TRIFOCAL ARTIFICIAL OPHTHALMIC LENS AND METHOD FOR ITS PRODUCTION

Abstract

The invention relates to a trifocal artificial ophthalmic lens (20), which contains an anterior side optical surface (21), a posterior side optical surface (22) and an optical axis (23), at least one of the anterior side optical surface (21) and the posterior side optical surface (22) contains an optics having three useful focal points and having an at least partially diffractive profile. The three useful focal points correspond to focal points (31, 32) belonging to the 0.sup.th and 1.sup.st diffraction orders of the diffractive profile, and to a focal point (33) belonging to an enhanced diffractive secondary peaks between the 0.sup.th and the 1.sup.st diffraction orders. The invention also relates to a method of producing the aforementioned trifocal artificial ophthalmic lens.

Claims

1. Trifocal artificial ophthalmic lens (20), which contains an anterior side optical surface (21), a posterior side optical surface (22) and an optical axis (23), at least one of the anterior side optical surface (21) and the posterior side optical surface (22) contains an optics having three useful focal points and having an at least partially diffractive profile, characterised by that the three useful focal points correspond to focal points (31, 32) belonging to the 0th and 1st diffraction orders of the diffractive profile, and to a focal point (33) belonging to an enhanced diffractive secondary peaks between the focal points (31, 32) belonging to the 0th and the 1st diffraction orders.

2. The artificial ophthalmic lens according to claim 1, characterised by that the secondary peaks are enhanced such that the maximum phase shift of a central zone (27) of the diffractive profile (25) is greater than λ/2, where the phase shift means the phase shift relative to a base defined by base points (30a) of the central zone of the diffractive profile (25).

3. The artificial ophthalmic lens according to claim 2, characterised by that the areas (29) between the zone boundaries of phase shifting zones (28) are identical in size, and a first arc linking the base points (30a) of the central zone (27) on the diffractive profile is selected so that an area (29′) delimited by a theoretical central zone (27′) having a second arc parallel with the first arc and having a maximum phase shift of λ/2, is the same as the areas (29) occupied by the individual phase shifting zones (28).

4. The artificial ophthalmic lens according claim 2, characterised by that the maximum phase shift of the central zone (27) is greater than λ/2 and smaller than λ.

5. The artificial ophthalmic lens according to claim 2, characterised by that the maximum phase shift of the central zone (27) is greater than λ/2 and smaller than or equal to 3/4λ.

6. The artificial ophthalmic lens according to claim 2, characterised by that the diffractive profile outside of the central zone (27) is apodized.

7. The artificial ophthalmic lens according to claim 2, characterised by that an peripheral, purely refractive portion is connected to the diffractive profile (25).

8. Method of producing a trifocal artificial ophthalmic lens (20), which artificial ophthalmic lens (20) contains (20) an anterior side optical surface (21), a posterior side optical surface (22) and an optical axis (23), at least one of the anterior side optical surface (21) and the posterior side optical surface (22) contains an optic optics having three useful focal points (for far, intermediate, and near vision) and having an at least partially diffractive profile, characterised by forming the diffractive profile so that the far vision focal point and the near vision focal point correspond to focal points (31, 32) belonging to the 0th and 1st diffraction orders of the diffractive profile, and the intermediate vision focal point corresponds to a focal point (33) belonging to an enhanced diffractive secondary peaks between the focal points (31, 32) belonging to the 0th and the 1st diffraction orders.

9. Method according to claim 8, characterised by enhancing the diffractive secondary peaks by creating a central zone (27) of the diffractive profile with a maximum phase shift greater than λ/2, where the phase shift means the phase shift relative to a base defined by base points (30a) of the diffractive profile.

10. Method according to claim 9, characterised by designing the diffractive profile starting from a bifocal theoretical diffractive profile, which has a theoretical central zone and theoretical phase shifting zones outside thereof, and a size of areas between zone boundaries of the theoretical phase shifting zones are is the same as a size of an area delimited by the theoretical central zone, and a maximum phase shift of the theoretical central zone is λ/2, and two useful focuses belonging to a 0th and a 1st diffraction orders of the theoretical diffractive profile substantially coincide with the focal points (31, 32) belonging to the 0th and 1st diffraction orders of the diffractive profile (25) of the artificial ophthalmic lens to be produced, and the method further comprising comprises increasing the central zone (27) of the diffractive profile (25) as compared to the theoretical central zone for the phase shift of the central zone to be greater than λ/2 in such a way that a first arc linking boundaries of the central zone (27) is maintained parallel to a second arc of the theoretical central zone, and the phase shifting zones (28) outside of the central zone are shifted in a direction perpendicular to the optical axis (23) as compared to the theoretical phase shifting zones in such a way that the area between the zone boundaries of the phase shifting zones (28) remains unchanged.

11. Method according to claim 9, characterised by providing the maximum phase shift of the central zone (27) is to be greater than λ/2 and smaller than λ.

12. Method according to claim 9, characterised by providing the maximum phase shift of the central zone (27) to fall within the range of 0.52λ to 0.8λ.

Description

BRIEF DESCRIPTION OF DRAWINGS

[0021] FIG. 1 depicts a schematic side view of an embodiment of the present invention.

[0022] FIG. 2 depicts the phase shift produced by a saw-tooth-type, non-apodized diffractive profile as a function of distance measured from the optical axis, where the maximum phase shift of the central zone is 5/8λ.

[0023] FIG. 3 also depicts the phase shift produced by a saw-tooth-type, non-apodized diffractive profile as a function of distance measured from the optical axis, where the maximum phase shift of the central zone is 3/4λ.

[0024] FIGS. 4 to 9 present the modulation transfer function (MTF) of the artificial ophthalmic lens containing the diffractive profile presented in FIGS. 2 and 3 as a function of distance measured from the focal point, at a spatial frequency of 50 lines/mm, but in the case of apertures of differing diameter, i.e. pupil size.

[0025] As the artificial ophthalmic lens described in the present invention may be an artificial lens implanted in the capsular bag, the ciliary sulcus or in the anterior chamber, or may be a contact lens, or an artificial lens that can be implanted in the cornea using an inlay or onlay technique, therefore the disclosed embodiments may be used at any of the aforementioned locations.

A DETAILED DESCRIPTION OF THE EMBODIMENTS ACCORDING TO THE INVENTION

[0026] FIG. 1 depicts a schematic side view of an embodiment of the present invention, in which it can be seen that the artificial ophthalmic lens 20 contains an anterior optical surface 21 and a posterior optical surface 22. The anterior optical surface 21 and the posterior optical surface 22 have a common optical axis 23, and the posterior optical surface 22 is formed as a multifocal optics 24 with a diffractive profile 25. The present embodiment is also provided with haptics 26, as an implantable artificial lens is depicted.

[0027] In a preferred embodiment the maximum phase shift of the central zone 27 of the diffractive profile 25 is greater than λ/2 and smaller than 3/4λ, where λ is the wavelength of the light for which the operation of the diffractive optical element is designed. FIG. 2 depicts a saw-tooth-type diffractive profile 25 as a function of distance measured from the optical axis 23, where the maximum phase shift of the central zone 27 is 5/8λ, where phase shift means the phase shift relative to the base defined by base points 30a of the diffractive profile. The diffractive profile 25 presented is non-apodized, in other words the heights of the phase shifting zones 28 outside of the central zone 27 are identical. The dashed line in the figure displays the original profile, while the solid line illustrates the modification according to the invention. The original profile displays the diffractive structure of a conventional bifocal lens known by itself, in the case of which the bifocality is ensured by that the maximum phase shift of the individual zones is λ/2, while the areas 29′ between the zone borders of the individual zones are of the same size, in other words the areas 29′ of the phase shifting zones 28′ outside the central zone 27′ of the original profile 27′ are the same as the area 29′ delimited by the central zone 27′, as is known from the literature by a person skilled in the art. The arc linking the base points 30a of the central zone 27 in the diffractive profile according to the invention (of which base points 30a only one is indicated) is parallel to the arc linking the base points 30a′ of the central zone 27′ of the original profile, and the areas 29 between the zone boundaries of the phase shifting zones 28 are of the same size as the area 29′ occupied by the central zone 27′ of the original profile.

[0028] FIG. 3 illustrates the phase shift of a saw-tooth-type, non-apodized diffractive profile 25 as a function of the distance measured from the optical axis 23, where the maximum phase shift of the central zone 27 is 3/4λ, where phase shift means the phase shift in relation to the base defined by the base points 30a of the diffractive profile. The dashed line in the figure shows the original (conventional bifocal) profile, while the solid line illustrates the modification according to the invention.

[0029] The remaining figures show the change of optical performance (modulation transfer function, MTF) belonging to the embodiments according to FIGS. 2 and 3 as compared to the optical performance of a conventional bifocal profile. The MTF curve belonging to the diffractive profile 25 according to the invention is shown with a solid line, and the MTF curve belonging to a conventional bifocal profile with a dashed line. The MTF curves illustrate how the imaging quality changes as the object distance changes. The MTF curves obtained at various apertures are determined by the depth of focus depending on the aperture diameter and on the intensity distribution together.

[0030] FIG. 4 shows the change of the optical performance of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 2, which is described by the modulation transfer function (MTF) as a function of distance measured from the point of focus, in the case of an aperture of 3.0 mm, and spatial frequency of 50 lines/mm.

[0031] FIG. 5 shows the change of the optical performance (MTF) of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 3 as a function of distance measured from the point of focus, in the case of an aperture of 3.0 mm, and spatial frequency of 50 lines/mm.

[0032] FIG. 6 shows the change of the optical performance (MTF) of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 2 as a function of distance measured from the point of focus, in the case of an aperture of 2.5 mm, and spatial frequency of 50 lines/mm.

[0033] FIG. 7 shows the change of the optical performance (MTF) of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 3 as a function of distance measured from the point of focus, in the case of an aperture of 2.5 mm, and spatial frequency of 50 lines/mm.

[0034] FIG. 8 shows the change of the optical performance (MTF) of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 2 as a function of distance measured from the point of focus, in the case of an aperture of 2.0 mm, and spatial frequency of 50 lines/mm.

[0035] FIG. 9 shows the change of the optical performance (MTF) of the artificial ophthalmic lens containing the diffractive profile 25 presented in FIG. 3 as a function of distance measured from the point of focus, in the case of an aperture of 2.0 mm, and spatial frequency of 50 lines/mm.

[0036] In the aforementioned FIGS. 4 to 9 it can be seen that the optical performance curves also have a local side maximum between the two main maxima, which can be enhanced to produce an intermediate (intermediate distance) vision focal point 33 as well, thereby making it possible to produce a trifocal optical element.

[0037] A possible way of enhancing the intermediate vision focal point 33 falling between the focal points 31, 32 belonging to the 0.sup.th and 1.sup.st diffraction orders of the artificial ophthalmic lens containing the diffractive profile is the enhancement of the side maxima of the 0.sup.th and 1.sup.st diffraction orders and simultaneously ensuring their constructive interference. The essence of the present invention is the production of a diffractive profile 25 that enhances the side maximum of the focal point 31 belonging to the 0.sup.th diffraction order and the side maximum the focal point 32 belonging to the 1.sup.st diffraction order and by simultaneously ensuring their constructive interference by increasing the maximum phase shift of the central zone 27 to above λ/2.

[0038] A possible method of increasing the phase shift of the central zone 27 of the diffractive profile 25 to above λ/2 is increasing the central zone 27 of the diffractive profile 25 in such a way that the arc connecting the boundaries of the central zone 27 remains unchanged and the phase shifting zones 28 outside of the central zone 27 are shifted, while the areas 29 between the zone boundaries of the phase shifting zones 28 (i.e. the areas of the rings determined by the base points 30b of the individual phase shifting zones 28) outside of the central zone 27 remain unchanged, in other words the additional dioptric power characteristic of the phase shifting zones 28 remains unchanged. In other words the area of the central zone 27 is increased as compared to the areas 29 of the phase shifting zones 28 outside of it, which remain unchanged and remain the same as in the case of conventional bifocal profiles. In other words the central zone 27 occupies a larger area than the individual phase shifting zones 28, however, the arc of the central zone 27 is the same as the arc of a theoretical central zone 27′ providing a phase shift of λ/2 and delimiting an area 29′ that is the same size as the area 29 of the individual phase shifting zones 28. The arcs of the central zone 27 and of the theoretical central zone 27′ are understood to mean arcs that run along the surface of the central zone 27 and along the surface of the theoretical central zone 27′, respectively, and intersect the optical axis linking two base points 30a and 30a′, respectively, (located on the opposite sides of the central zone 27 and the theoretical central zone 27′, respectively) that fall on a straight line passing through the optical axis via the shortest path.

[0039] The designing of the diffractive profile 25 according to the invention may also take place accordingly. The starting point is a theoretical conventional bifocal diffractive profile that has a theoretical central zone 27′ and theoretical phase shifting zones 28′ outside thereof, and the size of the areas 29′ between the zone boundaries of the theoretical phase shifting zones 28′ is the same as the size of the area 29′ delimited by the theoretical central zone 27′. In the case of the theoretical diffractive profile the phase shift of at least the theoretical central zone 27′ is λ/2, but in the present case the phase shift of every phase shifting zone 28′ of the initial theoretical diffractive profile is λ/2. The two useful focuses of the theoretical bifocal diffractive profile are selected so that the two useful focuses belonging to the 0.sup.th and the 1.sup.st diffraction order substantially coincide with the focal points 31, 32 belonging to the 0.sup.th and 1.sup.st diffraction orders of the diffractive profile 25 of the artificial ophthalmic lens to be produced (which focal points 31, 32 in the present case are a distant focus set to infinity and a near focus set to approx. 30 cm). Such a conventional bifocal diffractive profile can be designed easily based on design values taken from the prior art literature. As compared to the theoretical bifocal diffractive profile the phase shift of the central zone 27 is increased to above λ/2, while maintaining the arc linking the base points 30a of the central zone 27 unchanged, in other words the central zone 27 is increased in the direction perpendicular to the optical axis so that in the meantime the arc (passing through the optical axis) delimiting the central zone 27 and linking its base points 30a remains parallel to the arc linking the base points 30a′ (and passing through the optical axis) of the theoretical central zone 27′. In the meantime the phase shifting zones 28 outside of the central zone 27 are shifted in a direction perpendicular to the optical axis 23 in such a way that the areas 29 between the zone boundaries of the phase shifting zones 28 remain unchanged.

[0040] Comparing FIGS. 5, 7 and 9 with FIGS. 4, 6 and 8 it can be determined that the greater phase shift increase resulted in a more significant intermediate focus in the case of 3.0 and 2.5 mm apertures, and led to a significant extended depth of focus in the case of small pupil diameters, which effect did not appear at all in the case of conventional bifocal lenses. It was found that the intermediate distance focus and the extended depth of focus appearing in the case of small pupil diameters is especially significant in case the maximum phase shift of the central zone 27 is about 3/4λ, but an improvement over the conventional bifocal profile can be observed everywhere in case the maximum phase shift of the central zone 27 is greater than λ/2 and smaller than λ. Already at a maximum phase shift of a value of 0.52λ the effect is of such an extent that it provides an improvement in the optical performance of the lens perceived by the users. Preferably the maximum phase shift of the central zone 27 in the diffractive profile 25 falls within the range of 0.52λ-0.8λ, especially preferably in the range of 5/8λ and 3/4λ.

[0041] The performance of the present invention is not limited by the characteristics of the diffractive profile 25 outside of the central zone 27. The diffractive profile 25 outside of the central zone 27 may be apodized or non-apodized, an external, purely refractive area can also be attached to the diffractive profile 25. If the diffractive profile 25 outside of the central zone 27 is to be apodized, then in the design stage it is preferred to start from a theoretical bifocal diffractive profile wherein the maximum phase shift of the central zone 27′ continues to be λ/2, but the theoretical phase shifting zones 28′ outside of the central zone 27′ are apodized, in other words their maximum phase shift is varying (increasing or decreasing).

[0042] On the basis of the present invention a diffractive profile may also be realised that creates a lens with trifocal optical performance by enhancing a side maximum occurring between any two consecutive diffractive orders (such as the +1.sup.st and +2nd orders).

[0043] A further advantage of the present invention is that in addition to trifocal optical performance, the artificial ophthalmic lens comprising the diffractive profile 25 presented in the figures also ensures extended depth of focus optical performance in the case of small pupil diameters occurring in photopic conditions (through-focus curves measured in the case of a 2.0 mm aperture), as can be observed in FIGS. 8 and 9.