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1From the Schepens Eye Research Institute and Harvard Medical School, Boston, Massachusetts; the 2Department of Ophthalmology, Ribeirão Preto Medical School, University of São Paulo, São Paulo, Brazil; the 3Ophthalmic Consultants of Boston, Boston, Massachusetts; and the 4Department of Ophthalmology, University Hospital, Rheinisch-Westfälisch Technische Hochschule, Aachen, Germany.
| Abstract |
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METHODS. A computational approach was implemented with a readily available polarimeter used in glaucoma diagnosis, a nerve fiber analyzer (GDx; Laser Diagnostic Technologies, San Diego, CA). Using near-infrared illumination at each of 20 input polarizations, a series of image pairs was digitized. One image is made from the light returning from the eye that is polarized parallel to the input light, and the other image is made from the light that is rotated by 90° from the input polarization. Using raw data from these 40 images, and a simplified model of ocular polarization properties, images were computed based on their polarization content. Regions of hyperpigmentation, selected using stereo color fundus photographs, were quantified in three types of polarimetry images: (1) a depolarized light image resulting mainly from multiply scattered light; (2) an average image that is typical of confocal images; and (3) a birefringence image. Measurements on versus off hyperpigmentation were made in nine persons with suspected glaucoma or patients with primary open-angle glaucoma, selected to have clinically visible hyperpigmentation.
RESULTS. In the depolarized light images, hyperpigmented regions were significantly brighter than comparison areas (P < 0.0425)that is, had more scattered light and therefore more contrast (P < 0.037) than did color or other polarimetric images.
CONCLUSIONS. With this polarimetry imaging method, subretinal tissues such as those with hyperpigmentation can be visualized with increased contrast.
The present study was performed to investigate further the peripapillary abnormalities in patients with glaucoma by using a new imaging method based on polarimetry, described previously.9 10 Hyperpigmentation has been identified in many eyes preceding the development of geographic atrophy in the macular region, and these areas of hyperpigmentation indicate areas of diseased retinal pigment epithelium (RPE) at extreme risk.11 In both the macular and peripapillary regions, these pigmentary changes correspond histologically to degenerating RPE cells of nonuniform size and melanin content. These changes simultaneously occur with changes to photoreceptors, Bruchs membrane, and the choriocapillaris.11 12 Older adult eyes typically show some peripapillary pigmentary changes.13 Pigmentary changes are not routinely studied as a predictive factor for the progression of glaucoma, but their presence indicates degeneration of the RPE-Bruchs membrane complex surrounding the optic nerve head. The lack of a sensitive method that is immune to the normal variation of fundus pigmentation is needed before peripapillary changes can be fully tested as a reliable predictive factor across individuals and disease stages.
Pigmentary changes can be seen in indirect ophthalmoscopy and color fundus photographs. We investigated whether our polarimetric imaging method would reveal tissue disorder in the peripapillary region, to a greater extent than do standard methods. In advanced glaucoma, deeper structures such as hyperpigmentation may be visualized not only because they appear with more severe damage but also because they show through the thinned nerve fiber layer. For early detection, and for progression, a method is needed that reduces the contribution of the nerve fiber layer so that the deeper structures are revealed.
We have shown that polarization analysis offers the opportunity to emphasize different layers or features of the fundus selectively in retinal images.9 10 Information about the nerve fiber layer and superficial structures such as blood vessel walls are obtained in images by using light that is polarization preserving. The deeper structures can be emphasized by removing this polarization preserving light. Then, the remaining light, which has passed through the retina and been multiply scattered, forms a useful and novel image.14 15 16 17 However, most previous multiply scattered light imaging studies have relied on techniques with annular or displaced apertures. Multiply scattered light images show enhanced contrast of drusen, which are in the layers beneath the retina,9 10 14 15 16 17 and we now extend the polarimetry method to another subretinal feature: hyperpigmentation.
Our hypothesis is that changes in polarization properties of the peripapillary region may help to classify disease state and track progression, by being more resistant to contrast variation arising from various amounts of nerve fiber layer loss. Specifically, although focal hyperpigmentation often appears dark due to increased absorption of concentrated melanin and debris, we anticipate that the focal disruption of the tissues leads to increased scattered light and to increased brightness of these tissues in scattered light images when compared to surrounding tissue. However, when the disease is not focal and is embedded in a larger region of diverse disease, the index of refraction changes may require a much more detailed model. Thus, to test our hypothesis, we confined our sample to focal hyperpigmentation in patients without widespread atrophy.
| Subjects and Methods |
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Scanning laser polarimetry was performed in all patients (GDx; Laser Diagnostic Technologies, San Diego, CA). This device was originally developed to measure the thickness of the nerve fiber layer by birefringence.18 The instrument is designed to be used with pupils of only 2.5 mm in diameterthat is, having an entrance and exit pupil of 2.5 mm. As only 2 mW of near-infrared light (780 nm) is present at the cornea, the light level is comfortable. When lens changes are present, this wavelength more readily penetrates to visualize the retinal and subretinal structures than does short-wavelength light. Figure 1 shows a schematic of the system. Linearly polarized light is rotated by a half-wave plate to 20 different input polarization angles. For each of these angles, the retina is scanned in a raster pattern of 15° x 15° visual angle. The returning light is passed back through all the same optical elements as the illumination pathway, until reaching a polarizing beam splitter. There, the light is split into two beams, one of the same polarization as the illumination light (parallel polarized light, i.e., the detector for uncrossed polarization) and the other that collects light polarized at 90° to the illumination light (the detector for crossed polarization). Each beam passes through a small confocal aperture and is focused on an avalanche photodiode detector. In <1 second, 20 pairs of images are digitized from the amplitude signals of the detectors, with one image per detector and each pair representing illumination with a different angle of polarization for the illumination light. Each image of a series is saved as 256 x 256 pixels with 8 bits of gray scale. The polarization properties of the entire human eye, and not just the retinal and subretinal tissues, must be considered in the interpretation of these images, as noted in Figure 1 and the Discussion section.
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Raw data were processed from the GDx image series to generate images based on the polarization content of the returning light, and some of these do not exist as instrument output and are available only as computed images. We developed a set of computer routines (MatLab; The MathWorks, Natick, MA) to generate these images from the raw images.9 10 As for other analysis with this type of imaging, the best computations are obtained from properly focused image series with a centrally located optic disc, minimal eye movement artifact, and equal illumination in all quadrants. In our analysis, we assume that the changes in the measurable polarization properties are either due to the birefringence of the cornea and retinal nerve fiber layer or to multiple scattering in the retina and RPE. The cornea and to a lesser extent the lens are birefringent elements unrelated to the comparisons of interest in the current studies. Their effects were minimized by a fixed corneal compensator. The isolation per se of the depolarized light component can be decreased with incorrect compensation of corneal polarization. The influence of uncompensated birefringence is not critical for our purposes. This potential artifact causes an underestimation of the improvement in this type of imaging, and the expected decrease in improvement is small.10
All images were aligned to correct for eye movements. Next, we computed the following three image types (Fig. 2A 2B 2C 2D) : (1) a depolarized light image, computed as the minimum value of light returning to the detector for crossed polarization at each pixel for all input polarization angles; (2) an average image of all the light returning to both detectors for all the input polarization angles; and (3) a birefringence image, which represents the modulation of amplitude of light returning to the detector for crossed polarization. The average image is similar to near-infrared scanning laser images collected with small, confocal apertures.19 20
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On examination of the fundus photographs, peripapillary hyperpigmentation appeared dark, as expected, but it appeared bright in the computed depolarized light image, as hypothesized, due to increased scattering. This finding was taken into account for the following analysis. A 3 x 3-pixel region was selected in a region of interest containing the hyperpigmentation in each computed polarimetry image, and average gray-scale values were calculated on computer (MatLab; The MathWorks; Fig. 2F ). The same calculation was made for a control region (3 x 3 pixels) located approximately 200 µm away from the hyperpigmentation.
The color fundus photographs were manually aligned to the computed polarimetry images to have the same magnification as the computed images (Photoshop; Adobe) and were split into the three different color channels: red, green, and blue. The areas corresponding to those in the computed images were marked on the three different color images, and average intensities were calculated by using histograms in the image-management program. The sizes of the regions of interests for the color photographs and polarimetry images were the same, regardless of the number of pixels and the differing resolutions.
From the averaged gray-scale values for each polarimetry image and the three channels for the color fundus photographs, we calculated the difference for on versus off hyperpigmentation by using the Michelson contrast. The Michelson contrast is a metric that helps to decrease the influence of variations in illumination or fundus pigmentation. Michelson contrast is defined as MC = (Ifeature Iadjacent)/(Ifeature + Iadjacent), where Ifeature is the average gray-scale value of the hyperpigmentation region of interest and Iadjacent of the region of interest approximately 200 µm away.
Statistical analysis included paired t-tests for the mean gray-scale and the resultant Michelson contrast, comparing on versus off hyperpigmentation in each channel of the color photographs, as well as in each of the three computed polarimetry images (StatView; Abacus Concepts, Berkeley, CA). We additionally compared the Michelson contrast for on versus off hyperpigmentation for the depolarized light images and the blue channel images.
| Results |
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The average mean differences of the gray-scales for on versus off hyperpigmentation for the three computed images were 6.71 ± 8.36, 5.55 ± 8.68, and 1.73 ± 19.41 for the depolarized light image, the average image, and the birefringence image, respectively. The areas of hyperpigmentation appeared focal and corresponded to the locations seen in the color fundus photographs, indicating that there was good separation of multiply scattered light from retinal layers compared with long-range scatter from anterior segment artifact.
The gray-scale values for on versus off hyperpigmentation were significantly different only in the depolarized images (P = 0.0425) and not in the average images (P = 0.807) or the birefringence images (P = 0.108; Fig. 4 ). Similarly, Michelson contrasts were significantly different for the comparison of on versus off hyperpigmentation in depolarized images (P = 0.037), but lacked statistical significance for the other computed images (P = 0.189 for the birefringence image; P = 0.865 for the average image).
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| Discussion |
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The goal of this imaging method is to visualize small, pathologic features at high contrast, rather than to provide information about layers of tissues, such as numerical estimates of thickness.18 Scattered light, whether due to atrophy or hyperpigmentation, is visualized as bright by our depolarized images. This could be an advantage in that a region with several bright areas may be more recognizable as abnormal than would a few discrete, focal areas of hyperpigmentation. In grading studies and clinical examination of AMD, hyperpigmentation and hypopigmentation are often combined into the single category of "pigmentary changes."25 However, the appearance of specific pathologic features may differ between the polarimetry method used in this study and previously used methods, involving annular confocal apertures and also longer or shorter wavelengths11 15 or lateral displacement of the aperture with respect to the illumination.17 Further, most previous images were collected with larger-diameter apertures, allowing more and longer range scattered light and less sectioning of layers, consequently losing spatial resolution while delineating the large scattering structures. Additional clinical experience with polarimetry may be necessary before its utility for macular disease can be assessed.
The depolarized light images visualized regions of hyperpigmentation with higher contrast than any of the three channels of the color fundus photographs. Sometimes the control regions of interest were not brighter than the focal regions of hyperpigmentation, because of typical variations in fundus pigmentation across the retina, and this experimental difficulty occurred more frequently for the color fundus photographs than for the depolarized light images. Although the color fundus photographs were collected at higher spatial resolution and increased sampling can often improve signal-to-noise ratio, this increased sample size per pixel and consequently larger data file size had fewer, not more, statistically significant results. Models of combining color information across differently pigmented fundi do not yet exist for hyperpigmentation, and therefore the combination of three channels was not tested. However, there is an inherent difficulty with the fundus photography method, in that the nerve fiber layer can obscure peripapillary hyperpigmentation in normal subjects, whereas thinning of the nerve fiber layer allows the peripapillary hyperpigmentation to be revealed. Thus, the relation between the nerve fiber layer and RPE and photoreceptor loss was concluded to be unclear with this method.12
The pattern of hyperpigmentation that could be quantified in the color fundus images of our patients indicates two things. First, after removal of the patient with the more advanced peripapillary atrophy and hyperpigmentation, we had a patient sample with small, often multiple, regions of hyperpigmentation. We did not need a large sample size to obtain significant differences between depolarized light images and all three color separation images. With large lesions of the type we omitted, the pathologic tissues are typically even more visible. Second, our technique works on small regions of hyperpigmentation that were specifically sought by an experienced clinician, but that might in some cases be missed. Thus, the polarimetry technique provides more contrast and can be used on small regions. We tested only patients who still had sufficiently clear media that hyperpigmentation could be detected on clinical examination and with color fundus photographs. Confocal, near infrared imaging has already been shown to have the advantages of penetrating through cataract, providing a useful image in darkly pigmented fundi, and reducing long-range scatter from a variety of ocular media changes.14 This type of instrument does not require the pupil dilatation that is necessary for the high-quality fundus photographs, and the light levels are safe and comfortable.
The polarimetry imaging method seems suited for early detection of hyperpigmentation, either in new patients or as a potential means to determine progression of peripapillary damage. Chorioretinal abnormalities, such as atrophy or hyperpigmentation, have been reported to occur in some but not all eyes with glaucomatous optic nerve damage. Ophthalmoscopically, these changes have been divided into a central beta zone and a more peripheral alpha zone. The beta zone shows visible sclera, due to a complete loss of the RPE cells and a decreased number of photoreceptors, whereas the alpha zone is characterized by uneven hypo- and hyperpigmentation that histologically correspond to pigmentary irregularities in the RPE.13 26 27 28
Pigmentary changes, such as hyperpigmentation, result from severe damage to the RPE layer, and therefore may be an important sign of disease related damage to deeper layers of the retina.11 12 16 This may occur, not only in glaucoma but also in other diseases that affect the RPE, particularly when the RPE is one of the primary sites, such as in AMD. For AMD, focal hyperpigmentation is a well-known risk factor for disease progression.11 29 30 31 It is not known whether these changes are a very early sign of damage or merely quite visible, particularly once the retina is thinned.
Our novel polarimetry method has been shown to lead to enhanced contrast of subretinal features such as drusen.10 We have shown that it will also provide information for the hyperpigmented regions around the optic nerve head. Polarimetry methods have evolved32 so that they now distinguish the polarization retaining light from the depolarized light.9 10 33 We intentionally compute images that visualize features in scattered light, primarily originating from deeper structures in the fundus. This is one key difference between our method and the wide variety of new polarimetry methods that are optimized for high contrast34 or light with scatter minimized to the extent that a coherence method can be used35 that is, polarization retaining light.
The present results support our previous findings that different features are emphasized according to the proportion of polarization retaining light in the image, with superficial features better visualized with a high proportion of polarization containing light and deeper features visualized better for images that diminish the proportion of polarization retaining light.9 10 33 For glaucoma management, several important features were rapidly visualized in a few key computed images, without the need for dilatation or uncomfortably bright light. These features include the optic nerve head rim and cup, pores in the lamina cribrosa, a nerve bundle defect, peripapillary hyperpigmentation, peripapillary atrophy, retinal arteries and veins, the arterioles and veins associated with the optic nerve head, and the distribution of birefringence associated with the measurement of retinal nerve fiber layer thickness. In addition to visualizing features, the depolarized light images have been used to obtain better information from beneath and within blood vessels, because the specular reflection from blood vessel surfaces is greatly minimized.9 22 36 Other polarimetry techniques used for macular imaging have been used to improve the measurements of structures, such as the computation of retinal nerve fiber layer thickness that is based on the absolute retardance.37 38 39
Further improvement of polarimetry methods is being advanced by the use of Mueller matrix instrumentation, which completely specifies the polarization content in an image,34 40 41 42 and by experiments to identify factors such as individual variations in anterior segment optics.37 38 43 Both the specular and scattered light return, which were shown in panels B versus C in Figures 2 and 3 to provide different information for the optic nerve head structures, have been quantified with Mueller matrix polarimetry (Guthrie et al. IOVS 2004;45:ARVO Abstract 2796). Although the uses of polarimetry information are different, the mathematical treatments are closely related and well-described.9 10 37 41 42
Our sample included patients old enough to have aging changes to the cornea, lens, or vitreous that might alter the polarization results. None of the patients had severe enough changes to prevent color fundus photography, indicating that our sample did not include the most severe media changes. Two known artifacts of the cornea include an irregular tear film, which results in variation of optical power over the surface and over time, and individual differences in birefringence of the cornea.37 38 When the corneal compensator does not correct for corneal birefringence, then our method overestimates somewhat the amount of depolarized light. This effect is generally constant across the retina. For example, 85% to 90% of the light returning from the normal retina retains polarization.32 Therefore, if we remove only 70% of this component due to incomplete compensation of corneal birefringence, then the contrast of the depolarized light is two times higher. The addition of uniform depolarized light reduces image contrast to some extent. As for aging changes due to the lens, the polarization effects of the normal lens and most intraocular lenses are barely measurable with present instrumentation.43 The effect of a cataractous lens has not been measured in detail with this instrumentation, except for the comparison of before versus after cataract extraction.44 Such studies include not only the potential scattering of the cataractous lenses but also the alteration of corneal polarization due to wound healing after surgery. Differences on long-term follow-up were, on average, in the direction of improved signal amplitude with cataract extraction, but not generally statistically significant with either scanning laser polarimetry or confocal imaging. These findings are consistent with the idea that depolarization due to neither the cornea nor the lens has a large effect on the light return from the retinal plane, and consequently the computed depolarized image, due to the use of a confocal aperture to remove long-range scatter.
In a more general model, interesting polarization retaining information and possible artifacts could arise from sources not limited to the corneathat is, when considering light return that is not limited to only birefringence or only the cornea and nerve fiber layer. The present method differs from the use of a static, cross-polarizer to remove glints that may occur in a given plane of polarization. Further, light collected at the detector for crossed polarization, regardless of the source, has no effect on the depolarized light image, as long as it is modulated in phase with the polarization preserving light that here is attributed to the nerve fiber layer, varying systematically according to the input polarization angle. Unlike the case of a single cross-polarized element, this modulating light is removed by the computation. Alternatively, any light reaching the detector for crossed polarization that does not modulate in phase with the light attributed to the nerve fiber layer serves to reduce the computed modulation and therefore reduces the contrast of the depolarized light images. The artifact is only in one directiondecreasing contrastand does not add spurious features that are not present. The method described here clearly visualized the features of interest, some not otherwise visible, in a clinical population. Thus, further removal of artifacts, which although potentially small are inherent in an incomplete polarimetry device, would serve to make this method even better. Besides further reducing these already identified artifacts, the potential benefits of fully specifying polarization for pathologic structures is unknown in the eye. Image contrast in computed images as yet unavailable may be high for optically active molecules, and new information may be provided.
We tested only patients with clinically visible peripapillary hyperpigmentation, but we anticipate that this method may reveal similar findings in other patients with either more overlying nerve fiber layer, ocular pigmentation, or retinal disease such as epiretinal membrane that precludes visualization of hyperpigmentation. For patients undergoing scanning laser polarimetry in the management of glaucoma,18 19 37 38 39 there is almost no additional time needed during patient data acquisition. As we did not experience difficulties in distinguishing fundus features, despite large atrophic regions prone to scatter, this method may be extended to peripapillary atrophy, known to be concordant with visual field loss.45 This method may not only be more sensitive than traditional methods, but it also uses far less data storage. Thus, it should be considered for further studies for early detection of peripapillary changes improving the estimation of prognosis by factoring in peripapillary hyperpigmentation.
| Acknowledgements |
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| Footnotes |
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Presented in part at the annual meeting of the Association for Research in Vision and Ophthalmology, Fort Lauderdale, Florida, May 2002.
Supported by National Eye Institute Grant EY07624 and the Richard Saltonstall Foundation (AEE).
This technology is specifically not funded by the Small Business Innovative Research grant with Laser Diagnostic Technologies. They choose not to license it at this time. The authors are permitted but not obligated to seek other licensees.
Submitted for publication May 21, 2004; revised October 18, 2004; accepted November 22, 2004.
Disclosure: M.B. Mellem-Kairala, None; A.E. Elsner (P); A. Weber, None; R.B. Simmons, None; S.A. Burns (P)
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.
Corresponding author: Ann E. Elsner, Schepens Eye Research Institute, Harvard Medical School, 20 Staniford Street, Boston, MA 02114; elsner{at}vision.eri.harvard.edu.
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