Advanced
A Study of Optical Properties of Intraocular Lenses and of Measurement of the Index of Reflection for an Unknown Liquid
A Study of Optical Properties of Intraocular Lenses and of Measurement of the Index of Reflection for an Unknown Liquid
Journal of the Optical Society of Korea. 2012. Sep, 16(3): 236-242
Copyright ©2012, Optical Society of Korea
Color versions of one or more of the figures in this paper are available online.
  • Received : August 08, 2012
  • Accepted : August 08, 2012
  • Published : September 25, 2012
Download
PDF
e-PUB
PubReader
PPT
Export by style
Share
Article
Author
Metrics
Cited by
TagCloud
About the Authors
Won Don Joo
Manufacturing Technology Center, Samsung Electronics, Suwon 443-742, Korea
wdoptic@naver.com
Mee Suk Jung
Department of Nano-Optical Engineering, Korea Polytechnic University, Siheung 429-793, Korea
Abstract
In general, such methods as interferometers or wavefront sensors are commonly used for testing of an optical system and optical components. In these cases, the surrounding environments are unlikely to affect the measurements. On the other hand, intraocular lenses of hydrophilic materials with special properties experience a certain difficulty in testing the optical properties. An intraocular lens is dried in the air, which causes deformation and changes the optical characteristics such as index of refraction and thickness. Thus, it is hard to measure the optical characteristics of an intraocular lens by using common methods. In this study, a special structure is used for measuring of the transmission wavefront aberration and effective focal length of an intraocular lens of hydrophilic materials by using a Shark-Hartmann sensor among the various measuring methods. As an application of this measuring method, this study shows a simple method to measure the index of refraction of unknown liquids with a plano-convex lens with a well known index of refraction. Also, this method is used to measure the optical properties of a plano-convex such as index of refraction and curvature by using a liquid with a well known index of refraction.
Keywords
I. INTRODUCTION
One of the surgeries common in the area of ophthalmology is cataract surgery. There are various types of this surgery, and the common process is to break and suck in the lens through keratotomy and then insert and fix an intraocular lens in the spot. Recently, as medical technology and intraocular lens production techniques have developed, the expectation of the surgery result is higher than ever before. When it comes to cataract surgery, although the medical aspects are of importance, the evaluation of the optical characteristics of the intraocular lens inserted into the eyeball is also vital [1 - 5] since the intraocular lens, in replacement of the natural lens, affects the optical power of the eye to a large degree. When the optical power of the intraocular lens put into the eye is not appropriate or when aberrations are high, the eyes may not properly work. For this reason, it is essential to include precise testing on optical properties such as effective focal length (EFL) and transmission wavefront aberration of the intraocular lens.
Transmission wavefront aberration of common lenses may be readily evaluated by means of the interferometer or Shack-Hartmann sensor (S-H sensor) [6 - 8] . There are various methods to measure EFL of lenses including, y’tan(θ ) method, Nodal slide method, Cornu method, Moire deflectometry, Talbot interferometry, Fizeau interferometry, and Shack-Hartmann wavefront analysis [9 - 12] .
However, since an intraocular lens needs to be tested in liquid to maintain the optical properties during the testing process, common methods as above may not be enough. This study, therefore, takes into consideration for measuring the transmission wavefront aberration of the intraocular lens the fact that the surface of the liquid is flat under gravity and that the S-H sensor makes it easy to compensate for the aberration of the optical system except for the intraocular lens in the process of measuring. In addition, since the use of the S-H sensor enables the locating of the intraocular lens image to be more accurate, a very useful method to measure EFL of intraocular lens is introduced by means of this characteristic. In utilization of this EFL measuring method, this study introduces a simple method to measure the index of refraction of an unknown liquid.
II. DESIGN AND PRODUCTION OF INTRAOCULAR LENSES
In designing an intraocular lens, it is of great importance to consider the intraocular lens materials and the condition of the eyes for which the intraocular lens is used. In general, the material of the intraocular lens is sensitive to humidity, and thus the result in the testing after production may not satisfy the intended requirements although the performance seems satisfactory in the design.
Most lenses are used in air after production. As an intraocular lens, however, is used in the eye, the condition in the eye should be considered when the lens is designed and tested for satisfactory performance.
On the assumption that the eyes are in a normal condition, an intraocular lens was designed based on the eye model in Table 1 provided by “Zemax models of Human Eye” of the Zemax Knowledge base [13] .
The intraocular lens was designed to minimize RMS wavefront error (RMS WFE) in an eye with the pupil size 5 mm, thickness 1.5 mm and hydrophilic acrylic. The location of the intraocular lens in the eyeball was 3.2 mm from the cornea.
Table 2 shows the design data of the intraocular lens, and we can see that the RMS wavefront error and EFL of the intraocular lens in deionized water are 0.02λ and 53.12 mm at wavelength 555 ± 10 nm in design, respectively.
Hydrophilic acrylic, used as a material for the intraocular lens, is easy to produce, but the hydrophilic nature causes
Eye model provided by “Zemax models of human eye” of Zemax knowledge base
Lager Image
Eye model provided by “Zemax models of human eye” of Zemax knowledge base
Data of intraocular lens design
Lager Image
Data of intraocular lens design
Lager Image
A sample of intraocular lens.
the manufacturing precision to be affected a lot by humidity. Thus, a lot of experience is necessary to get proper optical properties in consideration of such aspects as contraction and expansion of the intraocular lens in the production. For manufacturing of the intraocular lens, Precitech NanoForm 250 with feedback control method was used for ultra-precision processing. The sample of intraocular lens is presented in Fig. 1 .
III. MEASUREMENT OF WAVEFRONT ABERRATION AND EFL OF AN INTRAOCULAR LENS
As mentioned in the introduction, the EFL and transmission wavefront aberration of an intraocular lens are measured by means of the S-H sensor. The problem is, though, that precise measuring of the optical characteristics such as thickness, curvature, and index of refraction is impossible by means of common methods since an intraocular lens is very sensitive to humidity. Since the intraocular lens exists in a liquid in the eye, the intraocular lens should be in liquid for accurate measuring. In this study, therefore, a specially designed intraocular lens holder is used to measure the optical characteristics of the intraocular lens while it is in deionized water. The intraocular lens holder is a cylinder type, metal holder of deionized water, which is sealed by means of the cover glass at the bottom of the holder so that light can be transmitted through it. With this intraocular lens holder held vertically, deionized water is put into it so that the intraocular lens is immersed. Then the set of water + intraocular lens + water + cover glass is formed. Since it is under gravity, this lens set can be regarded as a set of plano-convex-plano-plano. In addition, since changes of the thickness of the deionized water and the cover glass are not related to EFL of the lens set, the amount of water and the thickness of cover glass do not affect the measuring result and in the transmission wavefront aberration of intraocular lens too, the amount of water has little effect on it.
- 3.1. Shack-Hartmann Sensor
Basically, when a deformed wavefront goes through the
Lager Image
The spot shift upon the incidence of a deformed wavefront.
S-H sensor, it provides accurate measurements of the wavefront shape by analyzing the location of spots formed by imaging a beam of light onto a CCD with a microlens array (MLA).
In other words, when a deformed wavefront goes through a MLA, the location of the spots may be changed by each microlens depending on the tilt of the wavefront as illustrated in Fig. 2 . As is well known, the partial derivatives relative to x and y of wavefront are determined by the spot shifts of x and y, respectively, as well as by the focal length of the microlens as shown Eq. (1) [14 - 16] .
Lager Image
where W(x,y) describes the shape of the wavefront, f is the focal length of microlens and Δx and Δy are determined by calculating the center position of spots and subtracting the corresponding reference positions.
One of the outstanding advantages of the S-H sensor in measuring a wavefront is that the wavefront of a target object can be calculated using only the relative spot shift from the spot position formed by the optical system with the target object removed.
Thus, the quality of the optical components in measuring the optical system is not important, which makes it easy to measure the optical performance of an intraocular lens in liquid.
In general, wavefront aberration can be expressed as a superposition of Zernike polynomials [17 - 18]
Lager Image
where N nm is the normalization factor.
Lager Image
Using the data Δx and Δy obtained from the Shack-Hartmann wavefront sensor, the wavefront can be fit to a Zernike polynomial expansion where the expansion coefficients are determined using the least square estimation [14 - 17] .
- 3.2. Measuring of the Transmission Wavefront Aberration of an Intraocular Lens
The system as in Fig. 3 is formed to measure the wavefront aberration of an intraocular lens. The narrow band pass filter (555 ± 10 nm) on the white light source was used. The fiber was used to spread the light vertically from top to bottom, and the half ball lens was adopted to focus it on the 3 μm pinhole. With the pinhole as the light source, a collimated beam with 5 mm diameter was formed by means of the collimator and 5 mm aperture. This beam goes through the intraocular lens holder specially designed as above. The collimated beam into the intraocular lens is focused by the intraocular lens in deionized water. The focused beam goes through the infinity-corrected objective lens, forms the collimated beam, and enters the S-H sensor. In this experiment, the pinhole unit and sensor unit in Fig. 3 are designed to move quantitatively in the direction of the z-axis.
The main goal is to measure the transmission wavefront aberration of the intraocular lens only, and thus the wavefront aberration by deionized water, cover glass, and objective lens after the pinhole should be removed.
First, the intraocular lens holder was removed to measure the wavefront aberration by the objective lens, and the pinhole was put on the focal point of the objective lens to
Lager Image
The scheme to measure wavefront aberration.
measure the spot shift (Δx obj , Δy obj ) i by deformed wavefront aberration through the objective lens, where i indicates 1,2,3...i max , and i max the number of microlenses occupied by the beam transmitted into the S-H sensor.
Second, to measure the wavefront deformation by the cover glass and deionized water in the intraocular lens holder, the collimated beam is made incident on the intraocular lens holder, then the cover glass and deionized water will deform the collimated beam, and then it is possible to measure the spot shift (Δx com , Δy com ) j by this deformed wavefront from the collimator, deionized water and cover glass.
Let’s define the spot shift (Δx r , Δy r ) n as follows
Lager Image
The location (Δx r , Δy r ) n becomes the reference position of the S-H sensor in measuring the intraocular lens wavefront aberration.
Now the intraocular lens is immersed in deionized water in the intraocular lens holder, the focus of the intraocular lens is set on the focus of the objective lens, and then the spot shift (Δx total , Δy total ) k are measured by the S-H sensor.
Finally, the spot shift (Δx IOL , Δy IOL ) k by the wavefront deformation of the intraocular lens only are calculated as follows
Lager Image
The wavefront error map and spot displacement by intraocular lens only (500 times amplification).
Zernike standard coefficients of intraocular lens by S-H sensor
Lager Image
Zernike standard coefficients of intraocular lens by S-H sensor
Lager Image
The wavefront deformation by the intraocular lens only are calculated with Eq. (1), Eq. (2) and (Δx IOL , Δy IOL ) k and Fig. 4 shows the wavefront error map and spot shift (Δx IOL , Δy IOL ) k of the intraocular lens only, where the spot shift in Fig. 4 is the 500 times amplification of the displacement.
This experiment showed that the amount of deionized water had no effect on the wavefront aberration of the intraocular lens. With the intraocular lens in deionized water, the RMS WFE is 0.02λ in design while the RMS WFE is 0.047λ in measurement and Zernike standard coefficients of the intraocular lens are showed in Table 3 .
- 3.3. Measurement of the Effective Focal Length of the Intraocular Lens
As mentioned earlier, the optical characteristics of the intraocular lens are likely to change when it is inserted into deionized water after manufacturing. Thus, it is essential to measure EFL of the intraocular lens in liquid. This is because the most important optical property is the optical power of the intraocular lens when the intraocular lens is inserted into the eyes. Thus, whether the required optical power of the intraocular lens is appropriate is determined based on the comparison of EFL between the design and the measurement in liquid. This study introduces the easy way of measuring EFL, which is different from those using existing S-H sensors, and measures EFL of the intraocular lens by means of the introduced method. The S-H sensor is advantageous in that it can measure the location of an image point accurately. This is because the location of the image is found accurately by searching the proper position where the defocus coefficient among Zernike polynomial terms is minimized. Although it is possible to find the image position by means of the magnifying optical system and CCD instead of the S-H sensor, this study adopts the S-H sensor.
To measure EFL of the lens element, the measuring system as in Fig. 5 might be utilized.
It can be seen the relations as Eq. (6) and Eq. (7) from (b) and (c) in Fig. 5 and the lens equation.
Lager Image
Lager Image
From Eq. (6) and Eq. (7), f can be described as follows
Lager Image
Lager Image
Diagram on the EFL measuring principle.
where Δz 1 , Δz 2 , and Δz 2 ' become negative values when they move to the left, and positive when moving to the right, and f of the positive lens becomes positive value.
Eq. (8) shows that the EFL can be measured based on the only changes in location of the object and image.
To measure EFL, the pinhole is put at the focus (F 1 ) of a measuring lens as in Fig. 6 (a), and the S-H sensor at the back of the measuring lens. It is easy to find the focus by moving pinhole back and forth until defocus coefficient of Zernike polynomial terms becomes minimized.
The pinhole is relocated from F 1 to P 1 by Δz 1 , and the sensor unit to the right is relocated as well and the location of the sensor unit is where the defocus coefficient becomes minimum. In the same manner, the pinhole is relocated by Δz 2 , and then the sensor unit also is relocated by Δz 2 '.
EFL is calculated based on Eq. (8) by means of the resulting Δz 1 , Δz 2 , and Δz 2 '. To verify the accuracy of the EFL from Eq. (8) through the experiment, the curvature( C 1 , C 2 ) and thickness( t ) of five lenses manufactured by using high grade glass are measured, and then EFL is calculated based on Eq. (9) theoretically [19] .
Lager Image
The result was compared with that of the experiment result in the way stated in Fig. 6 with a He-Ne light source, unlike the case of the intraocular lens. As shown in Table 4 , the difference between the calculated value and measured one was less than 0.5%.
In the experiment, the size of the collimated input beam was adjusted to minimize the wavefront error as small as possible, and the beam expander was adopted when the beam projected into the S-H sensor was small.
To minimize the error in measuring EFL, the object is relocated many times while the location of the image is measured, then EFL will be chosen as the average of EFL
Lager Image
Scheme of device to measure EFL.
values calculated every time when the object was relocated.
Now EFL of the intraocular lens is measured by means of the method above. In the same way to measure wavefront errors, deionized water is put into the intraocular lens holder, the intraocular lens is put into it, and then Δz 1 , Δz 2 , and Δz 2 ' are measured in the way mentioned above to get the value of EFL. In measuring EFL of the intraocular lens, the quantity of deionized water and the cover glass of the intraocular lens holder do not affect EFL. Thus, measuring EFL of the intraocular lens as above is useful in that regard.
In the experiment with light source of 555 nm wavelength for the intraocular lens, the measured values are as follows: Δz 1 = -100, Δz 2 = -100, and z 2 ' = -14.44; thus, EFL = 53.7 mm.
Note that, 555 nm wavelength is used for the intraocular lens and He-Ne laser for others.
IV. MEASUREMENT OF THE INDEX OF REFRACTION OF AN UNKNOWN LIQUID, THAT OF A PLANO-CONVEX LENS, AND CURVATURE OF THE LENS
When a plano-convex lens, whose accurate index of refraction is known, is used, the index of refraction of an unknown liquid can be readily calculated by means of the EFL measuring method explained in Section 3.2.Conversely, when the index of refraction of the liquid is known, the curvature and index of refraction of a plano-convex lens can be calculated with measuring method of EFL.
Let’s consider a lens with the curvature C 1 and C 2 , the index of refraction n 0 and the thickness t. Let's make f 0 be the EFL when this lens is in the air and f the EFL when it is in a liquid whose index of refraction is n , then f 0 and f can be described as in Eq. (10) and Eq. (11) respectively.
Lager Image
Lager Image
To remove the dependence of t, the lens thickness, let’s consider a plano-convex lens.
In this case, EFL f and f 0 can be described as in Eq. (12) with C 2 = 0.
Lager Image
The index of refraction of an unknown liquid can be described as in Eq. (13) from Eq. (12).
Lager Image
Thus, on a plano-convex lens whose index of refraction( n 0 ) is known, the EFL f 0 in the air and EFL f in the unknown liquid are measured in the way explained in Section III.2, and then it is possible to calculate the index of refraction
Measurement result of EFL with He-Ne Laser. In this table, error (%) is calculated value-measured value)/calculated value *100
Lager Image
Measurement result of EFL with He-Ne Laser. In this table, error (%) is calculated value-measured value)/calculated value *100
of the unknown liquid with Eq. (13). Note that n in Eq. (13) is not in relation to the curvature and thickness of the lens, thus any kind of plano-convex lens may be used.
Using the lens with f 0 = 25.107 mm in Table 4 , f in deionized water is calculated as 91.16 mm based on the following measurements with He-Ne light source: Δz 1 = -100 mm, Δz 2 = -50 mm and Δz 2 ' = -27.7 mm.
With the index of refraction of the glass n 0 = 1.45702, f 0 = 25.107, f = 91.16, and based on Eq. (13), we can calculate that the index of refraction of deionized water is 1.331149.
The index of refraction of deionized water is 1.331747 at wavelength 0.6328μm, and thus the index of refraction of an unknown liquid may be measurable down to three places of decimals although there could be some variation depending on the measuring accuracy of EFL.
This way, the index of refraction n 0 and curvature C of the plano-convex lens is calculated with a liquid whose index of refraction is well known. n 0 and C from Eq. (12) can be described as in Eq. (14) and Eq. (15).
Lager Image
Lager Image
The accuracy of the index of refraction and curvature depends on the measuring accuracy of the image location.
V. CONCLUSION
As mentioned, an intraocular lens of hydrophilic materials and used in liquid is hard to measure by means of common lens testing methods. As emphasized above, to solve this problem, an intraocular lens should be tested in liquid. In this study, the transmission wavefront aberration of an intraocular lens was measured by means of the S-H sensor in consideration of the fact that the liquid is flat under gravity, and wavefront errors on the optical components other than the intraocular lens were removed easily. As for the intraocular lens, accurate measuring of EFL in addition to the transmission wavefront aberration is of great importance. The change in the image location as the object is relocated is measured by means of the S-H sensor, which indicates that EFL of intraocular lens or any lens is measurable. When the five sample lenses were used, it turned out that the error ratio of EFL was less than 0.5%. In addition, when a plano-convex lens, whose index of refraction was known, was used, EFL both in the air and in unknown liquid were measured in order to calculate the index of refraction of the unknown liquid. It is expected that this method could be utilized in measuring the index of refraction of unknown liquid in the future. Conversely, if the index of refraction of the liquid is known, the index of refraction and curvature of the plano-convex could be calculated. By means of a plano-convex lens with any thickness and curvature on a certain glass, the index of refraction of the glass could be measured in the way stated above. Note that this paper shows a very simple and new method with relatively high accuracy compared to the conventional methods to measure wavefront aberration and effective focal length.
References
Schwiegerling J. , DeHoog E. (2010) “Problems testing diffractive intraocular lenses with Shack-Hartmann sensors” Appl. Opt. 49 62 - 68
Zhou C. , Wang W. , Yang K. , Chai X. , Ren Q. (2008) “Measurement and comparison of the optical performance of an ophthalmic lens based on a Hartmann-Shack wavefront sensor in real viewing conditions” Appl. Opt. 47 6434 - 6441
Jeong T. M. , Yoon G. (2006) “Customized correction of wavefront aberrations in abnormal human eyes by using a phase plate and a customized contact lens” J. Korean Phys. Soc. 49 121 - 125
Ko D. S. , Lee B. H. (2006) “Optics of refractometers for refractive power measurement of the human eye” J. Opt. Soc. Korea 10 145 - 156
Moreno-Barriuso E. , Navarro R. (2000) “Laser ray tracing versus Hartmann-Shack sensor for measuring optical aberrations in the human eye” J. Opt. Soc. Am. A 17 974 - 985
Kelly T. , Veitch P. J. , Brooks A. F. , Munch J. (2007) “Accurate and precise optical testing with a differential Hartmann wavefront sensor” Appl. Opt. 46 861 - 866
Diaz-Uribe R. , Pedraza-Contreras J. , Cardona-Nunez O. , Cordero-Davila A. , Cornejo-Rodriguez A. (1986) “Cylindrical lenses: testing and radius of curvature measurement” Appl. Opt. 25 1707 - 1709
Nyyssonen D. , Jerke J. M. (1973) “Lens testing with a simple wavefront shearing interferometer” Appl. Opt. 12 2061 - 2070
Bernardo L. M. , Soares O. D. D. (1988) “Evaluation of the focal distance of a lens by Talbot interferometry” Appl. Opt. 27 296 - 301
Neal D. R. , Copland R. J. , Neal D. A. , Topa D. M. , Riera P. (2004) “Measurement of lens focal length using multi-curvature analysis of Shack-Hartmann wavefront data” Proc. SPIE 5523 243 - 256
Kumar Y. P. , Chatterjee S. (2009) “Technique for the focal length measurement of positive lenses using Fizeau interferometry” Appl. Opt. 48 730 - 736
Matsuda K. , Barnes T. H. , Oreb B. F. , Sheppard C. J. R. (1999) “Focal-length measurement by multiple-beam shearing interferometry” Appl. Opt. 38 3542 - 3548
Watkins R. (2007) Zemax Models of Human Eye http://www.radiantzemax.com/kb-en/Knowledgebase/Zemax-Models-of-the-Human-Eye
Lane R. G. , Tallon M. (1992) “Wave-front reconstruction using a Shack-Hartmann sensor” Appl. Opt. 31 6902 - 6908
Park S. K. , Baik S. H. , Seo Y. S. , Kim C. J. , Ra S. W. (2003) “Wavefront measuring algorithm with improved measurement resolution using a Shack-Hartmann sensor” J. Korean Phys. Soc. 42 743 - 750
Topa D. M. (2002) “Wavefront reconstruction for the Shack-Hartmann wavefront sensor” Proc. SPIE 4769 101 - 116
Malacara D. 2007 Optical Shop Testing 3rd ed. A John Wiley & Sons, Inc. NJ, USA
Born M. , Wolf E. 1999 Principles of Optics 7th ed. Cambridge University Press NY, USA
Hecht E. 2001 Optics 4th ed. Addison-Wesley NY, USA