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An evaluation of the Bausch & Lomb Zywave aberrometer

Taylor & Francis
Clinical and Experimental Optometry
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Purpose: The Bausch & Lomb Zywave uses Shack-Hartmann aberrometry to determine wavefront aberrations of the human eye and provide an estimate of refractive error. We investigated the effect of pupil size on the repeatability and validity of refractive errors estimated by the Zywave and the repeatability of higher-order aberrations. Methods: Twenty-three subjects were measured with the Zywave under natural and cycloplegic conditions on two occasions separated by at least one week. Refractive error was also measured using a Nidek ARK-700A autorefractor. At one visit, a cycloplegic subjective refraction was performed. Measured ocular wavefront aberrations were expressed as the polynomial coefficients from a least-squares fitted fifth-order Zernike polynomial expansion over three, five and seven millimetre diameters. Repeatability and validity were evaluated by calculating the difference between pairs of refractive estimates or Zernike terms, determining the mean and standard deviation of these differences and calculating the 95% limits of agreement (LoA = mean +/-1.96 x SD). Results: The repeatability of refractive error estimated by the Zywave was better than that of the Nidek autorefractor for both manifest and cycloplegic conditions. Manipulating the pupil size on the Zywave from three to seven millimetres changed the mean cycloplegic spherical equivalent from -1.91 D to -2.60 D, a shift that was negatively correlated with spherical aberration. As expected, the magnitude of the Zernike coefficients increased with increasing pupil diameter, as did their corresponding 95% LoA. The 95% LoA decreased for higher-order terms but the magnitude of the terms and the variation between subjects also decreased with increasing order. To compensate for these factors,the ratio of the SD between sessions to the SD across subjects was calculated. The ratios were lowest for second-order terms (less than 0.08 for 7.0 mm pupil), intermediate for the C4,0 spherical aberration term (0.14) and third-order terms (approximately 0.25) but approached and exceeded 1.0 for many fourth- and fifth-order terms. Conclusions: The Zywave provides valid and repeatable estimates of refractive error. We attribute the myopic shift for larger pupils to the eye's spherical aberration. The repeatability of the Zernike terms measured with the Zywave was acceptable for the second-order and spherical aberration terms but for other higher-order terms, the variation between sessions may exceed the variation between subjects indicating unacceptable repeatability. This may have important ramifications for wavefront-guided LASIK.
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ORIGINAL PAPER
An evaluation of the Bausch &
Lomb Zywave aberrometer
Clin Exp Optom 2009; 92: 3: 238–245 DOI:10.1111/j.1444-0938.2009.00360.x
Michael J Dobos*ODMS
Michael D TwaOD PhD
Mark A Bullimore* MCOptom PhD
* The Ohio State University College of
Optometry, Columbus, Ohio, USA
University of Houston, College of
Optometry, Houston, Texas, USA
E-mail: dobos.10@osu.edu
Purpose: The Bausch & Lomb Zywave uses Shack-Hartmann aberrometry to determine
wavefront aberrations of the human eye and provide an estimate of refractive error. We
investigated the effect of pupil size on the repeatability and validity of refractive errors
estimated by the Zywave and the repeatability of higher-order aberrations.
Methods: Twenty-three subjects were measured with the Zywave under natural and
cycloplegic conditions on two occasions separated by at least one week. Refractive error
was also measured using a Nidek ARK-700A autorefractor. At one visit, a cycloplegic
subjective refraction was performed. Measured ocular wavefront aberrations were
expressed as the polynomial coefficients from a least-squares fitted fifth-order Zernike
polynomial expansion over three, five and seven millimetre diameters. Repeatability and
validity were evaluated by calculating the difference between pairs of refractive estimates
or Zernike terms, determining the mean and standard deviation of these differences and
calculating the 95% limits of agreement (LoA =mean 1.96 ¥SD).
Results: The repeatability of refractive error estimated by the Zywave was better than that
of the Nidek autorefractor for both manifest and cycloplegic conditions. Manipulating
the pupil size on the Zywave from three to seven millimetres changed the mean cyclople-
gic spherical equivalent from -1.91 D to -2.60 D, a shift that was negatively correlated with
spherical aberration. As expected, the magnitude of the Zernike coefficients increased
with increasing pupil diameter, as did their corresponding 95% LoA. The 95% LoA
decreased for higher-order terms but the magnitude of the terms and the variation
between subjects also decreased with increasing order. To compensate for these factors,
the ratio of the SD between sessions to the SD across subjects was calculated. The ratios
were lowest for second-order terms (less than 0.08 for 7.0 mm pupil), intermediate for
the C4,0 spherical aberration term (0.14) and third-order terms (~0.25) but approached
and exceeded 1.0 for many fourth- and fifth-order terms.
Conclusions: The Zywave provides valid and repeatable estimates of refractive error. We
attribute the myopic shift for larger pupils to the eye’s spherical aberration. The repeat-
ability of the Zernike terms measured with the Zywave was acceptable for the second-
order and spherical aberration terms but for other higher-order terms, the variation
between sessions may exceed the variation between subjects indicating unacceptable
repeatability. This may have important ramifications for wavefront-guided LASIK.
Submitted: 1 November 2008
Revised: 6 January 2009
Accepted for publication: 23 January
2009
Key words: aberrations, aberrometer, evaluation, wavefront optics, Zernike polynomials
CLINICAL AND EXPERIMENTAL
OPTOMETRY
Clinical and Experimental Optometry 92.3 May 2009 © 2009 The Authors
238 Journal compilation © 2009 Optometrists Association Australia
Liang and colleagues1were the first to
use a Shack-Hartmann aberrometer on
human eyes and mathematically explain
the wavefront maps to the fourth-order
Zernike terms from the local derivatives of
the centroid patterns.2The laboratory
Shack-Hartmann aberrometer of Liang
and colleagues1provided adequate mea-
surements of higher-order aberrations
described by Zernike terms and conven-
tional refractive error measurements. In
the subsequent decade, Shack-Hartmann
wavefront measurement has been used
extensively in the clinical setting to
measure ocular aberrations in keratoco-
nus, dry eye, before and after refractive
surgery and cataract.3,4
Bausch & Lomb Zywave
The Zywave (Bausch & Lomb Zywave,
Rochester, NY) is a Shack-Hartmann aber-
rometer used to measure ocular aberra-
tions.2The Zywave focuses an infrared
laser beam of 785 nm on the retina, which
serves as a point source for light propa-
gated out of the eye. The Zywave provides
an adjustable optical system to compen-
sate for patient’s refractive errors and
adjusts for the subject’s far point by
fogging the image to control for accom-
modation. As a wavefront is propagated
back out of the eye, a lenslet array in the
Zywave that is conjugate with the pupil
plane focuses the wavefront into a
76-point centroid pattern on a CCD detec-
tor. The spatial displacement of each cen-
troid from its ideal location is used to
determine the slope of the aberrated wave-
front. The shape of the wavefront is deter-
mined by integration of the slopes for
each location in the pupil plane. The
Zywave uses Zernike terms to fit the slope
data and the coefficients can be used to
mathematically reconstruct the wavefront.
The Zywave measures total wavefront aber-
rations and mathematically represents
them up to the fifth-order Zernike terms.
Each Zernike term represents a specific
aberration with a specific mathematical
definition and predetermined shape.5
Each Zernike term has a corresponding
coefficient that represents the magnitude
of the wavefront shape in microns and is a
quantitative measure that represents how
much of that aberration is present.
The Zywave can give an estimate of
refractive error, representing the second-
order aberrations of the eye. The Zywave
was designed to measure refractive errors
over a range of +6.00 to -12.00 DS and up
to 5.00 D of cylinder. The Zywave is part of
the Zyoptix Diagnostic Workstation (along
with the Orbscan IIz corneal topogra-
pher) for wavefront-guided refractive
surgery.
Previous studies of the Zywave have paid
little attention to the effect of pupil size
and control of accommodation on the
repeatability and validity of estimates of
refractive error and Zernike terms. The
goals of this study were:
• to determine the repeatability and
validity of the refractive error measured
by the Zywave under manifest and
cycloplegic conditions for a range of
pupil sizes (three, five and seven milli-
metres plus the instrument’s default)
and in comparison to a conventional
autorefractor
to determine the repeatability of
higher-order aberrations under cyclo-
plegic conditions, specified as Zernike
coefficients, measured by the Zywave
for a range of pupil sizes (three, five
and seven millimetres) and compared
with the range of values found across
subjects.
METHODS
The tenets of the Declaration of Helsinki
were followed and all procedures were
approved by the Office of Research Risks
and Protection at The Ohio State Univer-
sity. Written informed consent was ob-
tained from each subject prior to any
procedures being performed. Subjects
were recruited from The Ohio State Uni-
versity College of Optometry. Subjects
were required to be at least 18 years of age
and have correctable visual acuity of at
least 6/6 in the right eye. Contact lens
wearers and patients with any ocular
disease or pathology that could affect
vision, for example, keratoconus or cata-
ract, were excluded.
Patients attended for two visits sepa-
rated by at least one week. On each occa-
sion, three refractive error measurements
were taken of the right eye with the Zywave
(Bausch & Lomb, Rochester, NY) and a
Nidek ARK–700A autorefractor (Nidek,
Fremont, CA). One drop of 1% tropicam-
ide was instilled into the subject’s right
eye and 30 minutes later, the Zywave
and autorefractor measurements were
repeated. Zywave measurements were
taken immediately after a blink to limit
tear film disruption. On one of the two
visits, the subject’s refractive error was
determined using standard subjective
techniques under cycloplegia by one of
two authors (MDT or MAB). No artificial
pupil was used. All measurements were
referenced to the spectacle plane.
The Zywave Version 3.21 software also
allows manipulation of the pupil diameter
by limiting the area of the wavefront used.
Among the data provided is an estimate of
the subject’s refractive error. Refractive
error was determined for the default pupil
size of 3.5 mm for both manifest and
cycloplegic measurements along with
pupil diameters of three, five and seven
millimetres under cycloplegia. The Zywave
software also calculates complete wave-
front aberration data in Zernike terms.
These data were determined and exported
for pupil diameters of three, five and
seven millimetres under cycloplegia. The
exported data are normalised Zernike
polynomial coefficients but do not strictly
conform to OSA, ANSI, and ISO stan-
dards. Specifically, the Zywave uses the
opposite reference for the direction of
wavefront propagation, where positive
propagation is toward the eye. As a conse-
quence, the sign of the coefficients was
reversed and the preferred notation used
(Znmfor the polynomial and Cnmfor the
corresponding coefficient).6
Data analysis
Refractive error data from the Zywave
and autorefractor were converted to the
Fourier components M, J0, and J45 for
further analysis.7Repeatability of refrac-
tive error data was assessed by comparing
the mean values for each session and for
each subject. The mean and standard
TheB&LZywave aberrometer Dobos, Twa and Bullimore
© 2009 The Authors Clinical and Experimental Optometry 92.3 May 2009
Journal compilation © 2009 Optometrists Association Australia 239
deviation of the differences were deter-
mined along with the 95% limits of
agreement (LoA) consistent with the rec-
ommendations of Bland and Altman.8The
validity of Zywave and autorefractor mea-
surements was assessed by comparing
values to the subjective refraction using
the same methods.
The repeatability of the higher-order
Zernike terms was assessed using the same
methods. The mean, SD and 95% LoA
were calculated for each Zernike term and
for each pupil size. To further assess the
impact of these values, the calculated
between-session standard deviation for
each Zernike term was compared to the
between-subject standard deviation. In
this way, the repeatability of each Zernike
term could be placed in the appropriate
context by comparing the value to the
variation across subjects.
RESULTS
Twenty-three subjects met the eligibility
criteria and completed the study. Ten
were male and 13 (57 per cent) were
female. Subjects ranged in age from 20
to 48 years (mean: 27.6 6.8 years). The
mean spherical equivalent for subjective
refraction under cycloplegia was -2.15
2.87 D (range -9.25 to +1.25 D.
Repeatability and validity of
refractive error measurements
The distribution of between-session differ-
ences in spherical equivalent are shown in
Figure 1 and the repeatability of refractive
error measurements is summarised in
Table 1. As expected, none of the mean
differences was significantly different from
zero. For the spherical equivalent (M), the
repeatability of the Zywave was better than
that of the autorefractor under both mani-
fest and cycloplegic conditions. The 95%
LoA were narrowest for the default and
three millimetre pupils under cycloplegia.
The repeatability of astigmatism showed
similar trends.
The validity of refractive error measure-
ments is summarised in Table 2. All values
are in comparison with the cycloplegic
subjective refraction. For the spherical
equivalent (M), the mean values for the
autorefractor are closest to zero. The 95%
LoA are narrowest for the autorefractor
under cycloplegia, closely followed by the
Zywave under cycloplegia for the default
and three millimetre pupil. For astig-
matism, the validity is similar for all
measurements.
For the Zywave, the spherical equivalent
showed a systematic shift in the myopic
direction as the pupil size is increased
1.00
0.75
0.50
0.25
0.00
-0.25
-0.50
-0.75
-1.00
-10.00 -8.00 -6.00 -4.00 -2.00 0.00 2.00
Mean spherical equivalent (D)
Difference in mean spherical equivalent (D)
Zywave 3 mm Zywave 5 mm Zywave 7 mm Zywave default Nidek
Figure 1. Summary mean versus difference plot comparing the Zywave at all pupil sizes
and the Nidek autorefractor under cycloplegic conditions
Measurement M J0J45
Mean SD 95% LoA Mean SD 95% LoA Mean SD 95% LoA
Nidek ARK–700A—Manifest -0.03 0.28 -0.57 to +0.52 +0.01 0.10 -0.19 to +0.22 -0.02 0.12 -0.26 to +0.22
Nidek ARK–700A—Cycloplegic +0.01 0.23 -0.45 to +0.47 +0.01 0.12 -0.22 to +0.24 +0.01 0.08 -0.15 to +0.17
Zywave—Manifest (default) +0.04 0.22 -0.39 to +0.48 +0.01 0.08 -0.15 to +0.18 -0.00 0.06 -0.13 to +0.12
Zywave—Cycloplegic (default) +0.04 0.17 -0.29 to +0.37 +0.00 0.07 -0.14 to +0.14 +0.00 0.07 -0.13 to +0.13
Zywave—Cycloplegic (3 mm) +0.04 0.14 -0.23 to +0.32 -0.01 0.11 -0.23 to +0.21 -0.01 0.09 -0.18 to +0.16
Zywave—Cycloplegic (5 mm) +0.03 0.21 -0.37 to +0.43 -0.03 0.16 -0.33 to +0.28 -0.03 0.11 -0.25 to +0.19
Zywave—Cycloplegic (7 mm) -0.02 0.16 -0.34 to +0.30 +0.01 0.09 -0.16 to +0.19 +0.00 0.06 -0.11 to +0.12
Table 1. The repeatability of refractive error measurement for the Nidek ARK–700A autorefractor and the Bausch & Lomb Zywave. All
values are in dioptres.
TheB&LZywave aberrometer Dobos, Twa and Bullimore
Clinical and Experimental Optometry 92.3 May 2009 © 2009 The Authors
240 Journal compilation © 2009 Optometrists Association Australia
from three to seven millimetres. This
trend is shown in Figure 2, which illus-
trates that the mean is -1.91 D for the three
millimetre pupil but -2.60 D for the seven
millimetre pupil. It was hypothesised that
this shift was due to spherical aberration
so the myopic shift was plotted as a func-
tion of the C40coefficient obtained for a
seven millimetre pupil (Figure 3). As can
be seen, those eyes with higher levels of
spherical aberration show the greatest
myopic shift associated with increasing
pupil size (r2=0.35).
Repeatability of higher-order
aberrations
Table 3 shows the repeatability of the
Zernike terms for the three, five and seven
millimetre pupils. For the three millime-
tre pupil, the Zywave only generates
Zernike terms through the third order.
Inspection of Table 3 suggests that repeat-
ability, as indicated by the size of the 95%
LoA, is best for the higher-order terms
and poorest for the lower-order aberra-
tions. For example, the largest standard
deviation and 95% LoA belongs to the C20
coefficient, which corresponds to the
spherical defocus. This is misleading
because for a given subject, the low order
terms are relatively large and vary consid-
erably across the subjects. In contrast,
the higher-order terms tend to be very
small in magnitude and vary little between
subjects. To compensate for this, the
within-subject, between-session standard
deviations for the seven millimetre pupil
Measurement M J0J45
Mean SD 95% LoA Mean SD 95% LoA Mean SD 95% LoA
Nidek ARK–700A—Manifest +0.06 0.40 -0.73 to +0.84 +0.06 0.16 -0.25 to +0.36 +0.00 0.12 -0.24 to +0.23
Nidek ARK–700A—Cycloplegic -0.06 0.28 -0.62 to +0.49 -0.07 0.15 -0.36 to +0.22 -0.03 0.11 -0.23 to +0.18
Zywave—Manifest (default) +0.11 0.46 -0.80 to +1.02 +0.10 0.13 -0.16 to +0.37 +0.02 0.13 -0.23 to +0.28
Zywave—Cycloplegic (default) +0.21 0.35 -0.47 to +0.90 +0.11 0.13 -0.15 to +0.37 +0.01 0.10 -0.19 to +0.20
Zywave—Cycloplegic (3 mm) +0.23 0.35 -0.46 to +0.92 +0.10 0.14 -0.16 to +0.37 +0.00 0.09 -0.18 to +0.18
Zywave—Cycloplegic (5 mm) -0.26 0.51 -1.26 to +0.75 -0.26 0.13 -0.50 to +0.01 -0.04 0.10 -0.24 to +0.16
Zywave—Cycloplegic (7 mm) -0.45 0.54 -1.51 to +0.61 +0.11 0.15 -0.19 to +0.41 -0.08 0.11 -0.29 to +0.14
Table 2. The validity of refractive error measurements compared to the subjective refractions. All values are in dioptres.
Zywave
3 mm
pupil
Zywave
default
pupil Nidek ARK-700A
Pupil diameter (mm)
2345678
Zywave
5 mm pupil
Subjective
refraction
Zywave
7 mm pupil
Mean spherical equivalent (D)
-1.00
-1.50
-2.00
-2.50
-3.00
Figure 2. Mean spherical equivalent determined by the Zywave as a function of pupil
size. The values for subjective refraction and the Nidek autorefractor are plotted as lines
for comparison.
Spherical aberration for 7 mm pupil (µm)
Difference in M (D)
7 mm minus 3 mm pupil
-2.00
-1.50
-1.00
-0.50
0.00
0.50
-0.50 0.00 0.50 1.00 1.50
Figure 3. Change in spherical equivalent refraction when pupil size is increased from
3 mm to 7 mm as a function of spherical aberration (C40) for a 7 mm pupil
TheB&LZywave aberrometer Dobos, Twa and Bullimore
© 2009 The Authors Clinical and Experimental Optometry 92.3 May 2009
Journal compilation © 2009 Optometrists Association Australia 241
from Table 3 are shown again in Table 4
along with the between-subject, within-
session standard deviations. The latter
values represent the distribution of
Zernike terms across our subject popula-
tion. The ratios of these two standard
deviations were calculated and are shown
in Table 4 and plotted in Figure 4. A low
ratio indicates good repeatability relative
to the variation within the subject popula-
tion. As would be expected, the second
order Zernike terms representing sphere
and cylinder have very low ratios indicat-
ing that the between-session variability
within a subject is very low compared to
the variability across subjects. In contrast,
some of the higher-order aberrations have
ratios of around one, indicating that a
repeated measure on a single subject will
differ by a similar amount to a new
measure on a completely different subject.
Of the higher-order aberrations, the coma
coefficient (C3
+1and C3-1) and spherical
aberration coefficient (C40) have the
lowest ratios. Analysis of the five millime-
tre pupil data shows very similar trends but
neither the data nor the analysis are
shown in the interest of space.
Zernike
coeff.
Within-
subject SD
(from Table 3)
Between-
subject SD
Ratio
C200.233 4.985 0.047
C2-2 0.064 0.787 0.081
C2
+20.102 1.467 0.070
C3-1 0.113 0.333 0.338
C3
+10.059 0.240 0.246
C3-3 0.053 0.197 0.268
C3
+30.051 0.193 0.263
C400.043 0.304 0.143
C4
+20.046 0.114 0.402
C4-2 0.034 0.065 0.524
C4
+40.051 0.093 0.546
C4-4 0.054 0.060 0.893
C5
+10.025 0.029 0.850
C5-1 0.029 0.047 0.606
C5
+30.028 0.036 0.774
C5-3 0.031 0.031 0.988
C5
+50.034 0.050 0.684
C5-5 0.038 0.031 1.221
Table 4. Comparison of the repeatability (within subject SD,
in mm) with the between-subject variability (SD, in mm) for
higher-order aberrations measured with the Zywave for 7 mm
pupil. The final column shows the ratio of these values, a
smaller value representing better repeatability.
Zernike
coeff.
3 mm pupil 5 mm pupil 7 mm pupil
Mean SD 95% LoA Mean SD 95% LoA Mean SD 95% LoA
C20+0.075 0.282 -0.478 to +0.628 +0.033 0.127 -0.216 to +0.282 +0.024 0.233 -0.433 to +0.481
C2-2 +0.011 0.037 -0.062 to +0.084 +0.009 0.050 -0.089 to +0.108 +0.016 0.064 -0.106 to +0.141
C2
+2+0.006 0.047 -0.086 to +0.098 +0.010 0.071 -0.130 to +0.150 +0.006 0.102 -0.194 to +0.206
C3-1 -0.006 0.024 -0.053 to +0.042 -0.022 0.042 -0.104 to +0.061 -0.017 0.113 -0.237 to +0.204
C3
+1+0.003 0.018 -0.031 to +0.037 +0.009 0.045 -0.080 to +0.098 +0.013 0.059 -0.103 to +0.129
C3-3 -0.005 0.023 -0.050 to +0.040 +0.008 0.035 -0.061 to +0.076 +0.005 0.053 -0.099 to +0.108
C3
+3-0.004 0.015 -0.034 to +0.025 +0.006 0.026 -0.044 to +0.056 +0.018 0.051 -0.081 to +0.117
C40-0.004 0.015 -0.035 to +0.026 -0.010 0.043 -0.095 to +0.075
C4
+2+0.001 0.013 -0.024 to +0.027 +0.008 0.046 -0.083 to +0.098
C4-2 -0.002 0.014 -0.030 to +0.026 -0.001 0.034 -0.067 to +0.066
C4
+4+0.001 0.014 -0.026 to +0.028 -0.002 0.051 -0.102 to +0.097
C4-4 -0.002 0.022 -0.044 to +0.041 -0.005 0.054 -0.111 to +0.100
C5
+1-0.000 0.010 -0.021 to +0.020 -0.003 0.025 -0.051 to +0.046
C5-1 +0.002 0.013 -0.023 to +0.027 +0.009 0.029 -0.048 to +0.065
C5
+3+0.001 0.007 -0.013 to +0.016 -0.011 0.028 -0.065 to +0.043
C5-3 -0.001 0.012 -0.025 to +0.023 -0.003 0.031 -0.064 to +0.057
C5
+5-0.002 0.010 -0.021 to +0.017 -0.009 0.034 -0.077 to +0.058
C5-5 -0.002 0.009 -0.020 to +0.016 +0.005 0.038 -0.070 to +0.080
Table 3. Repeatability of higher-order aberrations measured with the Zywave. All values are in mm.
TheB&LZywave aberrometer Dobos, Twa and Bullimore
Clinical and Experimental Optometry 92.3 May 2009 © 2009 The Authors
242 Journal compilation © 2009 Optometrists Association Australia
DISCUSSION
Repeatability and validity of
refractive error measurements
The Zywave gives valid and repeatable esti-
mates of refractive error as its measure-
ments compare favourably with the Nidek
ARK-700 autorefractor and the 95% LoA
are consistent with those found in previ-
ous studies of the repeatability of autore-
fractors.9,10 Estimates of repeatability and
validity can depend on the number of
measurements taken. Previous studies
have averaged between three and 10 mea-
surements. The Zywave also gives valid esti-
mates of a subject’s manifest refraction
and is comparable to other Shack-
Hartmann aberrometers.11–15
Two other studies have compared the
repeatability and validity of estimates of
refractive error using the Zywave. Hament,
Nabar and Nuijts11 compared Zywave mea-
surements to subjective refraction and
autorefraction in 20 myopic eyes. They
found that with a dilated pupil the Zywave
gave substantially more myopia than sub-
jective refraction (mean difference -1.10
0.46 D). For a 3.5 mm pupil, the differ-
ence was smaller but still significant (mean
difference -0.55 0.48 D). They also
report a repeatability coefficient of -0.25 to
+0.25 D based on three repeat measure-
ments during a short period. Mirshahi and
co-workers16 determined repeatability (SD
of within-session measures) to be -0.15
to +0.15 D using a similar analytical
approach in 20 patients. They reported
negligible mean differences between the
spherical equivalent values from the
Zywave and for the studies from subjective
refraction but a large range (mean 0.09 D,
range -0.81 to +1.83 D). In summary, the
Zywave-derived estimates of refractive
error data in the current study agree more
closely with subjective refraction than in
the studies of Hament, Nabar and NJuijts11
and Mirshahi and co-workers.16
The exact method of determining the
Zywave’s or any clinical aberrometer’s
autorefraction may not be fully known.
In general, clinical aberrometers have
autorefractive repeatability that is similar
or better than those of clinical autorefrac-
tors. Although higher-order aberrations
are measured with clinical aberrometers,
their fluctuating higher-order aberrations
may have minimal effects on the refractive
error data. Indeed, clinical aberrometers
have been shown to provide consistent
refractive error measurements despite
fluctuations in high-order aberrations.16,17
Consistent with the findings of Hament,
Nabar and Nuijts,11 as pupil size is manipu-
lated from three, five and seven mil-
limetres on the Zywave, the refractive
error becomes more myopic (Table 2,
Figure 2). The values of C20change in a
corresponding manner (data not shown).
This reflects the spherical aberration of
the eye and is confirmed by the correla-
tion between the myopic shift in refraction
and the C40coefficient shown in Figure 3.
The higher the magnitude of the spherical
aberration term, a higher myopic shift is
seen in spherical equivalent. This relation-
ship among spherical aberration, pupil
size and refractive error has been de-
scribed and discussed previously.18,19 The
influence of pupil size on the estimate of
spherical equivalent refractive error will
depend ultimately on the algorithm used
by the instrument and some aberrometers
adjust for the eye’s spherical aberration
to give an estimate of refractive error
approaching that obtained with a smaller
pupil.19
Repeatability of higher-order
Zernike terms
Many of the higher-order Zernike terms
measured by the Zywave in this study are
small in quantity, as many are only one-
thousandth of a micron. Because of their
small magnitude, this can give the impres-
sion that these measurements are very
consistent. In contrast, measures of
second-order aberrations—corresponding
to sphere and cylinder—appear less re-
peatable, having larger between-session
standard deviations, however, these
lower-order aberrations vary considerably
among subjects. We attempted to take a
balanced approach by referencing the
between-session standard deviations to the
corresponding between-subject standard
deviations. We assert that the calculated
ratio of these standard deviations gives a
truer indication of the repeatability of the
Zywave’s ability to estimate each Zernike
term. Figure 4 emphasises that the repeat-
ability of the second-order terms is good
with ratios less than 0.1. The repeatability
of third-order aberrations and spherical
aberration coefficients (C40) may be con-
sidered acceptable with ratios of around
0.2. In other words, the variation between
measurements on the same subject are
small compared to those between subjects.
In contrast, the repeatability of other
higher-order Zernike terms should be
SD ratio
Zernike term
1.40
C2
0C2
-2 C2
2C3
-1 C3
1C3
-3 C3
3C4
0C4
2C4
-2 C4
4C4
-4 C5
1C5
-1 C5
3C5
-3 C5
5C5
-5
1.20
1.00
0.80
0.60
0.40
0.20
0.00
Figure 4. The ratio of within-subject SD to between-subject SD for all Zernike aberration
terms measured with the Zywave for 7 mm pupil. A smaller ratio represents better
repeatability.
TheB&LZywave aberrometer Dobos, Twa and Bullimore
© 2009 The Authors Clinical and Experimental Optometry 92.3 May 2009
Journal compilation © 2009 Optometrists Association Australia 243
considered poor, with ratios closer
to 1.
A similar conclusion was drawn by Mir-
shahi and co-workers.16 Their approach
was slightly different—they calculated the
coefficient of variation for each term (SD/
mean)—but the outcomes show trends
similar to our data, with unsatisfactory
repeatability for most fourth- and fifth-
order Zernike terms. Inspection of their
Figure 2 shows that it has an appearance
very similar to our Figure 4.
With regards to higher-order aberra-
tions, there are many factors one must
examine as sources for differences in
repeatability data. For example, instru-
ment alignment,20 time between measure-
ments,20, 21 and biological variables (ocular
optics, tears, accommodation, pupil size)22
among others must be considered.
Aberrometry measurements and
wavefront-guided refractive
surgery
It is estimated that the higher-order aber-
rations of a normal and healthy eye
account for 0.25 D or less of dioptric
blur4,23,24 and yet, wavefront guided treat-
ments have increasingly become the
standard of care in corneal refractive sur-
gery.25 In part, this is because the visual
results of wavefront guided treatments are
somewhat better.26–28 Although higher-
order wavefront errors are only a small
fraction of the total optical aberrations of
the normal eye, when combined with the
additional aberrations induced by refrac-
tive surgical treatment, they can become
visually significant.29,30 Applegate, Sarver
and Khemsara31 have demonstrated that
not all aberrations have an equal influ-
ence on vision. Several third- and fourth-
order terms significantly degrade vision in
the postoperative eye, suggesting that
accurate measurements to at least this
level are needed.31
When accurate preoperative measure-
ments of aberrations are combined with
information about the magnitude of
treatment-induced aberrations, it is pos-
sible to minimise the treatment-induced
aberrations and optimise vision. The
ability to achieve this goal depends on
several factors. These include:
1. the ability to correctly measure ocular
wavefront errors
2. translation of the measured error to an
appropriate treatment plan
3. successful execution of the treatment
plan
4. a predictable biological response to the
treatment.
Here we report on only the first of these
factors that can influence visual results
after wavefront customised corneal refrac-
tive surgery.
Wavefront sensing has developed
rapidly in the field of refractive surgery
due to the understanding of not only how
refractive surgery may induce higher-
order aberrations32 but also analysis of
higher-order aberrations pre-operatively
to design a customised correction that can
achieve excellent visual performance.33
Analysing the inconsistency of some
higher-order aberrations, potentially one
may relate the importance of specific
higher-order aberrations in complete
wavefront error, despite the overall sum
being less than 0.25 D or less of dioptric
blur. Cheng and colleagues21 also pro-
posed that certain higher-order aberra-
tions are more worthy of correction than
others. Trying to correct a small and fluc-
tuating higher-order aberration may lead
to the generation of a further higher-
order aberration. Therefore, it is impor-
tant to identify the most relevant Zernike
terms, their role in determining the
overall wavefront and, ultimately, their
effect on vision when developing algo-
rithms for custom refractive surgery.
Caveats and limitations
Here we report on the performance of a
single commercially-available clinical aber-
rometer. The Zywave produces repeatable
and valid estimates of refractive error.
Given its level of sophistication compared
to traditional autorefractors, its superior
repeatability might have been anticipated.
The data were taken on the first genera-
tion of the Zywave and it is possible
that subsequent hardware and software
upgrades may further improve the repeat-
ability of this instrument. We did not
evaluate other clinical aberrometers,
which are believed to produce similar val-
ues,15,34 although differences may exist.20
One important difference between the
Zywave and other clinical aberrometers is
the relatively low spatial resolution of its
Shack-Hartmann grid. The Zywave has 76
spots on its centroid pattern while others
such as the LADARWave (Alcon Labs, Inc,
Fort Worth, TX) has 204 to 213, the
Wavescan (VISX, Santa Clara, CA) has 240
and the COAS (AMO-Wavefront Sciences,
Albuquerque, NM) has 1,452 sampling
points.35 Work may be done to analyse
benefits/limitations of the centroid pat-
terns and sampling points. It appears that
the Zywave will have a dynamic range that
is limited to calculating fewer Zernike
polynomial terms of lower frequency.15
Although this study was not specifically
designed to quantify the impact of Shack-
Hartmann spatial resolution on measure-
ment precision, we expect that this Zywave
design limitation explains some of the
poorer repeatability that we observed with
higher-order terms.
SUMMARY
The Zywave provides repeatable measures
of refractive error at the adjusted pupil
diameters under both cycloplegic and
manifest conditions over a range of refrac-
tive errors for normal eyes. The Zywave
refractive error estimates are comparable
to subjective refraction and another
autorefractor for small pupils but more
myopic when set to five or seven millime-
tres. The second-order Zernike terms
along with the spherical aberration and
coma terms derived from the Zywave show
good repeatability. Some of the higher-
order Zernike terms are small in magni-
tude and are variable between sessions.
GRANTS AND FINANCIAL SUPPORT
Supported by National Institutes of Health
grants NEI T35-07151 and K23-EY016225.
MAB has received research funding from
Bausch & Lomb that is unrelated to the
topic of this manuscript.
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Corresponding author:
Dr Michael J Dobos
The Ohio State University College of
Optometry
338 West 10th Avenue
Columbus, Ohio 43210-1280
USA
E-mail: dobos.10@osu.edu
TheB&LZywave aberrometer Dobos, Twa and Bullimore
© 2009 The Authors Clinical and Experimental Optometry 92.3 May 2009
Journal compilation © 2009 Optometrists Association Australia 245
... [6] Four wavefront aberrometers commonly used in refractive surgery are the Zywave (Bausch and Lomb, Rochester, NY, USA), OPD-Scan III (Nidek Technologies, Gamagori, Japan), iDesign (Abbott Medical Optics, Inc., Santa Ana, CA, USA), and GALILEI™ G2 (Zeimer Ophthalmic Systems AG, Port, Switzerland). These devices are based on different measurement principles; Zywave and iDesign use Hartmann-Shack, [7,8] while OPD-Scan III uses automatic retinoscopy, [9] and GALILEI™ G2 calculates HOA with its dual-Scheimpflug and Placido topography system. [10] To the best of our knowledge, this study is the first to assess the agreement between these devices. ...
... Zywave is an early Hartmann-Shack aberrometer, which measures 75 data points through the pupil and calculates up to five orders of Zernike coefficients. [7] iDesign is another Hartmann-Shack sensor that gathers more than 1,250 data points from up to a 7.0-mm pupil. [8] OPD-Scan III is a five-in-one device with topographer, keratometer, pupillometer, and wavefront aberrometer functions. ...
... Automatic averaging of the three measurements taken with Zywave and OPD-Scan III precluded evaluating repeatability with the examinations conducted in this study; however, previous studies have assessed the reproducibility of these devices. [7][8][9][10]33,34] In clinical practice, the importance of adhering to each manufacturer's recommendations regarding the number of aberrometry measurements is required for successful laser refractive surgery outcomes. [1] Conclusion This study has reported significant differences between most devices, some of which exceed the JND of the respective HOA, and thus may compromise the visual outcome of WFG LASIK. ...
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Purpose: To evaluate the agreement of selected higher order aberration measurements between aberrometers based on three different wavefront technologies. Methods: Twenty-three eyes of 23 participants were compared between Zywave, OPD-Scan III, and iDesign aberrometers, for total ocular aberrations. Participants were between 19 and 69 years of age, and exclusion criteria were previous ocular surgery or trauma, contact lens wear within the preceding 2 weeks, and ocular or systemic disease. Corneal aberrations were compared between the OPD-Scan III and GALILEI™ G2 aberrometers. Zernike coefficients of vertical and oblique trefoil, vertical and horizontal coma, and spherical aberration were analyzed in R software. Results: In all, 276 scans were captured in total, with a male-to-female ratio of 11:12. Total ocular vertical coma [mean difference (MD) = 0.026 μm, P < 0.005], vertical trefoil (MD = 0.033 μm, P < 0.05), and spherical aberration (MD = 0.022 μm, P < 0.05) differed significantly between the iDesign and OPD-Scan III. Differences in total vertical (MD = 0.072 μm, P < 0.05) and oblique trefoil (MD = 0.058 μm, P < 0.05) were demonstrated between the Zywave and OPD-Scan III, and spherical aberration (MD = 0.030 μm, P < 0.005) between iDesign and Zywave. iDesign corneal horizontal coma (MD = 0.025 μm, P < 0.05) and spherical aberration (MD = 0.043 μm, P < 0.005) measurements were significantly different between the GALILEI™ G2 and the OPD-Scan III. Conclusion: Zywave, iDesign, and OPD-Scan III, and GALILEITM G2 and OPD-Scan III may be used interchangeably for their total ocular and corneal wavefront functions, respectively; however, care must be taken if using these devices for guiding ablation or monitoring corneal disease.
... Several previous studies observed a poor repeatability in ocular aberrations from the third order with other aberrometers. 26,30 Similar intrasubject repeatability was found with this new aberrometer in comparison with previous publications [24][25][26][27]29 and better than the Otero et al. 23 study (Table 4). On the contrary, with this aberrometer, we found a good intrasubject repeatability for all Zernike coefficients except for the quatrefoil. ...
... Several previous studies observed a poor repeatability in ocular aberrations from the third order with other aberrometers. 26,30 Similar intrasubject repeatability was found with this new aberrometer in comparison with previous publications [24][25][26][27]29 and better than the Otero et al. 23 study (Table 4). On the contrary, with this aberrometer, we found a good intrasubject repeatability for all Zernike coefficients except for the quatrefoil. ...
... This fact could be because at 4.0 mm, the Zernike coefficients from third or fourth order are decimal lower values than at 6.0 mm and this leads to a high variability as commented before. When the repeatability outcomes were compared with other aberrometers, similar or higher values of ICC were obtained with this new pyramidal wavefront sensor [25][26][27][28] (Table 4). ...
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Purpose To evaluate the intrasubject repeatability of the ocular aberrometry obtained with a new ocular pyramidal aberrometer technology in a sample of normal eyes. Methods A total of 53 healthy eyes of 53 subjects with ages ranging from 18 to 45 years were included in this study. In all cases, three consecutive acquisitions were obtained. Intrasubject repeatability of the measurements with a pyramidal aberrometer was calculated. Intrasubject repeatability for 4.0- and 6.0-mm pupils was evaluated within the subject standard deviation (Sw) and intraclass correlation coefficient. Results Low values of the Sw and intraclass correlation coefficient outcomes close to 1 were observed for the sphere and cylinder at 3.0-mm pupil size. Most low Sw and intraclass correlation coefficient values close to 1 were observed for total, low-order aberrations and higher-order aberrations root mean square and for each Zernike coefficient analysis (intraclass correlation coefficient ⩾0.798) at 4.0-mm pupil size, with more limited outcomes for the aberrometric coefficient of Z(4, 4) with an intraclass correlation coefficient of 0.683. For a 6.0 mm pupil diameter, low Sw and intraclass correlation coefficient values close to 1 were observed for all aberrometric parameters or Zernike coefficients analyzed (intraclass correlation coefficient ⩾0.850). Conclusion The new pyramidal aberrometer Osiris provides repeatable and consistent measurements of ocular aberrometry measurements in normal eyes.
... The use of such systems is often involved in consultation and decisionmaking related to refractive surgery [10]. Wavefront aberrometers show the aberration of a light wave after it has passed through the eye's optical system [11,12]. Zernike and Fourier expansion series polynomials are mathematical tools used in modern optics to quantify aberrations and characterize the optical surface in three dimensions [1]. ...
... Every technique has advantages and disadvantages, mainly related to the amount of processing power and optical aberration. A Hartmann-Shack sensor is used by most wavefront-sensing devices that work in tandem with excimer lasers [12,13]. Additional techniques with their own benefits and drawbacks include the Tscherning method, ray tracing, dynamic skiascopy, and pyramidal wavefront sensing (PWS) [11]. ...
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... ey found similar values of repeatability for the sphere (r � 1.96 D; ICC � 0.983) compared to the Eye Refract in the keratoconus group (see Table 3). In healthy subjects, several studies measured objective refraction with different aberrometers, obtaining r values between 0.28 D and 0.59 D for the spherical equivalent [16,[26][27][28][29][30]. ese values were slightly better than the ones obtained with the Eye Refract in the healthy group (see Table 3). ...
... With an aberrometer, Piñero et al. [25] found better repeatability in keratoconus subjects for J0 (r � 0.45 D) compared to the Eye Refract in the keratoconus group, but worse for J45 (r � 1.55 D) (see Table 3). In healthy subjects, several studies measured astigmatism with different aberrometers, obtaining similar or slightly better values of repeatability compared to the current study [16,[26][27][28][29][30]. ...
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... Other studies analyzed the intersession repeatability of MSE with different wavefront autorefractors. In adults, several authors reported values of r between 0.28 D and 0.53 D [2,16,23,37,38], which agrees with the adults of the current study (Table 3). All these wavefront autorefractors keep their differences within a range of ±0.25 D. No studies assessing the intersession repeatability with wavefront autorefractors in other age groups were found in the scientific literature. ...
... In J45, since the differences between both wavefront autorefractors in terms of r were inferior to 0.25 D (except for presbyopes) and that the magnitude of J45 obtained with both wavefront autorefractors was substantially lower than MSE and J0 (Table 2), the improvement in J45 repeatability with the VX110 was not considered clinically relevant. In adults, other studies reported similar values of r in terms of J0 and J45 with different wavefront autorefractors [2,16,23,37,38]. ...
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... Some authoritative sources have argued that cycloplegic refraction should be the gold standard for epidemiological studies of myopia 35 . While we agree, autorefractors may vary in the ability of their fogging mechanism to relax accommodation in adults and those with a larger entrance pupil may result in changes in refraction with cycloplegia due to ocular aberrations, rather than accoomodation 35,36 . The myopia prevalence estimates from NHANES 13 www.nature.com/scientificreports/ the 1980s are lower than the 1999-2004 NHANES estimates in 40-60-year-olds but higher than the overall prevalence in 1971-1972 and none used a cycloplegic. ...
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Purpose: The aim of this work is to determine and compare the distribution and influence of higher-order aberrations (HOAs) both clinically and experimentally between different refractive errors. Methods: Commercially available Shack-Hartmann aberrometer was employed to measure the HOA clinically in human eyes. Experimentally, HOA was measured in a model eye by simulating various refractive errors by constructing an aberrometer based on the same Shack Hartmann principle. One-way analyses of variance and simple regression were employed to analyze the distribution and influence of HOA among various refractive errors. Results: A total of 100 eyes were clinically measured for aberrations, of which 35, 50, and 15 eyes were emmetropes, myopes, and hyperopes, respectively. Out of the total root mean square (RMS) value, the HOAs found in the human eyes were 23%, 7%, and 26% and in the model eye, it was 20%, 8%, and 10% between emmetropes, myopes, and hyperopes, respectively. The mean higher-order RMS was almost similar between the groups and among various refractive errors. There was no statistical significance between the individual Zernikes except for the coma in both human and model eyes. Conclusion: The mean HOA is similar amidst the different refractive errors. The presence of 23% HOA in emmetropes signifies that larger part of the human eye is capable of complying with HOA without compromising the image quality. This work signifies that HOA does not play an important role in image clarity for human eyes with regular refractive surface unlike irregular refractive surfaces.
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Introduction: This study aimed to evaluate the repeatability and agreement of Anterion with Pentacam HR and Orbscan II in corneal parameters after photorefractive keratectomy (PRK). Methods: This prospective study involved 42 patients (42 eyes) aged between 20 and 40 years undergoing PRK surgery. Corneal measurements were measured two times using Anterion in order to assess the repeatability of this device. Then, the same parameters were measured using Pentacam and Orbscan in order to determine the agreement of Anterion and the other two devices in measuring corneal parameters after PRK. Intraclass correlation coefficient (ICC) checked Anterion’s repeatability. Also, ICC and means of the 95% limits of agreement (LoA) were used to assess the agreement of Anterion results with those of the two other devices. Results: Anterion demonstrated high to moderate repeatability in corneal parameters post-PRK, except for anterior flat keratometry (ICC = 0.73), 4th order root mean square (RMS), and horizontal trefoil (ICC < 0.75). While Anterion and Pentacam showed good agreement in corneal topography and tomography (ICC > 0.90, P < 0.05), they were only interchangeable in keratometric parameters. Additionally, no agreement was observed between Anterion and Pentacam in aberration parameters after PRK. Although Anterion and Orbscan exhibited agreement in anterior average keratometry and central corneal thickness (CCT) (ICC > 0.90, P < 0.05), it was not clinically interchangeable. Conclusion: Anterion demonstrated notable repeatability in most corneal parameters after PRK. Although there was good agreement between Anterion and Pentacam HR in measuring corneal topography and tomography, their interchangeability was limited to other values. Furthermore, Anterion and Orbscan II were not clinically interchangeable.
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Purpose: To investigate the prevalence and repeatability of high-order aberrations (HOAs) from non-cyclopleged eyes in 1515 children and adolescents 2.5-18 years of age. Methods: The Leipzig Research Centre for Civilization Diseases (LIFE)-Child study is a population-based, prospective, observational single-centre study that investigates the development of children and adolescents in Germany. Wavefront measurements were repeated three times in each eye of 1515 healthy subjects. Results were described by 36 Zernike coefficients for a 5 mm reference pupil diameter. Short-term repeatability is given for each coefficient. The impact on vision is described by the root mean squared (RMS) value of the HOA Zernike coefficients. Results: High-order aberrations were dominated by five contributions. For 1004 right eyes: spherical aberration (c12 = 0.06 ± 0.07 μm), coma (c7 = 0.03 ± 0.09 μm, c8 = 0.03 ± 0.06 μm) and trefoil (c6 = -0.01 ± 0.07 μm, c9 = 0.008 ± 0.06 μm). The RMS value was 0.18 ± 0.06 μm. Modes higher than fourth order do not contribute clinically to the aberrations. HOAs show no clinically significant dependency with age. Instead, HOA values agree well with previous results on aberrations in adult eyes. Spherical aberration was highly correlated between the two eyes. Repeatability was worst for coma, 0.033 μm, due to variability in the alignment of the pupil centre. The left eye showed, on average, a 0.08 mm larger pupil diameter than the right eye (p < 0.02). Conclusions: Across the age span from 2.5 to 18 years, we see the same distribution of HOA as for adults. We established that only five Zernike coefficients, spherical aberration, coma and trefoil were of clinical significance in healthy eyes. A high correlation between the two eyes for spherical aberration suggests a common blueprint for each eye in any one subject.
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purpose. To evaluate the stability of clinical monochromatic aberrometry measurements over a wide range of time scales. methods. Monochromatic aberrations in four normal eyes were measured with a clinical Shack-Hartmann aberrometer. A chin rest or a supplemental bite bar attachment was used to stabilize head and eye position. Five repeated measurements were taken within one test (5 frames, t < 1 second) without realignment. With realignment between each measurement, aberration measurements were repeated five times (t < 1 hour) on each day, at the same time of day on five consecutive days, and again on 5 days at monthly intervals. A control experiment studied the effect of systematically misaligning the eye to determine whether fixation errors can account for the variation in the repeated measurements. results. Variability of wavefront root mean square (RMS) error (excluding defocus and astigmatism) was tracked across repeated measurements. Variances for different time scales were: 8.10 × 10⁻⁵ μm² (t < 1 second), 3.24 × 10⁻⁴ μm² (t < 1 hour), 4.41 × 10⁻⁴ μm² (t < 1 week), 9.73 × 10⁻⁴ μm² (t < 1 year). Bite bar and chin rest data were almost identical. Rotational fixation error up to 3° accounts for only part of the variability. conclusions. Increased variability in aberration maps between days and months indicates biological fluctuations that are large enough to prevent achievement of “perfect vision,” even in the unlikely event that spherical and astigmatic refractive errors are corrected perfectly. However, lack of stability does not justify withholding treatment. A lasting benefit of aberration correction is expected despite temporal variability.
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In response to a perceived need in the vision community, an OSA taskforce was formed at the 1999 topical meeting on vision science and its applications (VSIA-99) and charged with developing consensus recommendations on definitions, conventions, and standards for reporting of optical aberrations of human eyes. Progress reports were presented at the 1999 OSA annual meeting and at VSIA-2000 by the chairs of three taskforce subcommittees on (1) reference axes, (2) describing functions, and (3) model eyes. The following summary of the committee’s recommendations is available also in portable document format (PDF) on OSA Optics Net at http://www.osa.org/.
Conference Paper
In response to a perceived need in the vision community, an OSA taskforce was formed at the 1999 topical meeting on vision science and its applications (VSIA-99) and charged with developing consensus recommendations on definitions, conventions, and standards for reporting of optical aberrations of human eyes. Progress reports were presented at the 1999 OSA annual meeting and at VSIA-2000 by the chairs of three taskforce subcommittees on (1) reference axes, (2) describing functions, and (3) model eyes.
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The field of aberrations of the human eye is moving rapidly, being driven by the desire to monitor and optimise vision following refractive surgery. In this paper, I discuss the different ways of representing aberrations of the human eye, the terminology used, how wave aberrations are used to determine refractions, the influence of pupil size on aberrations, how to compare right and left eye aberrations, how aberrations can be manipulated into different forms, how to make corrections for changes in wavelength, the appropriate ocular axis, and corneal and lenticular components of the aberrations.
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The efficacy of the Shack-Hartmann technique for measuring the optical aberrations of the eye was evaluated for four classes of clinical conditions associated with optically abnormal eyes. These categories (with specific examples) are: anomalies of the tear film (dry eye), corneal disease (keratoconus), corneal refractive surgery [laser-assisted in situ keratomileusis (LASIK)], and lenticular cataract. We show that in each of these cases, it is possible to obtain at least a partial topographic map of the refractive aberrations of the patient's eyes, but severe losses of data integrity can occur. We further show that the Shack-Hartmann aberrometer provides additional information about the eye's imperfections on a very fine spatial scale (< 0.4 mm) which scatter light and further degrade the quality of the retinal image. Taken together, spatial maps of the variation of optical aberrations and scatter across the eye's entrance pupil represents an improved description of the optical imperfections of the abnormal eye.
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In clinical measurement comparison of a new measurement technique with an established one is often needed to see whether they agree sufficiently for the new to replace the old. Such investigations are often analysed inappropriately, notably by using correlation coefficients. The use of correlation is misleading. An alternative approach, based on graphical techniques and simple calculations, is described, together with the relation between this analysis and the assessment of repeatability.