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1 From the Retina Service, Department of Ophthalmology, Indiana University School of Medicine, Indianapolis; and the 2 Department of Psychology, University of Georgia, Athens.
| Abstract |
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METHODS. MPOD was measured using flicker photometry in free view at 458 nm with a 1° stimulus. Twenty-nine eyes from 24 patients with cataracts sufficiently severe to require cataract extraction were evaluated.
RESULTS. In the entire group of 24 patients, the mean (±SD) age measured 68.7 ± 9.5 years, and the mean MPOD measured 0.19 ± 0.11. For all 29 eyes measured, MPOD averaged 0.206 ± 0.13 before and 0.18 ± 0.12 after cataract extraction. MPOD measurements at the two time points (mean 8.1 ± 4.7 weeks after surgery) were highly correlated (r = +0.58), suggesting that a cataractous lens does not influence the MP measurement technique.
CONCLUSIONS. Psychophysical techniques can be used to obtain reliable measurements of MP in elderly subjects, even in those with cataracts. Moreover, differences in retinal illuminance due to varying opaqueness of the crystalline lens do not seem to have a measurable influence on MPOD.
| Introduction |
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Measurements of the retina are therefore affected by light loss due to lens absorption. For example, Maxwellian view optics focus a narrow ray of light through the center of the pupil, and this light passes through the central nucleus of the lens. Stimuli seen in natural view must pass through a wider area of the lens defined by the size of the pupil. Both psychophysical and physical methods must correct for the wide individual differences in this type of preretinal light loss to precisely specify retinal illuminance. Psychophysical methods are further limited, in that corrections are made for light absorption but not for the negative effects of a dense lens on visual performance.
There are generally two methods used to correct for absorption by the crystalline lens. One method involves measuring the optical density (OD) of the lens at specific wavelengths (see Snodderly and Hammond4 ) and then subtracting these values from the overall amount of light used in retinal measurements. Another method used to correct for lens absorption is to compare measures of retinal areas that differ only in the parameter being measured. In this way, light absorption by the lens is the same for both measures, and the only factor that differs is the variable being measured. This is the basic psychophysical method used when measuring macular pigment optical density (MPOD). In essence, retinal sensitivity to visible light is measured in an area where MP is dense (the fovea), and that measure is compared with an area where MP is optically immeasurable (usually at approximately 4°8° in the parafovea). When these two photopic sensitivity curves are equated at long wavelengths, they differ in the short-wave end of the visible spectrum. When these differences are plotted against wavelength, a spectral density curve is generated that has the same basic shape as the extinction spectrum of xanthophylls.5 Because absorption by the lens is equal in both cases, it is assumed that lens absorption does not influence the difference in these two spectral curves. Simulation data from Wooten et al.6 suggest that this is the case.
In the present study, we assessed the influence of lens absorption on MP measurements by comparing MP measured before and after cataract extraction. Although the subjects overall sensitivity to light increased after the extraction, their measured MPOD did not change significantly.
| Methods |
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All patients underwent planned phacoemulsification and placement of a foldable acrylic posterior chamber intraocular lens for cataract of sufficient severity to interfere with their activities of daily living. The median preoperative best corrected Snellen distance visual acuity measured 20/50. Patients were deemed eligible for this study if their near acuity could be refracted to 20/25 or better. In five patients, both eyes were considered cataractous, and MPOD was assessed in both. MP was originally measured before cataract extraction and then a mean (±SD) of 8.1 ± 4.7 weeks (range, 317; median 6 weeks) after completion of the surgery. During MPOD measurement, visual acuity was corrected to 20/25 near acuity. All subjects were naïve about the purpose of the study and were not experienced in psychophysical tasks. Informed consent was obtained, and the tenets of the Declaration of Helsinki were followed.
Measurement of MPOD
Schematics and an expanded discussion of the device and stimuli
used in the present study can be found in Wooten et al.6
For details regarding the procedure used, see Snodderly and
Hammond.4
A circular test stimulus was presented near the center of a 6°, 10.5-candelas (cd)/mm2, 470-nm circular background. The size of the test stimulus was 1°. The wavelength composition of the test stimulus alternated between a 458-nm measuring field (peak MP absorbance) and a 570-nm, 16.7-cd/mm2 reference field (minimal MP absorbance). The measuring and reference fields were superposed and presented out of phase in a square wave alternation rate of 11 to 12 Hz in the foveal condition and 6 to 7 Hz in the parafoveal condition.
The apparatus used for the MP measurement delivered the stimulus in natural view but used a stimulus that was similar to configurations used in past studies in which the stimulus was presented in Maxwellian view.7 8 9 10 11 Recent data6 on 32 subjects (age range, 1872 years) have shown that MPOD measured in natural view, with a slightly different stimulus configuration (e.g., this study used a 4° rather than a 6° parafoveal reference), provides the same values as MPOD measured in Maxwellian view.
Light for the 6° background was produced by three LEDs (packed tightly in a triangular array) with peak energy at 470 nm and half-widths of approximately 20 nm. Light for the 570-nm reference field was produced by an LED with peak energy at 570 nm (half-width, 20 nm). Light for the 458-nm measuring field was produced by two LEDs with peak energy at 458 nm (half-width, 20 nm). Light from the LED sources was collimated with planoconvex lenses and was then passed through polycarbonate diffusers (high-efficiency, holographic type; Physical Optics, Torrence CA), which served essentially as back-projection screens.
The sizes of the background and test stimulus were defined by circular apertures (constructed by computer-generated images exposed on high-density, photographic mylar film) placed after the collimating lenses. The background and test stimuli were then combined and reflected to the subject by a 2-in. beam splitter with the front surface located 16 in. from the subjects eye. The entire optical system was contained in a rectangular, black plexiglas box. One side of the box contained a 1-in. hole centered on the subjects optical axis through which the stimulus could be viewed. Subjects requiring refractive correction were allowed to wear the appropriate corrective lenses for the viewing distances used, provided these lenses were not tinted. Head alignment was accomplished by the use of an adjustable head and chin rest assembly and, when properly aligned, the subject viewed the hole in the box as slightly larger than and concentric with the background field.
Stimuli were calibrated using a photocell (PIN-10; UDT Sensors, Hawthorne, CA). The LEDS were driven by a constant-current power supply. Radiance variation was achieved by varying the frequency of a 1.5-µsec pulse over a range of 300 to 300,000 Hz. Calibration of the high-frequency pulse rate showed that the frequency delivery was proportional to the radiance output. Thus, MPODs could be derived by simply calculating the log ratio of the frequencies of the 458-nm measuring field at the foveal and parafoveal eccentricities, respectively.
Flicker photometry was used. Subjects adjusted the radiance of the 458-nm measuring field to achieve minimal flicker with the 570-nm reference. This measurement was performed in the fovea (where MP is the most dense) and at 4° in the parafovea (where light absorption by MP is negligible). A tiny (5-minute) opaque fixation point was located on the left edge of the background, and subjects fixated on this point when making the parafoveal measurement. The peak optical density of MP was derived by subtracting the log foveal sensitivity from the log parafoveal sensitivity at 458 nm. Five foveal and five parafoveal measurements were made after brief instructions and a few practice settings. The means ± SD of these numbers are provided in Table 1 .
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| Results |
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As shown in Figure 1 , the results of this study also suggest that the method used for measuring MPOD is reliable in older experimentally naïve subjects. The two values measured before and after cataract and at disparate time points yielded similar MPODs (r = +0.58). The absolute value of the average change between the first and second session was 0.085 ± 0.08. Nonetheless, as also shown in Figure 1 (open squares), there were two subjects whose data did not replicate well. When these two subjects (MH and NC) were removed, the correlation was improved (r = +0.74).
Table 1 lists the SDs of the five foveal and parafoveal measures used to derive MPOD. Although the changes in the variance of the parafoveal measures before and after cataract were minimal, the variance in the postoperative foveal values decreased by approximately 45%. These findings suggest that a dense lens can influence a subjects performance, particularly when making the foveal settings. It is unclear, however, whether increased variability in performance actually leads to less replicable data. There were instances (e.g., subject NC) when high within-session variability predicted poor replicability in the derived MPODs. As shown in Table 1 , however, for most subjects, variability within a session was not related to differences in the derived MPODs across sessions.
| Discussion |
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The similarity in the MP measurements before and after cataract has implications for both basic and applied research. From a basic-methods perspective, techniques analogous to the flicker photometry method used in the present study can assume minimal confounding due to absorption by the lens. Thus, comparative measures of two retinal loci are valid as long as the receptor populations between the two loci are equivalent or the differences are experimentally controlled. From an applied perspective, these results further motivate the need to measure lutein and zeaxanthin within the retina in elderly subjects who are most susceptible to age-related retinal and lenticular disease. Numerous epidemiologic studies have linked low dietary intake and blood levels of lutein and zeaxanthin to age-related cataract16 17 and macular degeneration.18 19 20 These studies, however, tend to be inconsistent.21 22 23 One explanation for the inconsistencies is that dietary intake and blood carotenoid levels may actually be poor predictors of the amount of lutein and zeaxanthin available to the eye, particularly in females.8 The ability to measure lutein and zeaxanthin directly provides a better assessment of the availability of these carotenoids to ocular tissue.
Recent years have seen a proliferation of lutein supplements being touted for their ability to protect the retina and lens from oxidative damage. It is probable that not all subjects will respond to these types of supplements equally. The ability to measure MPOD in vivo and repeatedly in the elderly would be one method of evaluating the efficacy of using these supplements and/or dietary modifications designed to increase MPOD.
| Footnotes |
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Submitted for publication September 19, 2000; revised December 15, 2000; accepted December 20, 2000.
Commercial relationships policy: N.
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: Thomas A. Ciulla, Retina Service, Department of Ophthalmology, 702 Rotary Circle, Indiana University School of Medicine, Indianapolis, IN 46260. tciulla{at}iupui.edu
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