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Fig 1.

Schema of IOL artificial eye.

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Fig 1 Expand

Table 1.

Optical lens data of the artificial eye.

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Table 1 Expand

Table 2.

IOL specifications and summaries of data from each manufacturer.

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Table 2 Expand

Fig 2.

LCA840-561 as a function of IOL’s power.

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Fig 3.

LCA840-561 as a function of age.

Dotted lines indicate the prediction intervals, and the dashed line indicates extrapolation of regression beyond the age range.

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Fig 3 Expand

Fig 4.

The Cauchyʼs fittings for each average of LCA.

Fittings were plotted using the wavelength 590 nm as an offset wavelength. Dotted lines indicate extrapolations of regressions. Symbols indicate measured points for each IOL.

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Fig 4 Expand

Fig 5.

The results of spherical aberration of each IOL type.

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Fig 5 Expand

Fig 6.

The results of HOA RMSx and total HOA RMS of each IOL type.

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Fig 6 Expand

Fig 7.

The results of polychromatic MTF simulations with LCA but without HOA.

The results of Alcon, HOYA XY-1, and AMO IOLs with the power +20 D, and the average of phakic eyes.

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Fig 7 Expand

Fig 8.

All polychromatic MTF results of IOLs.

Alcon (Left), HOYA XY-1 (Center), and AMO (Right) IOLs. Only the MTF in horizontal, with LEF considered, is shown in the figures.

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Fig 8 Expand

Fig 9.

The results of VSOTFs.

Results for phakic eyes that have three different degrees of HOA and results for eyes with Alcon’s IOL, HOYA XY-1’s IOL, and AMO’s IOL that have two different degrees of HOA for each manufacturer.

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Fig 9 Expand

Fig 10.

The VSOTFs as a function of LCA840-561.

The VSOTFs were calculated by considering both HOA and LCA.

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Fig 10 Expand

Fig 11.

The VSOTFs as a function of HOA RMS.

The VSOTFs were calculated by considering both HOA and LCA. The quadratic regressions for each manufacturer and for phakic eyes are also shown.

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Fig 11 Expand

Table 3.

The results of reflectivity and interferometry.

When values from the manufacturers are available, they are provided in parentheses.

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Table 3 Expand

Fig 12.

The results of refractive index chromatic dispersion of IOLs.

Results correspond to the Cauchy’s equation coefficients in Table 5. Dotted lines indicate extrapolations.

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Fig 12 Expand

Table 4.

The results of HSWA measurements for the artificial eye.

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Table 4 Expand

Table 5.

Cauchy’s equation coefficients of chromatic dispersion of the refractive index, refractive index of 555 nm and d-line, and Abbe’s number.

The chromatic dispersions were estimated by using the HSWA results of IOLs with the power +30 D.

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Table 5 Expand

Fig 13.

Calculated LCA and measured LCA with HSWA.

A Deming regression line is shown as a solid line and confidence intervals (α = 0.05) are shown as dashed lines. We acquired the ACD data for only 8 of 11 of Alcon’s IOLs, and the plot sizes were larger for the results using ACD data.

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Fig 13 Expand

Table 6.

Comparison of our results with other researchers’ results corresponding to comparable spectral regions.

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Table 6 Expand

Table 7.

The LCA840-561 of each surface, total LCA840-561, corneal LCA840-561, and LCA840-561 of IOL were calculated for each kind of IOL with the paraxial approximation.

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Table 7 Expand

Table 8.

The LCA840-561 of each surface, total LCA840-561, corneal LCA840-561, and LCA840-561 of the lens were calculated for the Navarro schematic eye [39], the Le Grand schematic eye [18], and the modified Le Grand schematic eye with the paraxial approximation.

We changed the Abbe’s number of the lens from 50 to 45 for the Le Grand Schematic eye.

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Table 8 Expand