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OptiSpheric®

Applications
 
Diopter Power
 
The diopter power of an IOL is defined as the reciprocal of the reduced paraxial focal length in aqueous humor. From the measured effective focal length of the IOL, the power can be determined directly when the measurement is made in situ.

When measuring in air the IOL software converts the diopter power of the IOL for in situ

conditions taking into account the design conversion factor of the lens. Measuring in air leads to easier handling of the lenses and fast throughput in production conditions for example when using a tray with several tens of IOLs.

The concept of lens power is linked with the magnification of a lens. Measuring the magnification of the complete optical set up including the IOL under test is used to calculate the IOL dioptric power. This is one of the methods proposed by the ISO 11979 standard as a basis of power measurement. Being the fastest and most accurate method it is used in the OptiSpheric®IOL equipment.

The setup for diopter power measurement includes a collimator which projects the image of a double slit to infinity. The parallel beam emerging from the collimator enters the IOL under test and forms an image of the target in the focal plane of the lens under test. This image is collected by the microscope and focused on the high resolution CCD camera.

The measuring head with the CCD camera is accurately moved up and down using the autofocus stage until the image of the double slit is sharply detected on the monitor.

In the best focus position the size of the target image is precisely determined with the CCD camera with subpixel accuracy.

The Effective Focal Length (EFL) of the lens under test is simply calculated using the magnification ratio between the target size and the image size.

From the measured EFL, the power of the lens is calculated with an accuracy of ± 0.1 % for diopters from 2 to 40.

OptiSpheric®IOL is supplied with calibration files for a wide measurement and wavelength range. Only Trioptics instruments are calibrated using master samples certified by the International Standard Institutes (PTB-Germany, NPL-UK or NIST –USA). The accuracy specified for OptiSpheric® IOL is thus directly traceable to international standards

 

Setup

Resolution Efficiency

The historical way of characterizing IOLs was to measure the resolution efficiency which is also available with the OptiSpheric® IOL. The principle is based on examining the image of an USAF 1951 test chart in the focal plane of the IOL in air using an aperture stop of 3.0 ±0.1 mm. From this examination, the finest pattern (e.g. Group G, Element E) which can be resolved is determined. The resolution efficiency is then calculated by comparison of the spatial frequency of the resolution limit with the cut-off frequency of the diffraction limited system.

This subjective way of determining the resolution of the IOL can be replaced by an objective measurement procedure based on the MTF measurement by taking into account the human eye contrast sensitivity function (CSF).

USAF Target

MTF-Measurement

The Modulation Transfer Function (MTF) is a parameter describing objectively the performance of optical imaging systems. Additionally MTF can be calculated from the lens design data which provides the manufacturers the possibility to compare the image quality of the manufactured lenses with the design expectations.

The resulting image produced by a lens or another optical system will always be somewhat degraded due to aberrations and diffraction phenomena. As a consequence, bright areas will not appear as bright as they do in the object, and dark or shadowed areas will not be as black as those observed in the original patterns.

The MTF is describing the ability of an optical system to transfer the details of an object to the image in terms of contrast and has the value 1 for a perfect contrast reproduction

and the value 0 for a system being unable to produce any image contrast.

The measuring process includes a collimator projecting a target with a suitable pattern typically a slit. The IOL under test collects the light from the target and transfers it into its own image plane. The high performance microscope lens picks up this image and focuses it onto the high resolution CCD-camera. The intensity profile of the target is scanned electronically in both the radial and tangential directions. The data is collected and, by using Fourier Transform techniques, the MTF is calculated and displayed on the PC-monitor in real-time.

The software calculates and displays the MTF value at selected spatial frequencies, the theoretical diffraction limited MTF-graph and the effective MTF-graph.

Instead of using a slit as reticle, evaluation of special target patterns with proprietary design developed by TRIOPTICS gives different advantages:

Using a cross target for example has the advantage of giving simultaneous measurement of the MTF in tangential and sagittal directions.

Using square targets allows for the simultaneous measurement of EFL and MTF in both sagittal and tangential directions. In this way OptiSpheric®IOL provides consistent accuracy and astigmatism information at an unmatched speed of measurement.

When using a pinhole target, the MTF is obtained by the analysis of the Point Spread Function (PSF) of the lens instead of the line spread function.

This method has a significant advantage compared with the slit method since it shows
the MTF of the lens in all azimuth directions.

Toric IOL can be described much faster and by this way the astigmatism axis are easily determined. Nevertheless this measurement method require a very high resolution CCD camera being more expensive than the one for the standard slit method.

MTF of IOL is recommended to be tested in situ. The Standard or Advanced Model Eye, whose own optical aberrations are negligible, may be used to hold the IOL.

Point Spread Function
Point Spread Function

 

2D
2D-Display of the MTF with Astigmatism axis

Back Focal Length

The Back Focal Length (BFL) is the distance from the lens vertex to the rear (back) focal point of the lens. To measure the BFL, in a first step the Measuring Head equipped with microscope objectives or achromats is focused to the vertex of the lens (sample) surface. The illuminated reticle of the measuring head is projected on the lens vertex, reflected back and focused again on the CCD-camera.

In a second step the accurate finding of the focal plane position of the lens (sample) is accomplished in the same way as in the power and MTF measurement.

The distance between these two positions is accurately measured to determine the BFL.

Back Focal Length

Radius of Curvature

The measurement of radius of curvature is similar to the BFL measurement. Focusing is now performed on the lens vertex and in the center of curvature of the surface under test. The distance is measured in the same way as the BFL.

The best focus positions for lens vertex and center of curvature are again found using the autofocus feature of the OptiSpheric®IOL.

 

Read more about MTF measurement and autocollimators.
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