Patent Application
20170075139
The invention relates to a spectacle lens for an observer, comprising a body which is transparent or at least partly transparent to light and has a phase object which guides the light incident at an angle of incidence α on a side distant from the observer into a direction depending on the wavelength λ of the light and the angle of incidence α of the light.
The invention also extends to a production method for such a spectacle lens, and to a method for establishing the configuration of such a spectacle lens.
A spectacle lens of the type set forth at the outset is known from WO 99/34248 A1. A spectacle lens with holographic optical elements (HOE) lying one above the other is described therein. Here, the holographic optical elements form a volume grating, by means of which the light incident on the spectacle lens at a certain angle of incidence is diffracted, leading to deflection of the light, incident on the spectacle lens, for this angle of incidence.
WO 2014/064163 A1 describes a spectacle lens with a multiplicity of light-diffracting zones, which have a different refractive power.
Spectacle lenses in the form of refractive progressive lenses allow an observer suffering from a visual impairment to be able to observe objects arranged at different distances with a more or less sharp visual impression, even if the accommodation capability of the eyes of this observer is no longer there, for example, due to old age, or greatly limited.
Visual zones are usually defined for the configuration of refractive progressive lenses. These visual zones relate to regions of the surface of a progressive lens penetrated by the viewing direction of an observer. If the observer peers through different visual zones, this observer can see objects at different object distances in focus, without an eye requiring accommodation herefor.
Refractive progressive lenses generally have a distance zone which, when these lenses are used as intended, is penetrated by the viewing direction of an eye of an observer peering into the distance. When peering through the distance zone, the objects arranged at infinity for the observer should be imaged in focus on the retina. Moreover, refractive progressive lenses usually also have a so-called near zone in addition to the distance zone, the near zone being spaced apart from the distance zone and, when the progressive lens is used as intended, being peered through by an observer with a maximum accommodation in order to observe objects arranged at a near distance (for example, 40 cm) in front of the eyes.
Progressive lenses often have a so-called progression channel between the near zone and the distance zone. This progression channel connects the distance zone to the near zone. The refractive power of the progressive lens differs locally in the progression channel. In order to provide a wide visual field to an observer with the progressive lens, attempts are made, as a matter of principle, for the progression channel to be as wide as possible. However, the obtainable width of the progression channel is restricted due to the differential geometric Minkwitz theorem. A consequence of this mathematical theorem is that an observer must accept non-correctable astigmatic imaging aberrations with increasing width of the progression channel, that is, an astigmatism caused by the Minkwitz theorem. Thus, fundamental limits are placed on the imaging quality of refractive progressive lenses and on the possible extent of the near region zone and distance region zone of refractive progressive lenses.
It is an object of the invention to provide a spectacle lens for an observer, the optical effect of which for different viewing directions can be adapted with an improved imaging quality to the requirements of the observer, and to specify a method for establishing the configuration of such a spectacle lens and a production method for such a spectacle lens.
In the present case, the optical effect of a spectacle lens is understood to mean the property of deflecting light.
The invention is based on the idea that, for an observer with a spectacle lens, different distance regions can be visualized in focus and without the astigmatic imaging aberrations necessarily occurring in the peripheral regions of a progressive lens if the light beams imaging the object region are deflected not by refraction but by diffraction.
In the present case, the diffraction of light is understood to mean the physical phenomenon of the change in the phase of the light, caused by a phase object, on account of interactions between light and matter. Here, a phase object is preferably a transparent object which influences or changes the phase of the light. A phase object needs a diffraction structure in order to diffract light at the phase object. Such a diffraction structure represents a regular, or else irregular, spatial modulation of the complex refractive index, for example, in the form of a grating, which may extend in one dimension or in two dimensions (plane grating) or in three dimensions (volume grating).
A diffraction structure diffracts the light in a manner dependent on the angle of incidence of the light, at which it is incident on the diffraction structure, and in a manner dependent on the wavelength λ of the light. If light is diffracted at a diffraction structure, it can be deflected in one or more different, discrete directions due to constructive interference. In the present case, these directions are referred to as orders of diffraction and denoted, in line with general convention, by integers 0, ±1, ±2, ±3, . . . , with the central order being denoted by 0 and all further orders being numbered consecutively.
Accordingly, diffraction of the light into an order of diffraction |m|≧1 is understood to mean the deflection of the light in the direction defined by the order of diffraction which arises by constructive interference of phase-shifted light.
A spectacle lens according to the invention allows an observer, in particular, to perceive objects arranged in different distance regions in focus and without imaging aberrations which distort the visual impression, even in the case of a restricted accommodation capability of the eyes.
A spectacle lens according to the invention has a body which is transparent or at least partly transparent to the light. Thus, such a body is at least partly transparent to the light.
The angle to which a light beam is diffracted by a diffraction structure and the angle at which a light beam diffracted by the diffraction structure may be incident on the diffraction structure increase with increasing absolute value of the order of diffraction in this case. Here, a positive order of diffraction corresponds to a deflection angle for the light, related to the direction of incidence, which is positive; a negative order of diffraction corresponds to a negative deflection angle related to the direction of incidence of the light.
The ratio of the intensity Idiffracted of the light diffracted by a diffraction structure into an order of diffraction |m|≧1 to the intensity Iincident of the light incident on a boundary of the diffraction structure at a specific angle of incidence α′ is presently referred to as the diffraction efficiency η of the diffraction structure. The boundary of a diffraction structure may coincide with the surface of the transparent body of the spectacle lens, but this need not be the case. The boundary of a diffraction structure may also be situated within the transparent body.
The invention exploits the fact that the diffraction efficiency of a diffraction structure in a layer made of an optically transparent material arranged on a carrier is dependent on:
The implicitly existing relation due to the dependencies between these variables means that it is possible to specify, for a given wavelength, the angle of incidence at which the layer, in which the refractive index is modulated, efficiently diffracts the light incident thereon, that is, in such a way that the diffraction efficiency n is greater than a specific threshold which is fundamentally selectable.
According to the invention, the phase object has a multiplicity of diffraction structures, which diffract monochromatic light at a wavelength of 380 nm≦λ≦800 nm with a diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the monochromatic light is incident at an angle of incidence α on the side of the spectacle lens distant from the observer which lies within a diffraction-structure-specific angle interval which is 15° wide and depends on the wavelength of the light.
In the present case, the angle of incidence of the light on a boundary is understood to mean the angle α formed by the propagation direction of the light with the surface normal {right arrow over (n)} of the boundary facing the incident light.
It is advantageous if the phase object of the transparent body of the optical visual aid comprises a multiplicity of diffraction structures, which each deflect all light of a wavelength λ lying in a diffraction-structure-specific wavelength interval λ0±0.1 μm, the wavelength being incident at an angle of incidence α which lies in a diffraction-structure-specific angle of incidence range α0±2.5°, preferably at an angle of incidence α which lies in a diffraction-structure-specific angle of incidence range α0±2°, on the side of the spectacle lens distant from the observer, with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1.
It is possible to deviate from the values, specified above, for the width of the wavelength interval of 0.2 μm and the width of the range for the angle of incidence α and for the threshold ηmin of 70% for the diffraction efficiency η, without departing from the invention in the process. However, the deviation from the aforementioned values is no more than 20%, preferably no more than 10%, particularly preferably no more than 5%. By way of example, a single diffraction structure in an optical visual aid according to the invention may have a thickness of 17 μm and an extent of approximately 25 square millimeters (mm2). The aforementioned property of a diffraction structure can be achieved by means of, for example, a density LD=1/Λ of light-diffracting structures in the form of a modulated refractive index (line density), where Λ denotes the period of the structures, which is approximately 300 to 5000 lines per millimeter in the case of a refractive index of, for example, n=1.492 and the modulation amplitude of Δn=0.02. Here, the optically transparent material may be a photopolymer, in particular a photopolymer which has the formulation described in WO 2012/062658 A1, to which reference is herewith made in the entirety thereof and the disclosure of which is included in the description of the present invention.
The diffraction structures are preferably embodied in such a way that, in the parameter plane spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis and an angle of incidence parameter axis, they approximately each have an efficiency window extending along a straight line, which increases monotonically in relation to the wavelength λ, in which efficiency window the light incident at a specific angle of incidence α on the side of the spectacle lens distant from the observer is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane, lies in the efficiency window.
A straight line along which the efficiency window extends may, in particular, be a straight line which approximately follows a line passing through the efficiency window and on which the diffraction efficiency is at a maximum. Hence, at the points lying on this line, the gradient of the diffraction efficiency η according to the angle of incidence α and the wavelength λ in the parameter plane spanned by the wavelength λ and the angle of incidence α extends tangentially at this line.
Here, δ≦0.036°/nm, preferably δ≦0.024°/nm, particularly preferably δ≦0.012°/nm, applies to the gradient δ of the straight line.
According to the invention, the diffraction structures in the parameter plane spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis and an angle of incidence parameter axis can also be embodied in such a way that they each have an efficiency window extending along a straight line, which increases monotonically in relation to the wavelength λ, between a first tangent parallel to the increasing straight line and a second tangent displaced in parallel to the first tangent in the direction of the angle of incidence parameter axis by the angle Δα≦20°, preferably Δα≦15°, particularly preferably Δα≦10° or Δα≦6°, in which efficiency window the light incident at a specific angle of incidence α on the spectacle lens is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane, lies in the efficiency window.
Here, the efficiency window may extend approximately symmetrically along the straight line.
To this end, each diffraction structure for light can be, in particular, embodied as a modulation of the complex refractive index n(λ; x,y,z):=nr(λ; x,y,z)+ini(λ; x,y,z) of the transparent body in at least one spatial direction.
Here, an amplitude Δn(λ) of the modulation of the complex refractive index n(λ; x,y,z) may, for example, satisfy the following relationship for the light of the wavelength 380 nm≦λ≦800 nm: 0.01≦|Δn(λ)|≦0.05.
It is advantageous if each diffraction structure forms an actuator-compensator pair with a further diffraction structure which is spatially separate from the diffraction structure, wherein the deflections of the light incident at the angle of incidence on the side of the spectacle lens distant from the observer caused by the diffraction structures forming an actuator-compensator pair are at least partly canceled.
Here, the diffraction structures forming an actuator-compensator pair may adjoin one another. However, it is also possible for the phase objects forming an actuator-compensator pair to be spaced apart from one another.
The phase object in the body of the spectacle lens may have an optical effect, that is, a light-deflecting effect, in particular a lens effect. The body may also comprise a phase object which is constructed from layers, lying one above the other, of an optically transparent material with a modulated refractive index. Here, the layers, lying one above the other, of the optically transparent material may be applied to a carrier transparent to the visible light.
Within the scope of the invention, it is possible for the spectacle lens to also have a light-refracting effect in addition to the light-diffracting effect. The optical effect of the spectacle lens is preferably dependent on a viewing direction, passing through the spectacle lens, of the observer.
The body of the spectacle lens, which is transparent or at least partly transparent to the light, may have an edge and two or more connected visual zones which have a different optical effect, extend over the spectacle lens and cover the spectacle lens in the process, wherein the transparent body of the spectacle lens, in this case, has no regions with an astigmatism caused by the Minkwitz theorem.
The invention also extends to a method for establishing the configuration of a spectacle lens, in which
Moreover, the invention also extends to a method for establishing the configuration of a spectacle lens, in which a predetermined optical transfer function at least partly compensates at least one visual impairment of the observer.
Moreover, the invention extends to a production method for a spectacle lens,
The invention will now be described with reference to the drawings wherein:
The spectacles 10 shown in
The spectacle lenses 16, 18 each have a body that is transparent to the visible light. In principle, the configuration of the spectacle lens 16 corresponds to the configuration of the spectacle lens 18. Preferably, the spectacle lenses 16, 18 have a preferably individualized optical effect, which has been adapted for the left eye and the right eye of an observer. The spectacle lenses 16, 18 have a body which is produced from plastic which transmits the visible light.
There respectively are phase objects 20, 22 in the transparent body of the spectacle lens 16 and of the spectacle lens 18. These phase objects 20, 22 contain a multiplicity of diffraction structures.
The diffraction structures 24, 26 are embodied as a spatial modulation of the complex refractive index of the transparent body of the spectacle lens 16. In the spectacle lens 16, the second diffraction structure 26 is arranged at a distance from the first diffraction structure 24. That is, the first diffraction structure 24 and the second diffraction structure 26 are spatially separated from one another here. Hence, there is no overlap between the diffraction structures 24, 26 in the spectacle lens 16 in the present case.
Of the many diffraction structures 24, 26 of the phase object of the spectacle lens 16, two form a so-called actuator-compensator pair 31 in each case. In an actuator-compensator pair 31, the deflection of the light which is caused by one diffraction structure, for example, the diffraction structure 26, when the light passes through this diffraction structure is at least partially undone by the other diffraction structure, for example, the diffraction structure 24, if the light also passes through this diffraction structure.
Hence, the phase object of the body of the above-described spectacle lens has a multiplicity of actuator-compensator pairs 31. It should be noted that the diffraction structures forming an actuator-compensator pair 31 need not necessarily adjoin one another but may also be spaced apart from one another.
The phase object of the spectacle lens 16 contains at least one actuator-compensator pair 31 made of two different diffraction structures 24, 26 for each surface segment 32 of the object surface 29, by means of which diffraction structures the light which originates from a surface segment 32 and is incident on the spectacle lens 16 is diffracted in such a way that a sharp image of the relevant surface segment 32 of the object surface 29 arises on the retina 36 of the eye 27 of the observer. Here, the actuator-compensator pairs 31 in the phase object of the spectacle lens 16 bring about an overall image of the object surface 29, constructed from images, which are combined in a mosaic-like manner, of different surface segments 32 of the object surface 29, on the retina 36.
In this case, the light incident on the boundary 33 of the diffraction structure 26 in the propagation direction 49 at the angle of incidence α′ lying in the angle of incidence range α′0±2° is diffracted with the diffraction efficiency η≧70% in the direction of the first diffraction maximum m=1, which has been identified by the arrow 50. The practical deflection of the light incident on the boundary 35 in the direction of the arrow 50, connected therewith, is at least partly undone again because of the corresponding diffraction of the light in the direction denoted by the arrow 52 in the diffraction structure 24 with the diffraction efficiency η≧70%.
The diffraction structures 24, 26 in the spectacle lens 16 have the property that the amplitude Δn(λ) of the modulation of the complex refractive index n(λ; x,y,z) of the phase object of this diffraction structure satisfies the following relationship for light of the wavelength 380 nm≦|Δn(λ)|≦0.05.
All diffraction structures 24, 26 of the transparent body of the spectacle lens are dimensioned in such a way that they diffract light at a wavelength λ lying in a diffraction-structure-specific wavelength interval Δ0±0.1 μm, which light is incident on the boundary 33 facing the object surface 29 (see
The complex refractive index n(λ; x,y,z) in the diffraction structure 26 has a curve which has a translational invariance in the direction of the line 43. Here, in the diffraction structure 24, the complex refractive index n(λ; x,y,z) has translational invariance in the direction of the line 45. It should be noted that, as a matter of principle, the lines 43, 45 can be not only straight, but also curved.
By setting the direction of a local translational invariance of the complex refractive index n(λ; x,y,z) in a diffraction structure 26 of the phase object in the spectacle lens 16, it is possible to set, in a defined manner, the direction in which a light beam which passes through the relevant diffraction structure in the phase object is diffracted.
Here, the invention exploits the fact that, as identified by the inventors, a phase object embodied in the transparent body of a spectacle lens may be constructed from a multiplicity of diffraction structures 24, 26 which diffract light. Here, the diffraction structures in a phase object may also be at least partly overlaid on one another. However, every diffraction structure only diffracts the light whose wavelength λ lies in a specific wavelength range Δ0±Δλ and which is incident on the diffraction structure, in relation to the object-side boundary, at an angle of incidence α′ lying in a specific diffraction-structure-specific angle of incidence range α0±Δα.
The different diffraction structures matched to a specific wavelength range λ0±Δλ and a specific angle of incidence range α′0±Δα′ for the light do not have any perceivable, light-diffracting influence on light whose wavelength λ and whose angle of incidence α′ in relation to the object-side boundary lie outside of the characteristic, diffraction-structure-specific range for the angle of incidence α′ and the wavelength λ of a single diffraction structure component.
The spatial overlay of the multiplicity of light-diffracting diffraction structures may be, for example, a volume grating of the complex refractive index. By way of example, such a volume grating can be generated by a holographic adjustment of the complex refractive index of a material, such as, for example, a photopolymer, which is transparent to light lying in the visible spectral range with a wavelength of 380 nm≦λ≦800 nm.
A spatial overlay of a multiplicity of light-diffracting diffraction structure components may, in particular, exist in the form of layers, lying over one another, of an optically transparent material with a modulated refractive index, wherein the layers lying over one another are applied onto a carrier which is transparent to the visible light.
In this respect, the inventors discovered in comprehensive experiments that the diffraction efficiency η, shown in the graph 52 in
According to the invention, the diffraction structures 56, 58, 60 each have the property that there is an efficiency window 65 extending along a straight line 57, which increases monotonically in relation to the wavelength λ, in the parameter plane 55 spanned by the angle of incidence α′ and the wavelength λ with a wavelength parameter axis 51 and an angle of incidence parameter axis 53. In this efficiency window 65, the light incident at a specific angle of incidence α′ on the spectacle lens 16, 18 is diffracted by means of the diffraction structures 56, 58, 60 with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [λ, α′] of the wavelength λ and the angle of incidence α′ of the light, corresponding to a point in the parameter plane 55, lies in the efficiency window 65.
The straight line 57 is approximately an axis of symmetry of the efficiency window 65. Here, the straight line 57 approximately follows a line which passes through the efficiency window and on which the diffraction efficiency has a local maximum in a direction intersecting this line. That is, the efficiency window 65 extends approximately symmetrically along the straight line 57. In the present case, the efficiency window 65 has approximately mirror symmetry in relation to the straight line 57. In the present case, the following applies to the gradient δ of the straight line 57 in
The efficiency window 65 of a diffraction structure in a spectacle lens according to the invention has the form of an area surrounded by an elongate ellipse in the parameter plane 55. In the efficiency window 65, the light incident at a specific angle of incidence α on the spectacle lens 16, 18 is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1. Here, the efficiency window 65 of a diffraction structure lies between a first tangent 59 parallel to the increasing straight line 57 and a second tangent 61 parallel to the first tangent 59. In relation to the first tangent 59, the second tangent 61 is respectively displaced in parallel by the angle Δα≈3° in this case.
Here, the curve of an efficiency window 65 in the parameter plane 55 can be set by way of the thickness h of the volume grating VG of a diffraction structure, the spatial period of the volume grating VG, that is, the line density 1/Λ of the volume grating VG, and by the angle of inclination φ of the periodic grating planes 34 in relation to the object-side boundary 33 of a volume grating VG.
To this end, a transparent carrier 62 is provided in a first step. Then, a first transparent layer 66 made of a photopolymer is applied to a first side 64 of the transparent carrier 62 by means of spin coating, spinning-on or an application by doctoring and/or flat coating or a contact transfer of films.
Thereupon, a multiplicity of diffraction structures in the form of a spatial modulation of the complex refractive index are introduced in a subsequent step into the transparent layer 66 by exposure using a holographic method.
This is preferably carried out by the coherent superposition of light from a light source with the light from this light source reflected at a reference object or with the light from this light source after it has passed through a reference object. However, as an alternative thereto, it is also possible to impress corresponding diffraction structures into the matter, for example, point-by-point by means of a laser beam.
Thereafter, a further transparent layer 68 made of a photopolymer is applied to the layer 66 by means of spin coating or an application by doctoring. This layer is then likewise provided with diffraction structures, for example by way of the holographic method described above. Thereupon, the diffraction structures in the layer 68 are likewise stabilized. Then, a further transparent layer 70, in which diffraction structures are generated in turn, is applied onto the transparent layer 68, and so on.
After producing the layers 66, 68, 70, lying over one another, of an optically transparent material with diffraction structures formed therein on the side 64 of the transparent carrier 62, layers 72, 74, 76, lying over one another, of an optically transparent material with diffraction structures formed therein are produced in the same way on the other side 78 of the transparent carrier 62.
The apparatus 80 contains a light source, for example, a laser 82, which provides a laser beam 84. The laser beam 84 provided by the laser 82 is split into a first partial beam path 88 and a further partial beam path 90 by means of a beam splitter 86. Then, the partial beam path 88 is directed to the layer 66 by a focusing lens 92. The partial beam path 90 is guided, via a mirror 94, along the optical axis 100 through a focusing lens 96 and a lens element 98 and then coherently superposed on the partial beam path 88 on the layer 66 in an exposure region 67. Here, the focusing lens 92 can be linearly displaced in accordance with the double-headed arrow 99 and tilted about the axis 103 in accordance with the double-headed arrow 101 in order thereby to modify the distance a of the focusing lens 92 from the layer 66 and the angle φ between the optical axes of the partial beam paths 88, 90 interfering in the layer 66.
Thus, the apparatus 80 generates a hologram of the focusing lens 92 in the photopolymer of the layer 66. This hologram has an optical transfer function corresponding to the arrangement of the focusing lens 92. Hence, it is possible to set the spatial profile of the modulation of the complex refractive index in the layer 66 in a defined manner by modifying the interference angle φ, the tilt angle θ of the focusing lens 92, the tilt angle θ′ of the carrier 62 or the distance a of the focusing lens 92 from the layer 66. In this case, the period Λ of the generated diffraction structure approximately satisfies the following relationship: Λ˜sin φ/λ, where λ is the wavelength of the laser light provided by the laser 82. By the successive modulation of the refractive index in different regions of the layer 66, it is possible, in the layer 66, to generate various diffraction structures which are separated from one another in space or which overlap on one another and it is possible to set an optical transfer function for this layer. By the successive generation of holograms in layers 66, 68, 70, 72, 74, 76 made of a photopolymer and applied onto a carrier 62, it is thus possible to provide spectacles with a spectacle lens, the optical effect of which is determined by the diffraction of the light at the diffraction structures realized by means of the holograms in the layers lying one above the other.
It should be noted that it is also possible to use optical components or combinations of optical components in the apparatus 80 in place of the focusing lens 92 in
In order to establish the configuration of such an optical visual aid, an image surface 104 is predetermined in a first step. An object surface 106 and the position of the optical visual aid are defined in a further step. Then, in a subsequent step, an optical transfer function which images the object surface 106 into the image surface 104 in focus is predetermined for the visual aid. This optical transfer function is then approximated by calculating, with variation, the deflection of the light due to diffraction and, with variation, the diffraction efficiency.
The spectacle lens 112a of
The position of the visual zones 114, 116 in the spectacle lens 112a shown in
For the spectacle lens 112b in
In the spectacle lens 112c, 112d and 112e shown in
As the optical effect of the spectacle lenses 112a, 112b, 112c, 112d and 112e described above is set by means of the diffraction structures, these visual aids do not have regions with an astigmatic effect which is caused by the Minkwitz theorem, unlike conventional progressive lenses based on the refractive effect of a glass body for light.
It should be noted that the invention also extends to a spectacle lens in which combinations of features from different embodiments for diffraction structures, described above, can be found.
In conclusion, the following preferred features should, in particular, be retained: A spectacle lens 16, 18 for an observer comprises a body which is transparent or at least partly transparent to light and has a phase object 20 which guides the light incident at an angle of incidence α on the side distant from the observer into a direction depending on the wavelength λ of the light and the angle of incidence α of the light. The phase object 20 has a multiplicity of diffraction structures 24, 26, which diffract monochromatic light at a wavelength of 380 nm≦λ≦800 nm with a diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the monochromatic light is incident at an angle of incidence α on the side of the spectacle lens 16, 18 distant from the observer which lies within a diffraction-structure-specific angle interval which is 15° wide and depends on the wavelength of the light.
According to another embodiment of the invention, a spectacle lens (16, 18) for an observer, includes a body which is transparent or at least partly transparent to light and has a phase object (20) which guides the light incident at an angle of incidence α on a side of the spectacle lens distant from the observer into a direction depending on the wavelength λ of the light and the angle of incidence α of the light. The phase object (20) has a multiplicity of diffraction structures (24, 26, 56, 58, 60), which diffract monochromatic light at a wavelength of 380 nm≦λ≦800 nm with a diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the monochromatic light is incident at an angle of incidence α on the side of the spectacle lens distant from the observer which lies within a diffraction-structure-specific angle interval which is 15° wide and depends on the wavelength of the light.
Each diffraction structure (24, 26, 56, 58, 60) diffracts all light of a diffraction-structure-specific wavelength λ lying in a diffraction-structure-specific wavelength interval Δ0±0.1 μm, said wavelength being incident at an angle of incidence α which lies in a diffraction-structure-specific angle of incidence range α0±2.5° on the side of the spectacle lens distant from the observer, with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1.
The diffraction structures (24, 26, 56, 58, 60) in the parameter plane (55) spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis (51) and an angle of incidence parameter axis (53) each have an efficiency window (65) extending along a straight line (57), which increases monotonically in relation to the wavelength λ, in which efficiency window the light incident at a specific angle of incidence α on the side of the spectacle lens distant from the observer is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane (55), lies in the efficiency window (65).
The term δ≦0.036°/nm applies to the gradient δ of the straight line (57) or in that δ≦0.024°/nm applies to the gradient δ of the straight line (57) or in that δ≦0.012°/nm applies to the gradient δ of the straight line (57).
The diffraction structures (24, 26, 56, 58, 60) in the parameter plane (55) spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis (51) and an angle of incidence parameter axis (53) each have an efficiency window (65) extending along a straight line (57), which increases monotonically in relation to the wavelength λ, between a first tangent (59) parallel to the increasing straight line (57) and a second tangent (61) displaced in parallel to the first tangent (59) in the direction of the angle of incidence parameter axis (53) by the angle Δα≦20°, in which efficiency window the light incident at a specific angle of incidence α on the side of the spectacle lens distant from the observer is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane (55), lies in the efficiency window (65), or in that the diffraction structures (24, 26, 56, 58, 60) in the parameter plane (55) spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis (51) and an angle of incidence parameter axis (53) each have an efficiency window (65) extending along a straight line (57), which increases monotonically in relation to the wavelength λ, between a first tangent (59) parallel to the increasing straight line (57) and a second tangent (61) displaced in parallel to the first tangent (59) in the direction of the angle of incidence parameter axis (53) by the angle Δα≦15°, in which efficiency window the light incident at a specific angle of incidence α on the side of the spectacle lens distant from the observer is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane (55), lies in the efficiency window (65), or in that the diffraction structures (24, 26, 56, 58, 60) in the parameter plane (55) spanned by the angle of incidence α and the wavelength λ with a wavelength parameter axis (51) and an angle of incidence parameter axis (53) each have an efficiency window (65) extending along a straight line (57), which increases monotonically in relation to the wavelength λ, between a first tangent (59) parallel to the increasing straight line (57) and a second tangent (61) displaced in parallel to the first tangent (59) in the direction of the angle of incidence parameter axis (53) by the angle Δα≦10° or Δα≦6°, in which efficiency window the light incident at a specific angle of incidence α on the side of the spectacle lens distant from the observer is diffracted with the diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the parameter pair [α, λ] of the wavelength λ and the angle of incidence α of the light, corresponding to a point in the parameter plane (55), lies in the efficiency window (65).
The efficiency window (65) extends symmetrically along the straight line (57) and/or in that the straight line (57), along which the efficiency window (65) extends, approximately follows a line passing through the efficiency window (65) on which the diffraction efficiency η is at a maximum.
Each diffraction structure (24, 26) is embodied as a modulation of the complex refractive index n(λ; x,y,z):=nr(λ; x,y,z)+ini(λ; x,y,z) of the body in at least one spatial direction.
An amplitude Δn(λ) of the modulation of the complex refractive index n(λ; x,y,z) satisfies the following relationship for light of the wavelength 400 nm≦λ≦800 nm: 0.01≦|Δn(λ)|≦0.05.
Each diffraction structure (24) forms an actuator-compensator pair (31) with a further diffraction structure (26) which is spatially separate from the diffraction structure (24), wherein the deflections of the light incident on the side distant from the observer caused by the diffraction structures (24, 26) forming an actuator-compensator pair (31) are at least partly canceled, and/or in that the phase object (20) has an optical effect, in particular a lens effect, and/or in that the phase object comprises layers (66, 68, 70), lying one above the other, of an optically transparent material with a modulated refractive index, wherein the layers (66, 68, 70) lying one above the other are applied to a carrier (62) transparent to the visible light.
A light-refracting effect is present in addition to the light-diffracting effect. The optical effect thereof is dependent on a viewing direction, passing through the spectacle lens (112a, 112b, 112c, 112d, 112e), of the observer.
The body of the spectacle lens (112a, 112b, 112c, 112d, 112e) has an edge and two or more connected visual zones (114, 116) which have a different optical effect, extend over the body and at least partly cover the body in the process, wherein the body has no regions with an astigmatism caused by the Minkwitz theorem.
A method for establishing the design of a spectacle lens, in which a geometry and an optical transfer function are predetermined for the spectacle lens (102) provides that a phase object which has a multiplicity of diffraction structures is calculated for the predetermined optical transfer function and the predetermined geometry, which diffraction structures diffract monochromatic light at a wavelength of 380 nm≦λ≦800 nm with a diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the monochromatic light is incident at an angle of incidence α on the side of the spectacle lens distant from the observer which lies within a diffraction-structure-specific angle interval which is 15° wide and depends on the wavelength of the light, wherein the phase object has a diffractive effect f(θa) which, together with the refractive effect of the spectacle lens (102), at least approximates the predetermined optical transfer function.
The predetermined optical transfer function at least partly compensates at least one visual impairment of the observer.
A production method is provided for a spectacle lens including a transparent carrier (62), on which an optical layer (66) or a plurality of optical layers (66, 68, 70) are applied. In the production method, a transparent carrier (62) is provided; an optical layer (66) or a plurality of optical layers (66, 68, 70) made of a photopolymer are applied onto the transparent carrier (62); and, a hologram of an optical element (98) is arranged in a defined position in relation to the optical layer is generated in one optical layer (66, 68, 70). A phase object which has a multiplicity of diffraction structures is generated on the optical carrier (62) in the process, said phase object having a plurality of diffraction structures, which diffract monochromatic light at a wavelength of 380 nm≦λ≦800 nm with a diffraction efficiency of η≧70% into one and same order of diffraction |m|≧1 when the monochromatic light is incident at an angle of incidence α on the side of the spectacle lens distant from the observer which lies within a diffraction-structure-specific angle interval which is 15° wide and depends on the wavelength of the light.
It is understood that the foregoing description is that of the preferred embodiments of the invention and that various changes and modifications may be made thereto without departing from the spirit and scope of the invention as defined in the appended claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10 2014 209 792.4 | May 2014 | DE | national |
This application is a continuation application of international patent application PCT/EP2015/061476, filed May 22, 2015, designating the United States and claiming priority from German application 10 2014 209 792.4, filed May 22, 2014, and the entire content of both applications is incorporated herein by reference.
| Number | Date | Country | |
|---|---|---|---|
| Parent | PCT/EP2015/061476 | May 2015 | US |
| Child | 15359476 | US |
