WO2019205107A1 - Vr technology-based method for optometry and simulation - Google Patents

Vr technology-based method for optometry and simulation Download PDF

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Publication number
WO2019205107A1
WO2019205107A1 PCT/CN2018/084922 CN2018084922W WO2019205107A1 WO 2019205107 A1 WO2019205107 A1 WO 2019205107A1 CN 2018084922 W CN2018084922 W CN 2018084922W WO 2019205107 A1 WO2019205107 A1 WO 2019205107A1
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lens
optometry
parameters
space
transfer function
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PCT/CN2018/084922
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French (fr)
Chinese (zh)
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方绚莱
普拉莫·威廉
冯玉林
张志飞
贺晓宁
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深圳摩方材料科技有限公司
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Priority to PCT/CN2018/084922 priority Critical patent/WO2019205107A1/en
Publication of WO2019205107A1 publication Critical patent/WO2019205107A1/en

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    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B3/00Apparatus for testing the eyes; Instruments for examining the eyes
    • A61B3/02Subjective types, i.e. testing apparatus requiring the active assistance of the patient
    • A61B3/028Subjective types, i.e. testing apparatus requiring the active assistance of the patient for testing visual acuity; for determination of refraction, e.g. phoropters
    • GPHYSICS
    • G02OPTICS
    • G02BOPTICAL ELEMENTS, SYSTEMS OR APPARATUS
    • G02B27/00Optical systems or apparatus not provided for by any of the groups G02B1/00 - G02B26/00, G02B30/00
    • G02B27/01Head-up displays
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F17/00Digital computing or data processing equipment or methods, specially adapted for specific functions
    • G06F17/10Complex mathematical operations
    • G06F17/16Matrix or vector computation, e.g. matrix-matrix or matrix-vector multiplication, matrix factorization

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  • the invention relates to the field of optometry technology, in particular to an optometry and simulation method based on VR technology. Background technique
  • the design of glasses including glasses, reading glasses, astigmatism and other glasses, is generally designed to wear the a priori light of the demander, and then based on the prescription of the optometry results.
  • the prescriptions obtained by the current optometry system generally include degrees and astigmatism. , the axial position, the prism degree and other optimal imaging parameters of various lenses.
  • the human eye looks at the instrument in front, and the eyeball is only at a certain rotation angle (ie, a specific field of view), so the data obtained by such optometry is only a parameter of a certain angle.
  • the prescription of the obtained glasses cannot guide the use under the large field of view. That is to say, this optometry method cannot comprehensively consider the imaging effect of the spectacle lens in different direction of the field of view (ie, the different angle conditions of the eyeball rotation), that is, the picture of the entire format that the actual eye needs to see cannot be prescribed by the spectacle lens. The way is expressed.
  • the spectacle lens produced according to the prescription obtained by the conventional optometry can only exhibit the best imaging effect when the eyeball of the human eye is just at the above specific rotation angle.
  • the imaging effect of the spectacle lens must be different or The effect is very poor, but in actual use, the rotation of the human eye is randomly occurring. Therefore, the ophthalmic lens produced by the conventional optometry method cannot fully meet the actual needs.
  • the method also proposes that during the optometry process, the user can communicate and feedback with the VR system through the body or language to adjust the sharpness of the image.
  • An object of the present invention is to overcome the above disadvantages and to provide an optometry and simulation method based on VR technology which takes the rotation of the human eye into consideration during the optometry process.
  • An optometry and simulation method based on VR technology comprising the following steps:
  • the first step simulating the direction of the optical axis in the VR system Z, the object to be observed;
  • a lens is simulated in the VR system, and the lens is placed in the direction of the optical axis and placed between the human eye and the observed object, and the human eye observes the observed object through the lens;
  • the third step for the same imaging point of the observed object, define various possible different field of view directions g in a vector space K, and define a specific field of view g in the conventional optometry in another vector space K' in;
  • various parameters of the specific field of view g are converted into parameters of the K space by the mapping matrix, thereby obtaining optimal imaging parameters of the lens including various different fields of view.
  • the direction of the rotation of a certain eyeball, g (a, b) vector direction can be perfect imaging, in this vector direction g (a, b), the light energy captured by the human eye is l (a, b, A ) , where A is the wavelength; in the K space, the light energy captured by the human eye in the vector direction g(as, bs) is l(as, bs, A ), according to the above mapping matrix T: K' K, defines the mapping matrix G of two spatial K and K' light energy: l(a, b, in) - l(as, bs, A), and calculates the optimal imaging effect parameters of the lens according to the following formula:
  • Calculating the final point transfer function according to the above formula for calculating the final point transfer function includes the following steps:
  • the VR-based optometry and simulation method further includes a lens verification method, and the lens verification method includes the following steps:
  • the VR system adjusts the simulated lens according to the optimal imaging parameters of the lens obtained in the above steps _ to 5 to form a new lens, and the parameters of the new lens completely conform to the Optimal imaging parameters of the lens;
  • Step 2 Simulate the human eye to observe the observed object through the new lens, and during the observation process, the eyeball is rotated by different angles to verify the imaging effect of the new lens.
  • the invention has the beneficial effects that: the invention uses the VR technology to simulate and design the lens, and simulates the human eye to observe the object to be observed through the lens, and passes various parameters in a specific field of view direction in the traditional actual optometry through the mapping matrix. Converting to optimal lens imaging parameters including various fields of view; that is, the present invention considers different directions of eye rotation in the optometry process, thereby producing optimal lens parameters obtained according to the optometry and simulation methods of the present invention.
  • the lens can fully meet the needs of different directions of eyeball rotation in actual use, that is, when the wearer's eyeball rotates to the direction of the field of view of the lens edge, the imaging effect of the lens is also very good, only small astigmatism, chromatic aberration, distortion will appear. That is to say, the present invention combines optometry and simulation with VR technology, thereby providing a complete solution for high-precision optometry and vision correction, and solving the problem of optometry in a single field of view in the prior art.
  • 1 is a flow chart of a method for optometry and simulation of the present invention
  • FIG. 2 is a schematic view of a g-direction of a g-direction of the eyeball in the method of the present invention
  • Figure 3 is a schematic view showing the direction of rotation of the eyeball in two different spaces of K and K' in the method of the present invention
  • 4 is a schematic diagram of a three-dimensional display model of the progressive multifocal lens curvature in the method of the present invention
  • FIG. 5 is a schematic diagram showing the curvature of the progressive multifocal lens in the method of the present invention.
  • the optometry and simulation method based on the VR technology of the present invention comprises the following steps: Step 1: Simulate the optical axis direction Z in the VR system, the observed object;
  • the second step emulating a lens in the VR system, placing the lens in the direction of the optical axis and positioning it between the human eye and the object to be observed, and the human eye observing the observed object through the lens;
  • the third step for the same imaging point of the observed object, define various possible different field of view directions g in a vector space K, and define a specific field of view g in the conventional optometry in another vector space K' in;
  • various parameters of the specific field of view g are converted into parameters of the K space by the mapping matrix, thereby obtaining optimal imaging parameters of the lens including various different fields of view.
  • the projection component of the vector g(a, b) in the YOZ plane is g y
  • the projection component in the XOZ plane is g x
  • the angle in the g ⁇ Z direction is a
  • the angle between the g x Z direction is b
  • the direction of the optical axis is defined as the Z direction
  • the human eye is at the position of the 0 point.
  • the human eye observes the observed object through the lens, and the optical axis is in the z direction.
  • the direction of the field of view is g.
  • the point A can be clearly observed through the glasses.
  • g B the point B can be clearly observed through the glasses, and
  • g A and g B are specific directions, which are defined in the above vector space K'.
  • the vector space K there are any more directions to observe the point A on the object, such as the g AS direction.
  • the imaging effects of the glasses are evaluated only in the K' space.
  • the present invention is to convert various parameters of the specific field of view direction g into parameters of the K space through the mapping matrix, that is, to convert the parameters of the K' space into the parameters of the K space through the mapping matrix T, that is, Better imaging conditions in a single field of view translate into better imaging conditions across multiple fields of view.
  • the mapping matrix can reflect how the original imaging quality (astigmatism, chromatic aberration, distortion, etc.) of the lens decreases under the condition of the eyeball rotation.
  • the mapping matrix T: K' K is understood to be T: (a, b) (as, bs).
  • a certain _ eyeball rotation direction, g (a, b) vector direction can be perfect imaging, or in the traditional optometry mode, the wearer of the glasses is The direction can clearly observe the object to be observed, that is, the lens corrects the astigmatism, chromatic aberration, distortion, etc. to a reasonable range.
  • the light energy captured by the human eye is l(a, b, A), where A is the wavelength; in the K space, the human eye is in the vector direction g(as, bs)
  • the captured light energy is l(as, bs, A)
  • the mapping matrix G of the light energy is defined: l(a, b, in) - l(as, bs, A ), and calculate the optimal imaging effect parameters of the lens according to the following formula:
  • the final point transfer function includes the optimal imaging effect parameters of the lens, and the point transfer function can be understood as an associated relation function of different monochrome images. It can be seen from the above calculation formula that in the K space, the light energy l(as, bs, A) captured by the human eye is equal to the integral of l(a, b, in) and the point transfer function /, . The above calculation formula is used in the vector space.
  • the step mapping matrix G is l(a j , b j , A) l(aS j , bS j , A) , that is, the parameters of the K′ space are converted into the K space, the steps (1) and (2) Then it is the parameter of the known K space, and then the parameters in the K' space are pushed backwards.
  • the F light is cyan, the wavelength is 486 nm, the D light is yellow light, the wavelength is 589 nm, the C light is red light, and the wavelength is 656 nm.
  • the point transfer function calculated in steps (2) and (4) is a monochromatic light condition, and the final point transfer function f is the final result considering different wavelengths.
  • the present invention considers the rotation of the eyeball in the process of optometry, and converts various parameters in a specific field of view direction of the conventional actual optometry into a matrix containing various fields of view.
  • the lens imaging parameters that is, the conditions for clear imaging of large-format images in different fields of view will be given, thereby solving the problem of optometry in the single field of view in the prior art.
  • the progressive multifocal lens has a constant radius of curvature on one side of the lens, that is, the eyeball is in different directions of rotation, and the degree of the glasses is different.
  • the spline curve Different radii of curvature are shown, and the relative magnitude of the radius of curvature is determined by the relative length of the indicator line.
  • the degrees of the lenses are different in different fields of view, and if the conventional optometry method is used, more errors will be generated, and the present invention is utilized.
  • the optometry and simulation methods provided can effectively reduce the error and improve the optometry precision of such lenses.
  • a progressive multifocal presbyopic lens Take a progressive multifocal presbyopic lens as an example, that is, if the wearer needs a view Near-field +5.0D reading glasses, at the same time there are other degrees in the far-distance area, there is a transition zone between the near-field and the far-field, and the peripheral area of the glasses.
  • conventional optometry such optometry is performed.
  • the accuracy is required to be accurately matched with the optometry, the error is large; and the +5.0D reading glasses produced by the optimal lens imaging parameters obtained by the method of the present invention are 40 cm away from the glasses, the wearer After the eyeball rotates 35 degrees, the effect of the field of view is observed.
  • the reading lens distortion is less than 2%, the astigmatism in the meridional and sagittal directions is less than 0.03D, and the optometry precision is very high.
  • the optometry and simulation method based on the VR technology of the present invention further comprises a lens verification method, and the lens verification method comprises the following steps:
  • the VR system adjusts the lens designed by the simulation according to the optimal imaging parameters of the lens obtained in the above steps _ to 5 to form a new lens, and the parameters of the new lens completely conform to the Optimal imaging parameters of the lens;
  • Step 2 Simulate the human eye to observe the observed object through the new lens, and during the observation process, the eyeball is rotated by different angles to verify the imaging effect of the new lens, such as astigmatism, chromatic aberration, distortion and the like.
  • the effectiveness of the optimal imaging parameters of the lens obtained by the optometry and simulation methods of the present invention can be further ensured by the lens verification method.

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Abstract

A VR technology-based method for optometry and simulation, which comprises the following steps: for the same imaging point of an observed object, defining various possible different field of view directions g in one vector space K, and defining a specific field of view direction g in conventional optometry in another vector space K'; defining a mapping matrix T of the two spaces: K'→K; converting various parameters of the specific field of view direction g into parameters of the K space by means of the mapping matrix, thereby obtaining the optimal imaging parameters of a lens comprising the various different field of view directions; the lens made according to the optimal imaging parameters of the lens may meet actual usage requirements; even if the eyeball of a wearer turns to the field of view direction at an edge of the lens, the imaging effect of the lens is still very good.

Description

一种基于 VR技术的验光及仿真方法 技术领域  An optometry and simulation method based on VR technology
本发明涉及验光技术领域,尤其涉及一种基于 VR技术的验光及仿真方法。 背景技术  The invention relates to the field of optometry technology, in particular to an optometry and simulation method based on VR technology. Background technique
目前对于眼镜的设计,包括近视眼镜、 老花镜、 散光等眼镜的设计, 一般 是佩戴需求者先验光,然后根据验光结果得出的处方进行设计, 目前的验光系 统得到的处方一般包括度数、 散光、 轴位、 棱镜度数等各种镜片最佳成像参数。  At present, the design of glasses, including glasses, reading glasses, astigmatism and other glasses, is generally designed to wear the a priori light of the demander, and then based on the prescription of the optometry results. The prescriptions obtained by the current optometry system generally include degrees and astigmatism. , the axial position, the prism degree and other optimal imaging parameters of various lenses.
但是常规的验光过程中 ,人眼注视在前方的仪器,眼球只是在某一个特定 转动角度(即特定视场方向),所以这种验光得到的数据只是某一个特定的角度 的参数,这种方式得到的眼镜处方无法对大视场下的使用产生指导意义。 也就 是说这种验光方法无法将不同的视场方向下(即眼球转动的不同角度条件)眼 镜片的成像效果综合考虑,即无法将实际眼睛需要看到的整个幅面的图片以眼 镜片处方的方式表现出来。 根据常规验光得到的处方制作出的眼镜片只能在人 眼眼球刚好处于上述特定转动角度时能表现出最佳的成像效果,若佩戴者人眼 眼球转动了 ,眼镜片的成像效果必然不同或者成效效果很差,但是在实际使用 过程中 ,人眼眼球的转动是随机发生的。 所以通过常规验光方法而后制作出的 眼镜片并不能完全满足实际需要。  However, in the conventional optometry process, the human eye looks at the instrument in front, and the eyeball is only at a certain rotation angle (ie, a specific field of view), so the data obtained by such optometry is only a parameter of a certain angle. The prescription of the obtained glasses cannot guide the use under the large field of view. That is to say, this optometry method cannot comprehensively consider the imaging effect of the spectacle lens in different direction of the field of view (ie, the different angle conditions of the eyeball rotation), that is, the picture of the entire format that the actual eye needs to see cannot be prescribed by the spectacle lens. The way is expressed. The spectacle lens produced according to the prescription obtained by the conventional optometry can only exhibit the best imaging effect when the eyeball of the human eye is just at the above specific rotation angle. If the wearer's eyeball rotates, the imaging effect of the spectacle lens must be different or The effect is very poor, but in actual use, the rotation of the human eye is randomly occurring. Therefore, the ophthalmic lens produced by the conventional optometry method cannot fully meet the actual needs.
而也有些验光用到了 VR技术,如中国专利申请 201710222691 .3(专利名 称: _种基于 VR 技术的验光方法及 VR 眼镜验光仪,专利申请公布号 : CN106963334A, 申请日 : 2017年 4月 7 日 ),其公开了一种基于 VR技术的 验光方法及 VR眼镜验光仪,该方法在 VR系统中建立验光专用图像,并采用拟 合出人眼所看到的清晰图像的位置 x与人眼度数 y之间的关系式 y=f(x),该方法 还提出 ,在验光过程中 ,用户可以通过肢体或语言与 VR系统进行交流、 反馈, 从而调整图像的清晰度。 但是该方法所指的图像清晰度仍然和现有的验光技术 中_样,得到的是某 _个特定的眼球转动方向下(即某个特定的视场方向下) 的最佳镜片设计参数。 若验光人眼球转动到不同方向了 ,就没法进行正常验光 了。 发明内容 Some optometry also uses VR technology, such as Chinese patent application 201710222691 .3 (patent name: _ VR-based optometry method and VR glasses refractometer, patent application publication number: CN106963334A, application date: April 7, 2017 ), which discloses a VR-based optometry method and a VR glasses refractometer, which establishes a optometry-specific image in the VR system, and adopts a position x and a human eye degree of a clear image seen by the human eye. The relationship between y is y=f(x). The method also proposes that during the optometry process, the user can communicate and feedback with the VR system through the body or language to adjust the sharpness of the image. However, the image clarity referred to by this method is still the same as that of the existing optometry technique, and the optimal lens design parameters of a particular eye rotation direction (ie, under a specific field of view direction) are obtained. If the optometry eyeball turns to a different direction, there is no way to perform normal optometry. Summary of the invention
本发明的目的在于克服上述缺点,提供一种基于 VR技术的验光及仿真方 法,其将人眼球的转动考虑在验光过程中。  SUMMARY OF THE INVENTION An object of the present invention is to overcome the above disadvantages and to provide an optometry and simulation method based on VR technology which takes the rotation of the human eye into consideration during the optometry process.
为实现上述目的,本发明所采用的技术方案是:  In order to achieve the above object, the technical solution adopted by the present invention is:
一种基于 VR技术的验光及仿真方法,包括以下步骤:  An optometry and simulation method based on VR technology, comprising the following steps:
第一步:在 VR系统中模拟出光轴方向 Z、 被观察物体;  The first step: simulating the direction of the optical axis in the VR system Z, the object to be observed;
第二步、在 VR系统中仿真设计出一镜片,将该镜片置于所述光轴方向上并 使其位于人眼与被观察物体之间 ,人眼通过所述镜片观察被观察物体;  In the second step, a lens is simulated in the VR system, and the lens is placed in the direction of the optical axis and placed between the human eye and the observed object, and the human eye observes the observed object through the lens;
第三步:对于被观察物体的同一个成像点,将各种可能的不同视场方向 g 定义在一个矢量空间 K中 ,将常规验光中的特定视场方向 g定义在另一个矢量 空间 K' 中 ; The third step: for the same imaging point of the observed object, define various possible different field of view directions g in a vector space K, and define a specific field of view g in the conventional optometry in another vector space K' in;
Figure imgf000004_0001
Figure imgf000004_0001
第五步、 将所述特定视场方向 g的各种参数通过所述映射矩阵转换成 K空 间的参数,从而得出包含各种不同视场方向下的镜片最佳成像参数。  In a fifth step, various parameters of the specific field of view g are converted into parameters of the K space by the mapping matrix, thereby obtaining optimal imaging parameters of the lens including various different fields of view.
定义在 K' 空间中 ,某 _个眼球转动方向 ,g(a , b)矢量方向可以完善成像, 在这个矢量方向 g(a, b)上,人眼捕捉到的光能量为 l(a, b, A ) ,其中 A 为波长; 在 K空间中 ,人眼在矢量方向 g(as,bs)上捕捉到的光能量为 l(as,bs,A ),根据上 述映射矩阵 T: K' K ,定义两空间 K与 K' 光能量的映射矩阵 G : l(a, b,入 ) - l(as,bs,A ) ,并根据以下公式计算镜片最佳成像效果参数:  Defined in the K' space, the direction of the rotation of a certain eyeball, g (a, b) vector direction can be perfect imaging, in this vector direction g (a, b), the light energy captured by the human eye is l (a, b, A ) , where A is the wavelength; in the K space, the light energy captured by the human eye in the vector direction g(as, bs) is l(as, bs, A ), according to the above mapping matrix T: K' K, defines the mapping matrix G of two spatial K and K' light energy: l(a, b, in) - l(as, bs, A), and calculates the optimal imaging effect parameters of the lens according to the following formula:
Figure imgf000004_0002
Figure imgf000004_0002
佳成像效果参数 ,。 Good imaging effect parameters.
上述计算公式使用在矢量空间中 , 由于人眼的眼球转动是有不同的角度, 所以 l(a, b, A )和 l(as,bs,A )中的角度 a和 b有各种不同的值, 因此将它们分别 定义为 l(a], bj,入 )和 l(as],bSj,A ),j=1 , . m,其中 ,j=1 , . m表示不同的角 度。 The above calculation formula is used in the vector space. Since the eye rotation of the human eye has different angles, the angles a and b in l(a, b, A) and l(as, bs, A) have various differences. Values, so they are defined as l(a ] , b j , in) and l(as ] , bS j , A ), j=1 , . m, where j=1 , . m denotes different angles.
根据上述计算最终点传递函数的公式计算最终点传递函数包括以下步骤:  Calculating the final point transfer function according to the above formula for calculating the final point transfer function includes the following steps:
( 1 )在 K空间 ,对于特定图片,选取一系列的 l(asj,bsj,A ),j=1 , . m ; ( 2 )计算映射矩阵 G : l(aj, bj, (asj,bsj,入 ),j=1 , . m ; (1) In the K space, for a particular picture, select a series of l(asj, bsj, A), j=1, .m; (2) Calculate the mapping matrix G: l(aj, bj, (asj, bsj, in), j=1, .m;
( 3 )计算点传递函数 f(as,bs,a,b,入 ); (3) Calculate the point transfer function f(as, bs, a, b, in);
( 4 )在 K' 空间 ,对于上述特定图片,选取三种波长,迭代计算点传递函 数 f(as,bs,a,b,入 ); (4) In the K' space, for the above specific picture, three wavelengths are selected, and the point transfer function f(as, bs, a, b, in) is iteratively calculated;
( 5 )将上述第 ( 2 )步到第 ( 4 )步的计算结果代入到上述计算最终点传递 函数的公式中 ,计算出最终的点传递函数 f ,所述最终的点传递函数 f包含 镜片最佳成像参数。 (5) Substituting the calculation results of the above steps (2) to (4) into the above formula for calculating the final point transfer function, and calculating the final point transfer function f, the final point transfer function f including the lens Optimal imaging parameters.
所述基于 VR技术的验光及仿真方法,还包括镜片验证方法,所述镜片验证 方法包括以下步骤:  The VR-based optometry and simulation method further includes a lens verification method, and the lens verification method includes the following steps:
第 1步、 所述 VR系统根据上述第_步到第五步得出的镜片最佳成像参数 对上述仿真设计出的镜片进行调整而形成为新镜片,该新镜片的各参数完全符 合所述镜片最佳成像参数;  In the first step, the VR system adjusts the simulated lens according to the optimal imaging parameters of the lens obtained in the above steps _ to 5 to form a new lens, and the parameters of the new lens completely conform to the Optimal imaging parameters of the lens;
第 2步、 再模拟人眼通过所述新镜片观察被观察物体,且在贯观察过程中 , 通过不同方向角度转动眼球来验证新镜片的成像效果。  Step 2: Simulate the human eye to observe the observed object through the new lens, and during the observation process, the eyeball is rotated by different angles to verify the imaging effect of the new lens.
本发明的有益效果为 :并发明利用 VR技术仿真设计出镜片,并模拟人眼通 过镜片观察待观察物体,将传统实际验光中的某一个特定视场方向下的各种参 数,通过映射矩阵,转换成包含各种不同视场方向的最佳镜片成像参数;即是 说,本发明将眼球转动的不同方向考虑在验光过程中 ,从而根据本发明验光及 仿真方法得到的最佳镜片参数制作出来的镜片完全能满足实际使用中眼球转动 不同方向的需要,即在佩戴者眼球转动到镜片边缘视场方向下,该镜片的成像 效果同样很好,只会出现较小的像散、 色差、 畸变;即是说,本发明利用 VR技 术将验光与仿真结合起来,从而能为高精度验光、 视力矫正提供完整的解决方 案,解决了现有技术中单一视场方向下验光的问题。 附图说明  The invention has the beneficial effects that: the invention uses the VR technology to simulate and design the lens, and simulates the human eye to observe the object to be observed through the lens, and passes various parameters in a specific field of view direction in the traditional actual optometry through the mapping matrix. Converting to optimal lens imaging parameters including various fields of view; that is, the present invention considers different directions of eye rotation in the optometry process, thereby producing optimal lens parameters obtained according to the optometry and simulation methods of the present invention. The lens can fully meet the needs of different directions of eyeball rotation in actual use, that is, when the wearer's eyeball rotates to the direction of the field of view of the lens edge, the imaging effect of the lens is also very good, only small astigmatism, chromatic aberration, distortion will appear. That is to say, the present invention combines optometry and simulation with VR technology, thereby providing a complete solution for high-precision optometry and vision correction, and solving the problem of optometry in a single field of view in the prior art. DRAWINGS
图 1为本发明验光及仿真方法的流程框图 ;  1 is a flow chart of a method for optometry and simulation of the present invention;
图 2为本发明方法中眼球某_个转动方向 g矢量的示意图 ;  2 is a schematic view of a g-direction of a g-direction of the eyeball in the method of the present invention;
图 3为本发明方法中在 K与 K' 两个不同空间下眼球转动方向示意图 ; 图 4为本发明方法中渐进多焦点镜片曲率的三维显示模型示意图 ; 图 5为本发明方法中渐进多焦点镜片截面曲率显示示意图。 具体实施方式 Figure 3 is a schematic view showing the direction of rotation of the eyeball in two different spaces of K and K' in the method of the present invention; 4 is a schematic diagram of a three-dimensional display model of the progressive multifocal lens curvature in the method of the present invention; FIG. 5 is a schematic diagram showing the curvature of the progressive multifocal lens in the method of the present invention. detailed description
如图 1所示,本发明基于 VR技术的验光及仿真方法包括以下步骤: 第一步:在 VR系统中模拟出光轴方向 Z、 被观察物体;  As shown in FIG. 1 , the optometry and simulation method based on the VR technology of the present invention comprises the following steps: Step 1: Simulate the optical axis direction Z in the VR system, the observed object;
第二步:在 VR系统中仿真设计出一镜片,将该镜片置于所述光轴方向上并 使其位于人眼与被观察物体之间 ,人眼通过所述镜片观察被观察物体;  The second step: emulating a lens in the VR system, placing the lens in the direction of the optical axis and positioning it between the human eye and the object to be observed, and the human eye observing the observed object through the lens;
第三步:对于被观察物体的同一个成像点,将各种可能的不同视场方向 g 定义在一个矢量空间 K中 ,将常规验光中的特定视场方向 g定义在另一个矢量 空间 K' 中 ; The third step: for the same imaging point of the observed object, define various possible different field of view directions g in a vector space K, and define a specific field of view g in the conventional optometry in another vector space K' in;
Figure imgf000006_0001
Figure imgf000006_0001
第五步、 将所述特定视场方向 g的各种参数通过所述映射矩阵转换成 K空 间的参数,从而得出包含各种不同视场方向下的镜片最佳成像参数。  In a fifth step, various parameters of the specific field of view g are converted into parameters of the K space by the mapping matrix, thereby obtaining optimal imaging parameters of the lens including various different fields of view.
如图 2所示,在角坐标系统中 ,矢量 g(a,b)在 YOZ平面的投影分量为 g y,在 XOZ平面的投影分量为 g x ,其中 g ^Z方向的夹角为 a, g x Z方向的夹角为 b,光 轴的方向定义为 Z方向,人眼位于 0点所在位置。 As shown in Fig. 2, in the angular coordinate system, the projection component of the vector g(a, b) in the YOZ plane is g y , the projection component in the XOZ plane is g x , and the angle in the g ^ Z direction is a, The angle between the g x Z direction is b, the direction of the optical axis is defined as the Z direction, and the human eye is at the position of the 0 point.
如图 3所示,人眼通过镜片观察被观察物体,光轴为 z方向 ,被观察物体 上有两点 A、 B ,当人眼在某 _个眼球转动角度下,即视场方向为 g A下,通过 眼镜可以清晰地观察到 A点,在视场方向为 g B下,通过眼镜可以清晰观察到 B 点, g A和 g B为特定的方向 ,定义在上述矢量空间 K' 中。 在矢量空间 K中 , 有任意多的方向可以观察到物体上的 A点,例如 gAS方向 ,同理,在矢量空间 K 中 ,有任意多的方向可以观察到物体上的 B点,例如 g BS方向。 可以理解为 , 在常规的验光系统中 ,只在 K' 空间中来评价眼镜的成像效果,如像散、 色差、 畸变等参数。 而本发明则是将所述特定视场方向 g 的各种参数通过所述映射矩 阵转换成 K空间的参数,即是说将 K' 空间的参数通过映射矩阵 T转换成 K空 间的参数,即将单一视场下的较好的成像条件转换成多个视场下的较好的成像 条件。其中映射矩阵能反映在人眼眼球转动的条件下,镜片原有的成像质量 (像 散、 色差、 畸变等 )是如何下降的。 在角坐标系统中 ,所述映射矩阵 T: K' K理解为 T : (a,b) (as,bs)。 As shown in Fig. 3, the human eye observes the observed object through the lens, and the optical axis is in the z direction. There are two points A and B on the observed object. When the human eye is at a certain angle of rotation of the eyeball, that is, the direction of the field of view is g. In A , the point A can be clearly observed through the glasses. In the direction of the field of view, g B , the point B can be clearly observed through the glasses, and g A and g B are specific directions, which are defined in the above vector space K'. In the vector space K, there are any more directions to observe the point A on the object, such as the g AS direction. Similarly, in the vector space K, there are any more directions to observe the point B on the object, such as g. BS direction. It can be understood that in the conventional optometry system, the imaging effects of the glasses, such as astigmatism, chromatic aberration, distortion, and the like, are evaluated only in the K' space. The present invention is to convert various parameters of the specific field of view direction g into parameters of the K space through the mapping matrix, that is, to convert the parameters of the K' space into the parameters of the K space through the mapping matrix T, that is, Better imaging conditions in a single field of view translate into better imaging conditions across multiple fields of view. The mapping matrix can reflect how the original imaging quality (astigmatism, chromatic aberration, distortion, etc.) of the lens decreases under the condition of the eyeball rotation. In the angular coordinate system, the mapping matrix T: K' K is understood to be T: (a, b) (as, bs).
为了更好地理解映射矩阵 T,定义在 K' 空间中 ,某 _个眼球转动方向 , g(a , b)矢量方向可以完善成像,或者说在传统的验光方式下,眼镜的佩戴者在该方向 可以清晰地观察到待观察物体,即镜片对像散、 色差、 畸变等都校正到一个比 较合理的范围内。 在这个矢量方向 g(a, b)上,人眼捕捉到的光能量为 l(a, b, A ) , 其中 A 为波长 ;在 K空间中 , 人眼在矢量方向 g(as,bs)上捕捉到的光能量为 l(as,bs,A ),根据上述映射矩阵 T: K' K,定义光能量的映射矩阵 G : l(a, b,入 ) - l(as,bs,A ) ,并根据以下公式计算镜片最佳成像效果参数: In order to better understand the mapping matrix T, defined in the K' space, a certain _ eyeball rotation direction, g (a, b) vector direction can be perfect imaging, or in the traditional optometry mode, the wearer of the glasses is The direction can clearly observe the object to be observed, that is, the lens corrects the astigmatism, chromatic aberration, distortion, etc. to a reasonable range. In this vector direction g(a, b), the light energy captured by the human eye is l(a, b, A), where A is the wavelength; in the K space, the human eye is in the vector direction g(as, bs) The captured light energy is l(as, bs, A), and according to the above mapping matrix T: K' K, the mapping matrix G of the light energy is defined: l(a, b, in) - l(as, bs, A ), and calculate the optimal imaging effect parameters of the lens according to the following formula:
Figure imgf000007_0001
Figure imgf000007_0001
式中 ,
Figure imgf000007_0002
,最终的点传递函数即包括所述镜片 最佳成像效果参数,点传递函数可以理解为不同的单色图像的相关联关系函数。 从上述计算公式可以看出 ,在 K空间中 ,人眼捕捉到的光能量 l(as,bs,A )等于 l(a, b, 入 )和点传递函数 / , , 的积分。 上述计算公式使用在矢量空间中 ,由于人眼的眼球转动是有不同的角度,所 以 l(a, b, A )^P I(as,bs,A )中的角度 a和 b有各种不同的值,因此必须将它们分别定 义为 l(a], b],入 ) l(asj,bs],入 ),j=1 , . m,其中 ,j=1 , . m是表示不同的角 度。
In the formula,
Figure imgf000007_0002
The final point transfer function includes the optimal imaging effect parameters of the lens, and the point transfer function can be understood as an associated relation function of different monochrome images. It can be seen from the above calculation formula that in the K space, the light energy l(as, bs, A) captured by the human eye is equal to the integral of l(a, b, in) and the point transfer function /, . The above calculation formula is used in the vector space. Since the eye rotation of the human eye has different angles, the angles a and b in l(a, b, A)^PI(as, bs, A) have various kinds of different Values, so they must be defined as l(a), b], in) l(asj,bs], in), j=1, .m, where j=1, . m is a different angle.
根据上述公式计算镜片最佳成像效果参数包括以下步骤:  Calculating the optimal imaging effect parameters of the lens according to the above formula includes the following steps:
( 1 )在 K空间 ,对于特定图片 (即某 _个视场方向下,通过传统验光人眼 观察认为比较清晰的一种图片,如常用的各种方向的 E子表格等 ),选取一系列 的 l(aSj,bSj,A ),j=1 , . m ; (1) In the K space, for a specific picture (that is, a picture that is considered to be relatively clear by a traditional optometry human eye in a certain field of view direction, such as commonly used E sub-tables in various directions, etc.), select a series l(aS j , bS j , A ), j=1 , . m ;
( 2 )计算映射矩阵 G : l(a], bj,
Figure imgf000007_0003
(2) Calculate the mapping matrix G: l(a), bj,
Figure imgf000007_0003
( 3 )计算点传递函数 f(as,bs,a,b,入 );  (3) Calculate the point transfer function f(as, bs, a, b, in);
( 4 )在 K' 空间 ,对于上述特定图片,选取 F、 D、 C三种光的波长,迭代 计算点传递函数 f(as,bs,a,b,入 ); (5)将上述第( 2)步到第( 4)步的计算结果代入到上述计算公式中 ,计 算出最终的点传递函数 f ,最终得到的点传递函数包含镜片最佳成像参数。 步映射矩阵 G是 l(aj, bj, A) l(aSj,bSj,A) ,即将 K' 空间的参数转换到 K 空间中 ,所述第( 1)步与第( 2)则是已知 K空间的参数,然后反向推 K' 空 间内的参数。 (4) In the K' space, for the above specific picture, select the wavelengths of the three lights of F, D, C, and iteratively calculate the point transfer function f(as, bs, a, b, in); (5) Substituting the calculation results of the above steps (2) to (4) into the above calculation formula, and calculating the final point transfer function f, and finally obtaining the point transfer function including the optimal imaging parameters of the lens. The step mapping matrix G is l(a j , b j , A) l(aS j , bS j , A) , that is, the parameters of the K′ space are converted into the K space, the steps (1) and (2) Then it is the parameter of the known K space, and then the parameters in the K' space are pushed backwards.
所述 F光为青光,波长为 486nm,D光即为黄光,波长为 589nm,C光即为 红光,波长为 656nm。  The F light is cyan, the wavelength is 486 nm, the D light is yellow light, the wavelength is 589 nm, the C light is red light, and the wavelength is 656 nm.
所述第( 2)步与第( 4)步计算的点传递函数是单色光条件下,最终的点 传递函数 f是考虑不同的波长下的最终结果。  The point transfer function calculated in steps (2) and (4) is a monochromatic light condition, and the final point transfer function f is the final result considering different wavelengths.
综上所述,本发明将眼球转动考虑在验光过程中 ,将传统实际验光中的某 一个特定视场方向下的各种参数,通过映射矩阵,转换成包含各种不同视场方 向的最佳镜片成像参数,即将不同视场方向下,大幅面的图像成像清晰的条件 将给出 ,从而解决了现有技术中单 _视场下验光的问题。  In summary, the present invention considers the rotation of the eyeball in the process of optometry, and converts various parameters in a specific field of view direction of the conventional actual optometry into a matrix containing various fields of view. The lens imaging parameters, that is, the conditions for clear imaging of large-format images in different fields of view will be given, thereby solving the problem of optometry in the single field of view in the prior art.
如图 4所示的渐进多焦点镜片的三维模型显示中 ,颜色不同代表不同的镜片 曲率半径。  In the three-dimensional model display of the progressive addition lens shown in Fig. 4, the color differences represent different lens curvature radii.
如图 5所示的渐进多焦点镜片,在镜片的某一面, 曲率半径不断变化,即眼 球在不同的转动方向下,眼镜的度数不一样,对于这种不同半径值的平滑过渡, 样条曲线显示出不同的曲率半径, 曲率半径大小相对值通过指示线的相对长短 来决定。  As shown in Figure 5, the progressive multifocal lens has a constant radius of curvature on one side of the lens, that is, the eyeball is in different directions of rotation, and the degree of the glasses is different. For such a smooth transition of different radius values, the spline curve Different radii of curvature are shown, and the relative magnitude of the radius of curvature is determined by the relative length of the indicator line.
在图 4、 5所显示的这类平滑过渡的渐进多焦点镜片中 ,在不同视场方向下, 镜片的度数不同,如果采用目前传统的验光发法将产生更多的误差,而利用本 发明提供的验光及仿真方法,可以有效减小误差,提高此类镜片的验光精度。  In the smooth transitional progressive multifocal lens of the type shown in Figures 4 and 5, the degrees of the lenses are different in different fields of view, and if the conventional optometry method is used, more errors will be generated, and the present invention is utilized. The optometry and simulation methods provided can effectively reduce the error and improve the optometry precision of such lenses.
以一个渐进多焦点的老花镜片为例进行说明 ,即如果配戴者需要的是一个视 近区 +5.0D的老花镜,同时在视远区有其它度数,在视近区和视远区之间存在过 渡区,以及眼镜的周边区,对于常规的验光来说,在进行此类验光时,其准确 度需要和被验光者准确配合才能完成,误差较大;而经过本发明方法得出的最 佳镜片成像参数制作出来的 +5.0D的老花镜,在距离眼镜 40cm远,佩戴者眼球 转动 35度后,观察视场方向效果,该老花镜畸变小于 2% ,子午和弧矢方向的像 散小于 0.03D ,验光精度非常高。 Take a progressive multifocal presbyopic lens as an example, that is, if the wearer needs a view Near-field +5.0D reading glasses, at the same time there are other degrees in the far-distance area, there is a transition zone between the near-field and the far-field, and the peripheral area of the glasses. For conventional optometry, such optometry is performed. When the accuracy is required to be accurately matched with the optometry, the error is large; and the +5.0D reading glasses produced by the optimal lens imaging parameters obtained by the method of the present invention are 40 cm away from the glasses, the wearer After the eyeball rotates 35 degrees, the effect of the field of view is observed. The reading lens distortion is less than 2%, the astigmatism in the meridional and sagittal directions is less than 0.03D, and the optometry precision is very high.
在本实施例中 ,较佳的,本发明基于 VR技术的验光及仿真方法还包括镜片 验证方法,所述镜片验证方法包括以下步骤:  In this embodiment, preferably, the optometry and simulation method based on the VR technology of the present invention further comprises a lens verification method, and the lens verification method comprises the following steps:
第 1 步、 所述 VR系统根据上述第_步到第五步得出的镜片最佳成像参数 对上述仿真设计出的镜片进行调整而形成为新镜片,该新镜片的各参数完全符 合所述镜片最佳成像参数;  In the first step, the VR system adjusts the lens designed by the simulation according to the optimal imaging parameters of the lens obtained in the above steps _ to 5 to form a new lens, and the parameters of the new lens completely conform to the Optimal imaging parameters of the lens;
第 2步、 再模拟人眼通过所述新镜片观察被观察物体,且在贯观察过程中 , 通过不同方向角度转动眼球来验证新镜片的成像效果,如像散、 色差、 畸变等 参数。  Step 2: Simulate the human eye to observe the observed object through the new lens, and during the observation process, the eyeball is rotated by different angles to verify the imaging effect of the new lens, such as astigmatism, chromatic aberration, distortion and the like.
如此,通过镜片验证方法可以进一步确保通过本发明验光及仿真方法得出 的镜片最佳成像参数的有效性。  Thus, the effectiveness of the optimal imaging parameters of the lens obtained by the optometry and simulation methods of the present invention can be further ensured by the lens verification method.

Claims

权 利 要 求 书 Claim
1、 一种基于 VR技术的验光及仿真方法,其特征在于:包括以下步骤:  1. An optometry and simulation method based on VR technology, characterized in that it comprises the following steps:
第一步:在 VR系统中模拟出光轴方向 Z、 被观察物体;  The first step: simulating the direction of the optical axis in the VR system Z, the object to be observed;
第二步、在 VR系统中仿真设计出一镜片,将该镜片置于所述光轴方向上并 使其位于人眼与被观察物体之间 ,人眼通过所述镜片观察被观察物体;  In the second step, a lens is simulated in the VR system, and the lens is placed in the direction of the optical axis and placed between the human eye and the observed object, and the human eye observes the observed object through the lens;
第三步:对于被观察物体的同一个成像点,将各种可能的不同视场方向 g 定义在一个矢量空间 K中 ,将常规验光中的特定视场方向 g定义在另一个矢量 空间 K' 中 ; The third step: for the same imaging point of the observed object, define various possible different field of view directions g in a vector space K, and define a specific field of view g in the conventional optometry in another vector space K' in;
Figure imgf000010_0001
Figure imgf000010_0001
第五步、 将所述特定视场方向 g的各种参数通过所述映射矩阵转换成 K空 间的参数,从而得出包含各种不同视场方向下的镜片最佳成像参数。  In a fifth step, various parameters of the specific field of view g are converted into parameters of the K space by the mapping matrix, thereby obtaining optimal imaging parameters of the lens including various different fields of view.
2、 根据权利要求 1所述的基于 VR技术的验光及仿真方法,其特征在于:定 义在 K' 空间中 ,某_个眼球转动方向 , g(a , b)矢量方向可以完善成像,在这 个矢量方向 g(a, b)上,人眼捕捉到的光能量为 l(a, b, A ),其中 A 为波长;在[< 空间中 ,人眼在矢量方向 g(as,bs)上捕捉到的光能量为 l(as,bs,A ),根据上述映 射矩阵 T: K' K ,定义两空间 K与 K' 光能量的映射矩阵 G : l(a, b, A ) l(as,bs,A ) ,并根据以下公式计算镜片最佳成像效果参数:
Figure imgf000010_0002
2. The VR-based optometry and simulation method according to claim 1, characterized in that: defined in the K' space, a certain _ eye rotation direction, g (a, b) vector direction can be perfect imaging, in this In the vector direction g(a, b), the light energy captured by the human eye is l(a, b, A), where A is the wavelength; in [< space, the human eye is in the vector direction g(as, bs) The captured light energy is l(as, bs, A ), and according to the above mapping matrix T: K' K , a mapping matrix G of two spatial K and K′ light energies is defined: l(a, b, A ) l(as , bs, A), and calculate the optimal imaging effect parameters of the lens according to the following formula:
Figure imgf000010_0002
成像效果参数, da,db代表对变量 a, b进行积分。 The imaging effect parameters, da, db, represent the integration of the variables a, b.
3、 根据权利要求 2所述的基于 VR技术的验光及仿真方法,其特征在于:上 述计算公式使用在矢量空间中 ,由于人眼的眼球转动是有不同的角度,所以 l(a, b,入 )m l(as,bs,A )中的角度 a和 b有各种不同的值,因此将它们分别定义为 l(a], bj,入 )和 l(as],bSj,A ),j=1 , . m,其中 , j=1 , . m表示不同的角度。 3. The VR-based optometry and simulation method according to claim 2, wherein the calculation formula is used in a vector space, and since the eye rotation of the human eye has different angles, l(a, b, The angles a and b in the ml(as, bs, A) have various values, so they are defined as l(a), b j , in) and l(as ] , bS j , A ) respectively. , j=1, .m, where j=1, .m denotes different angles.
4、 根据权利要求 3所述的基于 VR技术的验光及仿真方法,其特征在于: 根据上述计算最终点传递函数的公式计算最终点传递函数包括以下步骤:  4. The VR-based optometry and simulation method according to claim 3, wherein: calculating the final point transfer function according to the formula for calculating the final point transfer function comprises the following steps:
( 1 )在 K空间 ,对于特定图片,选取一系列的 l(asj,bsj,A ),j=1 , . m ; (1) In the K space, for a specific picture, select a series of l(asj, bsj, A), j=1, .m;
( 2 )计算映射矩阵 G : l(aj, bj, (asj,bsj,入 ),j=1 , . m ; ( 3 )计算点传递函数 f(as,bs,a,b,入 ); (2) Calculate the mapping matrix G: l(aj, bj, (asj, bsj, in), j=1, .m; (3) Calculate the point transfer function f(as, bs, a, b, in);
( 4 )在 K' 空间 ,对于上述特定图片,选取三种波长,迭代计算点传递函 数 f(as,bs,a,b,入 ); (4) In the K' space, for the above specific picture, three wavelengths are selected, and the point transfer function f(as, bs, a, b, in) is iteratively calculated;
( 5 )将上述第 ( 2 )步到第 ( 4 )步的计算结果代入到上述计算最终点传递 函数的公式中 ,计算出最终的点传递函数 f ,所述最终的点传递函数 f包含镜片 最佳成像参数。  (5) Substituting the calculation results of the above steps (2) to (4) into the above formula for calculating the final point transfer function, and calculating the final point transfer function f, the final point transfer function f including the lens Optimal imaging parameters.
5、 根据权利要求 1或 2或 3或 4所述的基于 VR技术的验光及仿真方法,其 特征在于:还包括镜片验证方法,所述镜片验证方法包括以下步骤:  5. The VR-based optometry and simulation method according to claim 1 or 2 or 3 or 4, further comprising: a lens verification method, the lens verification method comprising the steps of:
第 1步、 所述 VR系统根据上述第_步到第五步得出的镜片最佳成像参数 对上述仿真设计出的镜片进行调整而形成为新镜片,该新镜片的各参数完全符 合所述镜片最佳成像参数;  In the first step, the VR system adjusts the simulated lens according to the optimal imaging parameters of the lens obtained in the above steps _ to 5 to form a new lens, and the parameters of the new lens completely conform to the Optimal imaging parameters of the lens;
第 2步、 再模拟人眼通过所述新镜片观察被观察物体,且在贯观察过程中 , 通过不同方向角度转动眼球来验证新镜片的成像效果。  Step 2: Simulate the human eye to observe the observed object through the new lens, and during the observation process, the eyeball is rotated by different angles to verify the imaging effect of the new lens.
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