Abstract
purpose. To study the effect of small-incision cataract surgery on the optical aberrations of the cornea.
methods. Corneal topography was measured before and after cataract surgery on 70 eyes of 70 patients. Monofocal foldable IOLs were implanted after phacoemulsification through a clear-cornea, 3.5-mm incision without suture. Corneal aberrations, up to the fifth order and 6-mm pupil, were calculated by ray-tracing from the corneal topography. Pre- and postoperative aberrations were compared in each patient and the optical changes induced by surgery investigated.
results. The root mean square of the wave aberration slightly increased on average after surgery (pre, 0.65 ± 0.46 μm; post, 0.85 ± 0.63 μm). Most aberration terms were similar, averaged across the 70 patients, before and after surgery (spherical aberration: pre, 0.32 ± 0.12 μm, and post, 0.34 ± 0.19 μm; astigmatism: pre, 0.9 ± 0.8 D, and post, 1.1 ± 1.0 D; coma: pre, 0.27 ± 0.18 μm, and post, 0.32 ± 0.33 μm). However, in each patient, there were changes after surgery in the magnitude (either increasing or decreasing) and/or orientation of aberrations. The mean induced astigmatism was −1.0 ± 0.9 D at the orientation of the surgical meridian. Induced trefoil also showed a predominant pattern at this direction. Patients with nasal incisions experienced larger changes.
conclusions. Small-incision surgery does not systematically degrade the optical quality of the anterior corneal surface. However, it introduces changes in some aberrations, especially in nonrotationally symmetric terms such as astigmatism, coma, and trefoil. The incision site plays a main role in the corneal changes after surgery.
Today, the implantation of intraocular lenses (IOLs) is a successful procedure for cataracts and aphakia. However, due to the advancements in the field of ophthalmic wavefront sensing during the past few years, new questions and challenges have arisen that require additional study. The quality of the retinal image is mostly limited by the aberrations of the eye. The eye is a complex structure, and each of its components contributes differently to final optical performance. Thus, the study of individual contributions to ocular aberrations has become of great importance for both basic science and clinical applications. The aberrations of the complete eye can be measured currently by using different types of wavefront sensors, or aberrometers.
1 2 3 4 The aberrations introduced by the anterior corneal surface can be computed from data obtained by corneal topography.
5 In addition, the combined use of both corneal and ocular aberrations allows the estimation of the aberrations of the crystalline lens.
6 7 8 In particular, the possibility of measuring the aberrations of the cornea becomes relevant in cataract surgery. Degraded optical quality of the cornea after surgery would limit the performance of the eye with an implanted IOL. Thus, a major concern is to know the possible changes in the corneal optics induced by surgery. It has been shown that an increase in astigmatism may be common after cataract surgery.
9 10 11 12 13 In addition, we have found that the optical performance of the cornea is similar or slightly worse in patients with implanted IOLs,
14 with a small percentage of patients presenting corneal aberrations larger than the average in normal eyes. These conclusions were based on the comparison of corneal aberrations in a group of patients with IOLs after extracapsular cataract extraction in comparison with a group of normal subjects of similar age. A direct comparison in each patient of the corneal aberrations before and after phacoemulsification surgery has not been undertaken.
A related issue in cataract surgery has been the study of how the optics of IOLs combines with the eye’s aberrations to produce the final retinal image. It has been shown that typical IOLs, which are manufactured to meet high optical quality standards,
15 16 17 18 produce a relatively low retinal image quality.
19 We suggested that the reason could be that conventional IOLs are inadequate for compensating for the aberrations of the cornea.
14 That work inspired a new design of IOLs that compensates for the spherical aberration of the cornea and leads to a partial compensation, similar to the balance that occurs in young subjects between the cornea and the natural lens.
7 8 For these new IOLs to be effective in improving retinal image quality, the optics of the cornea must remain relatively unchanged after surgery.
In this context, the purposes of this work were to study the aberrations of the anterior surface of the cornea in a large population of patients, before and after small-incision cataract surgery, and to investigate the changes in corneal optics induced by the surgery. This information may provide better understanding of the optical performance of eyes implanted with IOLs and can be valuable to look for improvements in the incision procedures in case the surgery produced significant changes in the cornea.
Seventy eyes of 70 different patients with cataract were investigated. Ages ranged from 32 to 89 years (mean age, 70 ± 12 years). All clinical examinations and surgery were conducted at the Anterior Segment Division of Ramón y Cajal Hospital (Madrid, Spain). Surgeries were completed between 1999 and 2002 in all patients by the same surgeon (JT). Practices and research adhered to the tenets of the Declaration of Helsinki. Informed consent was obtained from the subjects after explanation of the nature and possible consequences of the procedures.
Clinical examination data recorded included corrected and uncorrected visual acuity, refraction, manual keratometry, intraocular pressure, and biomicroscopic anterior and posterior segment evaluation. All these tests were performed within 5 days before surgery and at 2 weeks, and between 4 and 6 months after surgery. The preoperative evaluation included biometry and IOL calculation. Videokeratoscopy (Eyemap EH-290; Alcon, Fort Worth, TX) was performed only at the preoperative and 4- to 6-month postoperative follow-up visit. Mean axial length was 23.6 ± 2.1 mm. Mean power of the implanted IOLs was 20 ± 5 D. Mean best corrected decimal visual acuity after surgery was 0.8 ± 0.3. Postsurgical spherical errors ranged from −2.5 to 4.5 D (mean, 0.5 ± 1 D).
Surgery was performed with eyes under topical anesthesia or retrobulbar block. A three-step corneo-corneal incision (2.8 mm blade) was used in all cases. After introduction of viscoelastic material into the anterior chamber, a 5-mm capsulorrhexis was made, followed by hydrodissection, the stop-and-chop phacoemulsification technique, aspiration of cortical masses, and introduction of Acrysof MA60BM (Alcon) or CeeOn edge 911A (Pharmacia & Upjohn Co., Pickerington, OH) foldable IOLs. The corneal incision was enlarged to 3.5 mm to implant the IOL and was not sutured.
The position of the incision was chosen according to a surgical plan for a right-handed surgeon. The criteria for the studied corneas were:
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Meridian with the largest curvature at 90 ± 20°: (1) superior incision if ocular astigmatism is 1.5 D or higher or (2) temporal incision for both right and left eyes if ocular astigmatism is lower than 1.5 D.
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Meridian with the largest curvature at 180 ± 20°: temporal incision for right eyes and nasal incision for left eyes.
There was no case of oblique astigmatism in the population studied.
Figure 1 shows a histogram with the percentage of patients who had the incision site at each angle. Most patients had the incision at 180°.
Corneal topography was measured (EH-290 EyeMap; Alcon). This is a 23-ring Placido-based system that makes a radial sampling of 0.2 mm and a meridional sampling of 10°. The inner ring has a radius of 0.2 mm. This sample density is sufficient for the study of aberrations up to the fifth order for a 6-mm diameter pupil. Sagittal elevations, measured with respect to a reference plane tangential to the corneal vertex, were exported from the topographer as a tabular ASCII file and preprocessed to be used later to calculate aberrations.
The accuracy of the system has been studied by using calibrated testing surfaces.
20 It has been shown that the system is reliable for radial distances up to 3 mm, which is the pupil radius we used for analyzing the aberrations. We tested the reproducibility by comparing four different topographic measurements in the same eye of a patient.
Figure 2 shows the mean value and the experimental error of each aberration coefficient, calculated by averaging the four aberration maps obtained from the four different topographies. Also shown is the correlation between the aberration coefficients for the different measurements taken in the same eye. The experimental error due to reproducibility is approximately 0.1 μm for astigmatism, coma, and trefoil coefficients. For spherical aberration the error is much lower: approximately 0.02 μm. The error of the root mean square (RMS), accounting for all the aberrations, is also approximately 0.1 μm. These results are similar to those obtained with others systems
5 and indicate that reproducibility was reasonably good.
The protocol for alignment and focusing the eye was as follows:
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The patient fixates a small red light in the center of a mire pattern and the operator aligns the eye.
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The system has autoalignment (centering in the x- and y-axes with respect to the corneal vertex) and autofocus (positioning in the z-axis) mechanisms to enhance manual positioning.
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Alignment is checked by superimposing a semitransparent topography map on the photokeratoscopy image.
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The system displays an isometric map, in which the power of the points in each ring are plotted against their axes, as if the rings had been straightened out. Distortion of these profiles may indicate inaccurate alignment.
If positioning was inadequate after these steps, the measurement was discarded and a new topographic map made. Using this protocol, we found high reproducibility when taking multiple measurements, as mentioned in the previous paragraph, and so a single image was finally recorded for processing.
Topography was performed in each patient at the preoperative and 4- to 6-month postoperative follow-up visits.
We calculated the aberrations produced by the anterior surface of the cornea from the data provided by the corneal topographer.
5 From the elevations at each sampled point, characterized by polar coordinates (
r,θ) in the pupil plane, we calculated the corneal wavefront aberration (WA) as the difference between the optical path lengths of the principal ray passing through the corneal vertex and a marginal ray passing through the point (
r,θ)
\[WA(r,{\theta})\ {=}\ n{^\prime}s{^\prime}\ {-}\ n{^\prime}d{^\prime}\ {-}\ nz,\]
where
n and
n′ are the refractive indices for the air and the cornea,
z is the corneal elevation at the point (
r,θ),
s′ is the distance from the vertex to the image point, and
d′ is the distance from the point (
r,θ) to the image point.
The corneal aberrations were obtained for a pupil 6 mm in diameter. We considered an artificial pupil centered at the corneal vertex. In many cases, the natural pupil is decentered with respect to the vertex. This decentering must be taken into account if, for example, one compares the aberrations of the cornea and those of the complete eye measured by a wavefront sensor that centers with respect to the natural pupil. This consideration was not necessary, however, in the present study. We systematically centered in relation to the vertex, the correct method to use in determining changes in the same eye between two situations.
We obtained the wave aberration up to the fifth order and expressed it as a weighted sum of the first 21 Zernike polynomials, Z
n m \[WA(r,{\theta})\ {=}\ {{\sum}_{\begin{array}{l}n{=}0\\m{=}{-}n,n\end{array}}^{n{=}5}}\ c_{n}^{m}\ {\cdot}\ Z_{n}^{m}(r,{\theta}).\]
Each Zernike coefficient
c n m corresponds to an individual aberration. For example,
c 2 ±2 represents astigmatism;
c 3 ±1, coma;
c 3 ±3, trefoil (also called secondary, or triangular, astigmatism); and
c 4 0, spherical aberration.
The coefficients
c 2 +2 and
c 2 −2 represent the refractive errors along the horizontal meridian and an oblique meridian at 45°, respectively. We calculated the astigmatism in diopters with the equation
5 21 \[astigmatism\ {=}\ {-}\ \frac{1}{r_{0}^{2}}\ 4\sqrt{6}\sqrt{(c_{2}^{{-}2})^{2}\ {+}\ (c_{2}^{{+}2})^{2}},\]
where
r 0 is the pupil radius (3 mm). The axis of the astigmatism (orientation of the meridian with the lowest curvature) in degrees was calculated as
\[axis\ {=}\ \frac{1}{2}\mathrm{arctan}(c_{2}^{{-}2}/c_{2}^{{+}2}).\]
The higher order aberrations were quantified by means of the RMS of the wave aberration
\[\mathrm{RMS}\ {=}\ \sqrt{{{\sum}_{i}}(c_{i})^{2}},\]
with
i excluding astigmatism and defocus.
Pre- and postoperative corneal aberrations were obtained in each patient. We performed regression analyses to seek correlations between pre- and postoperative aberrations. We used the two-sample paired t-test to determine whether the pre- and postoperative values differed from each other in a significant way. Our data are paired because there is a one-to-one correspondence between the values in the two samples. In most cases, the assumptions of the t-test were not met. These assumptions were that differences between samples would be normally distributed (which was examined by the χ2 test) and that the variances of the two samples would be equal. Although the t-test works well with large samples, even if its assumptions are not met, we also used the nonparametric Wilcoxon test. We also investigated the change in the total aberrations separately in two subgroups of patients, depending on the position of the incision: nasal (left eyes, near 180°), or temporal (right eyes, near 180°).
The changes between aberrations before and after surgery were studied by means of “induced aberrations.” We calculated these induced aberrations as the difference between post- and presurgical values for every aberration term
\[{\Delta}c_{n}^{m}\ {=}\ c_{n}^{m}(post)\ {-}\ c_{n}^{m}(pre).\]
In particular, we studied induced spherical aberration, astigmatism, coma, and trefoil. In the case of the nonrotationally symmetric aberrations (astigmatism, coma, and trefoil), we obtained both the magnitude and the orientation of the induced aberration. Thus, the induced astigmatism in polar values was calculated as
\[{-}\ \frac{4\sqrt{6}}{r_{o}^{2}}\sqrt{({\Delta}c_{2}^{{-}2})^{2}\ {+}\ ({\Delta}c_{2}^{{+}2})^{2}}\mathrm{D};\ axis\ {=}\ \frac{1}{2}\mathrm{arctan}({\Delta}c_{2}^{{-}2}/{\Delta}c_{2}^{{+}2})\ \mathrm{degrees}.\]
The induced coma was calculated as
\[\sqrt{({\Delta}c_{3}^{{-}1})^{2}\ {+}\ ({\Delta}c_{3}^{{+}1})^{2}}\ {\mu}\mathrm{m},\ axis\ {=}\ \mathrm{arctan}({\Delta}c_{3}^{{-}1}/{\Delta}c_{3}^{{+}1})\ \mathrm{degrees},\]
and the induced trefoil as
\[\sqrt{({\Delta}c_{3}^{{-}3})^{2}\ {+}\ ({\Delta}c_{3}^{{+}3})^{2}}\ {\mu}\mathrm{m},\ axis\ {=}\ \frac{1}{3}\mathrm{arctan}({\Delta}c_{3}^{{-}3}/{\Delta}c_{3}^{{+}3})\ \mathrm{degrees}.\]