Journal of China University of Science and Technology Vol.50-2012.01 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia 應用於近視性老花眼的多焦點硬式隱形眼鏡設計 洪嘉聰 Chia-Tsung Hung 1 2 李世文 Der-Chin Chen 3 Shih-Wen Lee 逢甲大學電機工程系副教授 中華科技大學電機工程系助理教授 1,2Department 3Department 陳德請 逢甲大學電機工程系碩士班研究生 2 3 1 of Electrical Engineering, Feng Chia University of Electrical Engineering, China University of Science and Technology ABSTRACT The purpose of this study is to design the progressive addition hard contact lens for myopic presbyopia patients by using the multi-configuration function in ZEMAX optical design program. The multi-configuration settings consist of four ranges, which are infinity, 2000mm, 1000mm and 400mm. So, the myopic presbyopia patients are able to see clearly under the four different fields of view after wearing progressive addition hard contact lens. Using the methods of multi-configuration and the free form surface; it could correct the -3.00D at the infinity and -1.0D at the near vision of myopia presbyopia, and the Modulation Transfer Function (MTF) value can reach above 0.3 at 30lp/mm. And super progressive addition hard contact lenses are designed. Key Word: Progressive Lens, Myopic presbyopia, Freeform 摘 要 本文研究目的係使用自由曲面最佳化設計一近視性老花眼硬式隱形眼鏡。研 究方法係採用 ZEMAX 光學設計程式的多重組態對無限遠、2000mm、1000mm、 400mm,4 種視場(View Field)進行設計,使近視性老花眼在配戴硬式隱形眼鏡後後 也適合看遠、中、近距離。除了可矯正近視 Myopia(-3.00D)之外,還可以使配戴近 視性老花眼硬式隱形眼鏡之後的視網膜解像率在 30 lp/mm 的 MTF 值達 0.3 以上。 61 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia 關鍵字:漸進鏡片、近視性老花、自由曲面 I. INTRODUCTION The crystalline lens in the eye structure looks like camera’s zoom lens, as shown in Fig.1. The accommodation whereby changes in the dioptric power of the crystalline lens occur so that an in-focus retinal image of an object of regard is obtained and maintained at the high resolution fovea for seeing near or far. From far to near is called positive accommodation, otherwise is called negative accommodation. Donders, Duane and Hofstetter has been successively in 1864, 1912 and 1947 to do the test that range of amplitude of accommodation for different age as shown in Table 1 [1-5] . The results for the age of 35 to 40 amplitude of accommodation over the age of amplitude of accommodation is remaining half of the age of 10, 70 at the age of accommodative power are almost zero. Three scholars chart changes in the statistics is not much difference, adjust the rate of Amplitude of Accommodation for poor people, prolonged close work on the eyes is a burden. We had published about the design of astigmatic eyeglass lenses by ZEMAX optical software in the previous issue of this journal [6]. The designing result of 1.0D astigmatic lens can obviously correct astigmatism and the MTF is more than 0.3 at 30 lp/mm. This paper studies the design of progressive addition hard contact lens. The difference of two researches is: the former is to correct astigmatic eye and the latter is to correct myopic presbyopia eye. 62 Journal of China University of Science and Technology Vol.50-2012.01 Fig.1 the structure of the eye 63 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia II. Amplitude of Accommodation with the Range of Clear Vision The amplitude of accommodation, expressed in diopters, is difference between the far point and the near point of accommodation with respect to the spectacle plane, the entrance pupil or some other reference point of the eye. The closest points conjugate to the retina with exertion of maximal accommodation. Table 1 Change the value of accommodate Ages 10 15 20 25 30 35 40 45 50 Donders 14 12 10 8.5 7 5.5 4.5 3.5 2.5 1.75 13.4 12.6 11.5 10.2 8 7.3 5.9 3.7 2 1.3 1.1 1.1 0 9.5 8 6.5 5 3.5 2 0.5 0.5 0 Duane(mean) 55 60 65 70 1 0.5 0.25 Hofstetter (probable) 15.5 14 12.5 11 @unit:diopter Maximum amount of accommodation represented in space is called near point of accommodation. The farthest point conjugates to the retina with exertion of minimum accommodation. Minimum amount of accommodation represented in space is called far point of accommodation. The equation of amplitude of accommodation is: AA=(1/ MrS) –(1/ MpS) (1) where AA is amplitude of accommodation, MrS the linear distance of far point of accommodation to spectacle plane and MpS is the linear distance near point of accommodation to spectacle plane. James Ware was the first person in the 19th century to understand that far sight was not necessarily associated with presbyopia as shown in Fig.2 . In 1855, Stellwag von Carion provided a relatively clear description with an optical explanation of the differences between hyperopia and presbyopia. We focused on 40 to 60 years (every 5 years), respectively, hyperopia +3.00 D ~ myopia-3.00D of the people to do the analysis clear horizon, as listed in Table 2. By the formula (1): amplitude of accommodation formula can change into: MpS= MrS/(1-AA* MrS), MrS≠0 or MpS=((1/ MrS)-AA)-1 and when MrS=0, MrS=(-AA) (2) (3) -1 (4) The AA value use data of Donders’s in Table 2. 64 Journal of China University of Science and Technology Vol.50-2012.01 III. The Optical Model of Human Eye In the book of Introduction to Optics, Frank L. Pedrotti, Leno M. Pedrotti, Leno S. Pedrotti mentioned the symbols and optical data of model eye in Table 3[7]. The optical layout of model eye optics is defined more or less differently as illustrated in Fig. 3.The model eye’s parameter in ZEMAX Software in as Fig.4 shows. Table 1 The Range of Clear Vision Ametropia +3.00D +2.00D +4.5D) 45 years IBE (+3.5D) 33.3 200 50 years IBE (+2.5D) IBE 33.3 80 60 years IBE (+1D) IBE 33.3 200 55 years IBE (+1.75D) IFE IBE 33.3 50 IFE IFE IFE 40 100 28.6 ∞ 22.2 100 18.2 50 15.4 33.3 13.3 IBE IFE IBE IFE IFE IFE IFE IFE 50 66.7 100 40 ∞ 28.6 100 22.2 50 18.2 33.3 15.4 IBE IFE IBE IFE IFE IFE IFE IFE IFE 50 200 100 66.7 ∞ 40 100 28.6 50 22.2 33.3 18.2 IBE IBE IBE IFE IFE IFE IFE IFE IFE 50 400 100 133 ∞ 57.1 100 36.4 50 26.7 33.3 21.1 IBE IBE IBE IFE IFE IFE IFE IFE IFE IFE 50 100 100 ∞ ∞ 100 100 50 50 33.3 33.3 25 IFE IFE IFE IFE F.P.=Far Point; N.P.=Near Point; I.F.E.=in front of eye; I.B.E.=in back of eye 65 IFE N.P. IBE IFE IFE N.P. F.P. IFE 33.3 66.7 50 IFE N.P. F.P. -3.00D (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) (㎝) IFE N.P. F.P. -2.00D (Acc.) IBE N.P. F.P. -1.00D F.P. IFE N.P. F.P. 0.00 Ages 40years( IBE N.P. F.P. +1.00D IFE IFE IFE IFE IFE IFE IFE IFE IFE Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia Fig.2 The range of clear vision with accommodation Table 3 optical data of eye model Optical surface Difining Distance from corneal Radius of curvature Refractive Refractive power or element Symbol vertex(㎜) of surface(㎜) index Cornea S1 — +8a — 41.6 Lens(unit) L — 1.45 30.5 Front surface S2 +3.6 +10b — 12.3 Back surface S3 +7.2 -6 — 20.5 Eye(unit) — — — — 66.6 Front focal plane F -13.04 — — — Back focal plane F' +22.38 — — — plane H +1.96 — — — Back principal plane H' +2.38 — — — Front nodal plane N +6.69 — — — Back nodal plane N' +7.38 — — — Anterior chamber AC — — 1.333 — Vitreous chamber VC — — 1.333 — Entrance pupil EnP +3.04 — — — Exit pupil ExP +3.72 — — — (diopter) Front principal 66 Journal of China University of Science and Technology Vol.50-2012.01 a:The cornea is assumed to be thin. b:Value is given for the relaxed eye. For the tensed or fully accommodated eye, the radius of curvature of the front surface is changed to +6mm. reference : adapted with permission from Mathew Alpern,”The Eyes and Vision,”Table1,Section 12, in Handbook of Optics (New York: McGraw-Hill Book Company,1978) Fig. 2 optical layout of eye model Fig. 3 The optical data of eye model in ZEMAX optical design software We simulate four visual ranges, for example: extra far distance (∞), the far distance (2000 mm), middle range (1000 mm) and near (400 mm), so need to use the multi-configuration. In Fig. 4, THIC in configuration 1 to configuration 4 that represent for distance at (∞), 2000 mm, 1000 mm, 400 mm; CRVT on behalf of lens curvature change; PRAM on behalf of the relative angle that between visual axis of the eyeball and central axis of the contact lens. 67 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia The solution to optimize the ophthalmic lens is to change the surface type of CL-front from sphere to free-form surface for giving more freedom of design. Polynomial expansion of free-form surface as in formula (5) shows, k of the Polynomial expansion will affect the contact lens to make distorted and the curvature of the distribution. Fig. 4 setting multi-configuration in ZEMAX optical design software (5) Where N is the total number of series in the polynomial coefficients, Ai for the first item expansion coefficients of the polynomial i, c for the curvature, r is radius, k coefficient for the quadratic surface. Quadratic surface which is less than -1 for the hyperbolic plane coefficient, equal to 1 for the parabolic in an ellipse between -1 and 0, equal to 0 for the sphere. IV. Result and Analysis This research is to design the progressive addition hard contact lens to correct the -3.00D far sight and -1.00D near sight myopia, the procedures are as followings: 4.1 Set up the three-dimensional layout (3D Layout) Fig.6 is a three-dimensional setting layout. First surface represent for the incident beam entering and the last surface on behalf of the retina for image plane. The other set are default value. The first surface is the object plane, if the object distance is infinity setting for the graph is blank. Fig.7 shows the eye of four configurations (from input beam to retina). 68 Journal of China University of Science and Technology Vol.50-2012.01 Fig.6 3D layout diagram setting 1 Fig.7 3D eye layout (four configurations) For understanding the relative included angle between the visual axis of eye and the central axis of contact lens, we can change the output settings of three-dimensional eye layout. Figure 8 shows the eye of four configurations (from CL-front to LENS-BACK). The 3D map of the four configurations shows in figure 9, 10, 11 and 12. 69 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia Fig.8 3D layout diagram setting 2 Fig.9 3D layout configuration 1(infinity) Fig.10 3D layout configuration 2(2000mm) Fig.11 3D layout configuration 3(1000mm) Fig.12 3D layout configuration 4(400mm) 4.2 Setting Modulation Transfer Function (MTF) Modulation Transfer Function (MTF) is an important method of describing the performance of an optical system, and describes the contrast in the image of a spatial frequency presented in the scene being viewed. The maximum spatial frequency of modulation transfer function set in30 lp 70 Journal of China University of Science and Technology Vol.50-2012.01 / mm for meeting the human eye of need. Figure 13 shows the fast Fourier transform MTF icon and the modulation transfer function setting of system. The MTF of the four configurations shows in figure 14, 15, 16 and17. Fig.13 Setting Modulation Transfer Function Fig.14 MTF configuration 1(Infinity) Fig.15 MTF configuration 2 (2000mm) Fig.16 MTF configuration 3(1000mm) Fig.17 MTF configuration 4(400mm) 71 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia The MTF plot for this eye glass, above, shows the contrast ratio for any spatial frequency up to the maximum that the eye glass can support. In this case, we choose to limit the spatial frequencies shown to a maximum of 30 cycles/mm. Also shown for reference is the diffraction limited performance of an aberration-free lens of the same f/# [8]. 4.3 Setting Partially Coherent Image Analysis Partially Coherent Image Analysis can be performed by using the incoherent of transfer functions and simulates the actual visual image. When generating diffraction images using incoherent transfer functions, diffraction effects are accounted for, however, each point on the source is considered to be incoherent with respect to all other points. The partially coherent transfer functions are characterized using a parametric function, Gamma. The Gamma function utilized for a particular analysis can be one of two types, Gaussian or Sinc (although others can be added upon request): γ(r)= e α2) andγ(r)=Sinc(x/α)*Sinc(y/α).For the Gaussian (-r*r/ Gamma function, the position vector, r, represents the distance between two points in the displayed image. For both functions, the parameter α is a scaling parameter defined in lens units. This parameter sets the effective width of the Gamma function. Use mostly incoherent method when α is small and γis narrow. First, let us try a small α value (i.e. 0.025). We know that for small α values, the resulting Gamma function is narrow and, as such, the results are mostly incoherent. The narrower the Gamma function, the more incoherent the resulting image will appear. Figure 18 show partially coherent image analysis settings. Figure 14, 15, 16 and 17 show the image analysis of the four configurations. Fig.18 Setting Partially Coherent Image Analysis 72 Journal of China University of Science and Technology Vol.50-2012.01 Fig.19 PCIA configuration 1(Infinity) Fig.21 PCIA configuration 3(1000mm) Fig.20 PCIA configuration 2(2000mm) Fig.22 PCIA configuration 4(400mm) Notice that the resulting image shows the general blurring expected (as a result of diffraction) in configuration 3 and 4. It is important to note that the image must be sufficiently sampled to generate accurate partial coherence results. Not all light sources are perfectly incoherent or perfectly coherent. Some light sources lie somewhere in the middle and, thus, are partially coherent. The degree of partial coherence is specified by a Gaussian or Sinc Gamma function. 4.4 Setting Power Field Map The sag of progressive hard contact lens surface is very complex. Set to show contours at an interval of 0.25 diopters, we can see the spherical and cylindrical power added by this surface over the all field of view. This feature computes optical power or focal length as a function of field coordinate. The method used is to trace a ring of real rays around the entrance 73 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia pupil at each point in the field. Figure 23 is partially coherent image analysis settings. Figure 24, 25, 26 and 27 shows the enlarged map of Power Field Map of four configurations. Fig.23 Setting Power Field Map Fig.24 PFM configuration 1 (Infinity) Fig.26 Fig.25 PFM configuration2 (2000 mm) PFM configuration 3(1000 mm) Fig.27 PFM configuration4 (400 mm) The feature of PFM can display x or y direction optical power, maximum and minimum power and spherical power. 74 Journal of China University of Science and Technology Vol.50-2012.01 4.5 Result After designed, the myopic presbyopia eye was corrected by progressive addition hard contact lens. Fig.28 shows the lens data of progressive addition hard contact lens (from surface 2 to surface 3), and Fig. 29, Fig.30, Fig.31 and Fig. 32 shows the MTF value after designed at four visions respectively. The progressive addition hard contact lens can correct myopic presbyopia and the average of MTF is over than 0.6 at 30 lp/mm spatial frequency. In Fig.29, Fig.30, Fig.31 and Fig.32, the MTF of tangential plane is superior to the MTF of saggital plane, because the tangential plane of toroidal surface uses the asphereic surface. The near vision has blur spot produced by defocusing at about 30 lp/mm spatial frequency so the MTFS is bad as shown in Fig32. The total MTF is in excess of 0.6 so it still fit performance requirement of vision. Fig. 28 the design result of progressive addition hard contact lens Fig. 29 The MTF at the far vision (infinite) Fig. 30 The MTF at the middle vision (200 mm) 75 Design the Progressive Addition Hard Contact Lens for Myopic Presbyopia Fig.31 The MTF at the middle vision (100mm) Fig. 32 The MTF at the near vision (40mm) The design result is satisfied with the following two specifications of the myopia presbyopia: -3.00 Diopters at the far (infinite) vision and -1.00 Diopters at the near vision. The MTF is an important parameter in optical system design. When optimizing on MTF, only the spatial frequency of interest is computed, this is much faster and requires far fewer rays for a given level of precision. For conventional eyeglass with large aberrations the Geometric MTF computes an approximate MTF with great speed. It is a good chose for "roughing in" a design for best MTF as fast as one can optimize RMS spot radius. Above method is used, MTF approaches diffraction-limited performance as RMS wave front error goes to zero. Therefore, initial optimization using the default RMS Wave front merit function is highly recommended. Also, do not start to optimize on MTF until all the desired spatial frequencies are within the first minimum of the MFT plot [8]. V. Conclusion From the result at section IV, we can summarize the system design of progressive addition hard contact lens. First, test the diopter of the myopic presbyopia eye. Secondly, choose the suitable diopter of the eyeglass, and it shows the diopter of the eyeglass is weaker than the expected. Designed the spheric surface to free-form aspheric, we can get a more suitable eyeglass to prevent to further degrade the myopic presbyopia eye. In this study, we also find the optical simulation code can be a tool to aid to predetermine the choosing a suitable diopter of the eyeglass. And we hope to corporate with eye clinical to construct the data base to verify the validity of weaker eyeglass for myopic presbyopia eye. We can offer innovative design method to correct myopic presbyopia eye. Based on your statement of myopic presbyopia eye, we 76 Journal of China University of Science and Technology Vol.50-2012.01 develop a solution that meets form, fit, and function specifications while satisfying your visual defect requirement. VI. Reference [1] Willian Andrew Keirl and Caroline Christie, “Clinical Optics and Refraction: A Guide for Optometrists, Contact Lens Opticians and Dispensing Opticians” Baillière Tindall Elsevier/Butterworth-Heinemann, chapter 13.pp.132-152, 2007. [2] Yung-Feng Shih, Luke L-K Lin and Por-Tying Hung, “Studies of Ocular Biometry in Taiwan”, Journal of Medical Ultrasound, Volume 15, Issue 1, pp.9-18, 2007. [3] Frank L. Pedrotti, Leno M. Pedrotti and Leno S. Pedrotti, “Introduction to optics,” Pearson Prentice Hall, chapter 19, pp.419-437, 2007. [4] DarryI J Meister and Scott W Fisher, “Progress in the spectacle correction of presbyopia. Part 2: Modern progressive lens technologies”, Clin. and Exp. Optom. , Vol.91, No.3, pp.251-264, May, 2008. [5] James E. Sheedy, Raymond F. Hardy, “The optics of occupational progressive lenses”, Journal of Optometry, Vol. 76, Vol. 8, August, 2005. [6] Der-Chin Chen, Shang-Wei Hsieh and Shih-Wen Lee, “ The Design of Astigmatic Lenses by ZEMAX Optical Software”, Journal of China University of Science and Technology,Vol.46, pp.77-86 ,April ,2011. [7] Frank L. Pedrotti, S.J., Leno M. Pedrotti and Leno S. Pedrotti, “Introduction to Optics”, chapter 19, pp.433-434, 2007. [8] http://www.zemax.com/kb/articles/187/1/How-to-Optimize-on-MTF/Page1.html. 77