecified European descent

All results are described in the format of mean ± standard deviation unless indicated otherwise

Table 2 shows the AUROC values for all 9 regions for the 6 parameters investigated in our cohort. Four of the 5 top AUROC curve values were for 3D parameters: BMO-MRW inferotemporal (0.946 [95% CI 0.89–0.99]), BMO-MRW global (0.928 [95% CI, 0.86–0.99]), BMO-MRW inferior (0.927 [0.86–0.99]), rim volume inferotemporal (0.917 [0.85–0.99]), and rim thickness inferotemporal (0.911 [0.84–0.99]). As seen in Table 2, global values of 3D rim parameters (BMO-MRW, rim volume, MDB thickness) were equal to or better than 2D parameters (RNFL thickness, rim area, rim thickness; p-values ranging from 0.023 – 1.0). In comparisons for diagnostic ability of the 3D rim parameters as determined by AUROC values using false discovery rates, no statistically significant differences were detected. When pairwise comparisons were done between 3D and 2D parameters for global and quadrant regions, we found that 3D parameters were similar to 2D parameters, except for the following pairs: 3D BMO-MRW better than 2D RNFL (nasal p=0.035, temporal p=0.037), 3D BMO-MRW better than 2D rim area (global p=0.023, inferior p=0.009, temporal p=0.036), 3D BMO-MRW better than 2D rim thickness (superior p=0.014, nasal p=0.031, temporal p=0.036), and 3D rim volume better than 2D rim area (inferior p=0.018).

Table 2.

Comparison of Diagnostic Capability of Retinal Nerve Fiber Layer and Five Neuroretinal Rim Ocular Coherence Tomography Parameters for Primary Open Angle Glaucoma

2D RNFL Thickness 3D MDB Thickness 3D BMO-MRW 3D Rim Volume 2D Rim Area 2D Rim Thickness
AUROC (SE) AUROC (SE) AUROC (SE) AUROC (SE) AUROC (SE) AUROC (SE)
Global 0.850 (0.046) 0.884 (0.045) 0.928 (0.036) 0.892 (0.042) 0.837 (0.050) 0.884 (0.043)
Inferior 0.875 (0.043) 0.903 (0.042) 0.927 (0.036) 0.905 (0.040) 0.821 (0.051) 0.910 (0.039)
Superior 0.816 (0.052) 0.811 (0.056) 0.875 (0.042) 0.842 (0.050) 0.792 (0.058) 0.793 (0.056)
Nasal 0.721 (0.065) 0.831 (0.053) 0.867 (0.045) 0.835 (0.050) 0.815 (0.054) 0.795 (0.055)
Temporal 0.678 (0.067) 0.796 (0.054) 0.838 (0.049) 0.770 (0.058) 0.735 (0.061) 0.725 (0.063)
Superotemporal 0.818 (0.053) 0.790 (0.057) 0.877 (0.042) 0.830 (0.050) 0.783 (0.059) 0.799 (0.054)
Inferotemporal 0.869 (0.046) 0.885 (0.043) 0.946 (0.026) 0.917 (0.036) 0.818 (0.053) 0.911 (0.038)
Superonasal 0.760 (0.059) 0.823 (0.056) 0.870 (0.043) 0.819 (0.056) 0.783 (0.060) 0.776 (0.060)
Inferonasal 0.806 (0.055) 0.889 (0.044) 0.902 (0.041) 0.871 (0.046) 0.803 (0.053) 0.861 (0.047)

2D = 2-dimensional, 3D = 3-dimensional

BMO-MRW = Bruch’s Membrane Opening - Minimum Rim Width

POAG = Primary Open-Angle Glaucoma

RNFL = Retinal Nerve Fiber Layer, MDB = Minimum Distance Band

All results are described in the format of mean (SE = standard error) unless indicated otherwise

Figures 4 and 5 depict the AUROC graphs for visual comparison between RNFL, BMO-MRW, MDB, and RNFL thickness, demonstrating that at approximately 95% specificity, BMO-MRW, MDB thickness, rim volume, and RNFL thickness yielded sensitivity values of 86%, 83%, 68%, and 60%, respectively. Figure 5 shows the AUROC curves for MDB thickness, BMO-MRW, rim volume, and RNFL for the 4 quadrants and 4 sectors. In Figure 5, there is a trend for RNFL thickness having lower total AUROC curves as compared to all three 3D neuroretinal rim parameters (i.e. MDB thickness, BMO-MRW, rim volume).

Figure 4.

Figure 4

The diagnostic capabilities and area under the receiver operating characteristic (ROC) curves for gold standard 2-dimensional retinal nerve fiber layer (RNFL) versus 3-dimensional (3D) global neuroretinal rim parameters [Bruch’s membrane opening-minimum rim width (BMO-MRW), minimum distance band (MDB), rim volume].

Three-dimensional (3D), two-dimensional (2D), minimum distance band (MDB), Bruch’s membrane opening minimum rim width (BMO-MRW), retinal nerve fiber layer (RNFL) thickness.

Figure 5.

Figure 5

The diagnostic ability and area under the receiver operating characteristic (AUROC) curves for gold standard 2-dimensional retinal nerve fiber layer thickness (RNFL) versus 3-dimensional (3D) neuroretinal rim parameters [Bruch’s membrane opening-minimum rim width (BMO-MRW), minimum distance band (MDB), rim volume]. The eight regions depicted include 4 quadrants (i.e. inferior, superior, nasal, temporal) and 4 sectors (i.e. superotemporal, inferotemporal, superonasal, and inferonasal).

Three-dimensional (3D), two-dimensional (2D), minimum distance band (MDB), Bruch’s membrane opening minimum rim width (BMO-MRW), retinal nerve fiber layer (RNFL) thickness.

Discussion

Our study demonstrates that 3D neuroretinal rim parameters obtained by SD-OCT imaging may be superior to 2D SD-OCT diagnostic tools in differentiating glaucoma from normal patients. Similar to patterns established in previous studies,36,37 we also found that the inferior quadrant and inferotemporal sector more consistently exhibited higher diagnostic capabilities compared to other regions for all 6 measured parameters (Table 2).9,22,3841 Using AUROC curves as an indicator for diagnostic capability, our results illustrate that the diagnostic performance of these 3D neuroretinal rim parameters (i.e. MDB thickness, BMO-MRW, rim volume) exceeds that of 2D RNFL thickness in almost all quadrants and sectors (Table 2). Also, Figures 4 and 5 illustrate a trend that sensitivity and AUROC curve values for these 3D neuroretinal rim parameters were superior to the 2D RNFL parameter. Based on our results, the development of new 3D SD-OCT parameters may augment or supplement the diagnostic capability of existing SD-OCT parameters, such as 2D RNFL thickness.

Multiple groups have acknowledged the advantages of 3D OCT imaging as well as the disadvantages of 2D RNFL thickness measurements in glaucoma. For example, groups have suggested that the 3D BMO-MRW not only may have better diagnostic capability compared to 2D RNFL thickness in humans (AUROC 0.96 vs. 0.92, respectively)19 but may also have better structure-function correlation with visual field defects (p < 0.01).25,28 Our group has also shown that peripapillary retinal thickness parameters derived from 3D volume scans have excellent diagnostic capability with fewer algorithmic errors for detecting glaucoma as compared to peripapillary RNFL thickness (p = 0.03).22 According to this22 and other papers, the performance of many 3D imaging parameters are not as affected by RNFL reflectivity loss, myopia, and peripapillary atrophy (PPA) in preliminary investigations.9,42 Unlike some 3D parameters, the reliability of RNFL thickness as a diagnostic indicator decreases in such scenarios, for example when there is PPA or RNFL reflectivity loss due to advanced glaucoma, or when measurements are made in nasal quadrants.6,8,9 Additionally, RNFL thickness is measured around a 3.4 mm or more diameter circle centered on the ONH.5,7,9,21 However, the lack of a true anatomical landmark as the focal center for circle scans allows for inaccuracies in RNFL measurements due to de-centration,19,21 which has been reported in even 27.8% of RNFL scans.43 It has been reported that for mild to advanced glaucoma, 70% to 94% of RNFL defects are diffuse in nature with some patients exhibiting changes only nearer to the RPE/BM complex.18 As such, measuring at a fixed distance from the disc can lead to misdiagnosis in certain patients, because there are individual as well as ethnic variations in disc size and because the RNFL is normally thicker closer to the RPE/BM complex. Unlike 2D RNFL circle scans, 3D parameters (i.e. MDB thickness, rim volume) described in this study are derived from 20 × 20 degree ONH volume raster scans that are capable of gathering data from the entire retina surrounding the ONH. These volume scans do not face the same limitations as RNFL thickness and can be considered as the next step for diagnostic imaging in glaucoma, because 3D volume scans are not as affected by an artifact in a single frame compared to a 2D scan which consists of just a single frame or B-scan. Plus, the peripapillary 2D RNFL thickness circle scan and the BMO-MRW radial scan are both largely focused on imaging a singular anatomic tissue, that is, the RNFL and the neuroretinal rim, respectively. In contrast, a single 3D ONH volume scan can generate many parameters, such as cup volume, MDB thickness and area, rim volume, rim area, rim thickness, peripapillary retinal thickness22 and volume, and peripapillary RNFL thickness and volume. Therefore, the results of this study are in agreement with past evidence that suggest that 3D SD-OCT derived parameters and 3D volume scans are superior to 2D parameters and are not subject to the same limitations of RNFL thickness measurements.

In comparing 3D neuroretinal rim parameters derived from volume raster scans (MDB thickness, rim volume) with those derived from radial scans (BMO-MRW), our study did not show any significant differences in diagnostic capability among 3D raster scan parameters and 3D radial scan parameters (i.e. false discovery rate p values > 0.05). Although there are no large studies which specifically compare BMO-MRW radial versus MDB raster scan protocols for rim parameters, the inherent differences in actual area scanned may temper the study design and conclusions of any such a study. The BMO-MRW radial scan is performed through radial cuts that are corrected according to the Fovea-BMO center (FoBMO) axis. The diagnostic utility of this feature has yet to be established and are currently inconclusive. A recent study by Mwanza et al44 has shown that adjustments made according to the fovea-disc angle have no consistent effect on diagnostic performance.26,45 However, it has been demonstrated by He et. al. that the rotation of the radial scans along the FoBMO axis results in a significantly shifted alignment between BMO-MRW scans and those not utilizing the FoBMO axis correction, thereby resulting in pairwise comparisons between non-identical quadrants and sectors.46 Future larger studies are needed to better define the differences between the MDB thickness parameter with associated 3D raster volume scan and the BMO-MRW parameter with associated radial scan protocol.

In terms of the image acquisition time and the resulting number of parameters procured, the 3D raster volume scan may have several advantages over the BMO-MRW radial scan protocol. For example, there are extra manual steps involved in the BMO-MRW radial scan protocol that may have contributed to its slightly improved, although not statistically better, diagnostic capability compared to raster scan parameters (i.e. MDB thickness and rim volume; Table 2). Before the BMO-MRW radial scan is done, one ideally needs to obtain corneal curvature readings from a keratometer and then input that corneal data into the Heidelberg Spectralis imaging device. Then the operator must determine the FoBMO axis. Then for this study, manual correction of the BMO border during the scan process was performed in the clinic for the 24 radial BMO-MRW scans. In contrast, for the MDB raster scan protocol, no individualized keratometry readings or manual correction of the RPE/BM complex was done during the scan process. Therefore, for this study, the BMO-MRW measurements with keratometry readings and with BMO manual corrections took up to 10 minutes per subject and resulted in neuroretinal rim measurements, while the 3D volume raster scan took less than 2 minutes and resulted in cup, neuroretinal rim, RNFL, and peripapillary retinal parameters (i.e. cup volume, MDB thickness and area, rim volume, rim area, rim thickness, peripapillary retinal thickness22 and volume, and peripapillary RNFL thickness and volume). It should be noted that for the MDB and other raster scan derived parameters, poor quality frames in the dataset were manually identified and automatically corrected by interpolation from good data using the in-house algorithm. Given the differing methods of image quality control, further studies are needed comparing the diagnostic ability of the BMO-MRW to the MDB thickness parameter, where correction of segmentation data for both radial and raster scan protocols is standardized and also comparable between studies. For example, in contrast to a study by Pollet-Villard et al.,28 the MDB thickness in our study was calculated without manual measurement of the neuroretinal rim tissue thickness. The raster line scan protocol presented also offers the advantage of having a higher density of information in the periphery near the RPE/BM complex and in the peripapillary region, as opposed to the radial scan protocol which has the lowest density of information in the peripapillary region and the highest density of information in the cup center, where there is usually space and no clinically useful data. As such, although 3D rim parameters have similar diagnostic capability for glaucoma, the 3D raster volume scan in particular may be an important tool to augment the current standard of care in glaucoma OCT imaging.

There were some limitations to our study. Our RNFL AUROC curve values were lower than other comparison studies (Table 2),9,36 and this may have been because our population contained a higher percentage of early glaucoma subjects (51%) compared to other studies. Additionally, another study needs to be done to see if acquiring the BMO-MRW without manual correction of the BMO border in the clinic and without keratometry readings yields similar diagnostic capability as the MDB scan protocol which does not need either manual adjustment of the RPE/BM complex in the clinic and which does not need keratometry readings. The small sample size of our study also necessitates larger studies evaluating these new 3D glaucoma OCT parameters, but the current study does generate new hypotheses for these future studies.

In conclusion, this study corroborates existing literature that 3D neuroretinal rim parameters which utilize anatomical landmarks derived from SD-OCT imaging are useful in enhancing the current standard of care in glaucoma diagnostics. MDB thickness, rim volume, and BMO-MRW are three such parameters that demonstrate superiority to 2D RNFL circle scans, but show similar diagnostic capability when compared to each other. Future studies are required to expand upon our current knowledge of 3D parameters, their individual advantages, and how best to utilize them alongside other clinical markers for glaucoma.

Acknowledgments

Funding/Support: Teresa C. Chen has received funding from the National Institutes of Health UL1 RR 025758, Massachusetts Lions Eye Research Fund, Fidelity Charitable Fund (Harvard University), and the American Glaucoma Society Mid-Career Award (San Francisco, California).

Footnotes

Financial Disclosures: Johannes de Boer, Center for Biomedical Optical Coherence Tomography Research and Translation Scientific Advisory Board Chair (Harvard Medical School), licenses to NIDEK, Inc. (Fremont, California), Terumo Corporation (Tokyo, Japan), Ninepoint Medical (Cambridge, Massachusetts).

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