Intraocular lens
Provided are an intraocular lens and a technique associated therewith, wherein an average value (exceeding 0 D) of base difference values within a first region from a lens center O to a position r1 of a first boundary is greater than 5 times an average value (exceeding 0 D) of base difference values within the first region from a lens center O of a virtual spherical lens having a base power at the lens center O to the position r1, a second region has a power resulting from adding one or more positive constant powers to a reference aspheric power, in a third region, the power is reduced so as to provide a negative longitudinal spherical aberration that cancels at least part of a positive longitudinal spherical aberration caused by a cornea, and a second step value is greater than a first step value.
1. An intraocular lens comprising
at least three visual acuity correction regions that are concentric with a lens center O at which a predetermined base power is set, and that are adjacent to each other,
wherein the visual acuity correction regions are set as a first region including the lens center O, and a second region and a third region disposed in this order radially from the first region,
when r1 is a position of a first boundary between the first region and the second region, and r2 is a position of a second boundary between the second region and the third region, as viewed radially from the lens center O,
the first region is a region for correcting a visual acuity for far vision or a visual acuity for vision between far vision and intermediate vision,
the second region is a region for correcting a visual acuity for intermediate vision or a visual acuity for near vision,
the third region is a region for correcting the visual acuity for far vision,
a change in power is discontinuous on the first boundary and the second boundary,
a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1Low of the first region on the first boundary is less than 50% of a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1High of the second region on the first boundary,
an average value (exceeding 0 D) of the base difference values within the first region from the lens center O to the position r1 of the first boundary is greater than 5 times an average value (exceeding 0 D) of the base difference values within the first region from a lens center O of a virtual spherical lens having a base power at the lens center O to the position r1,
the second region has a power resulting from adding one or more positive constant powers to a reference aspheric power, in an area from the position r1 to the position r2, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea,
the power is reduced in the third region so as to provide a negative longitudinal spherical aberration that cancels at least part of the positive longitudinal spherical aberration caused by the cornea,
a second step value constituted by a value obtained by subtracting a power P B2Low of the third region from a power P B2High of the second region on the second boundary is greater than a first step value constituted by a value obtained by subtracting the power P B1Low of the first region from the power P B1High of the second region on the first boundary, and
the power P B2High of the second region on the second boundary is greater than the base power, and the power P B2Low of the third region on the second boundary is less than the base power.
2. The intraocular lens according to claim 1 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
3. An intraocular lens comprising
at least three visual acuity correction regions that are concentric with a lens center O at which a predetermined base power is set, and that are adjacent to each other,
wherein the visual acuity correction regions are set as a first region including the lens center O, and a second region and a third region disposed in this order radially from the first region,
when r1 is a position of a first boundary between the first region and the second region, r2 is a position of a second boundary between the second region and the third region, and r3 is a position of an outermost edge of the third region, as viewed radially from the lens center O,
the first region is a region for correcting a visual acuity for far vision or a visual acuity for vision between far vision and intermediate vision,
the second region is a region for correcting a visual acuity for intermediate vision or a visual acuity for near vision,
the third region is a region for correcting the visual acuity for far vision,
a change in power is discontinuous on the first boundary and the second boundary,
a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1Low of the first region on the first boundary is less than 50% of a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1High of the second region on the first boundary,
an average value (exceeding 0 D) of the base difference values within the first region from the lens center O to the position r1 of the first boundary is greater than 5 times an average value (exceeding 0 D) of the base difference values within the first region from a lens center O of a virtual spherical lens having a base power at the lens center O from to the position r1,
a power P B2High of the second region on the second boundary is greater than the base power, and a power P B2Low of the third region on the second boundary is less than the base power, and
the first region, the second region, and the third region are shaped such that a total power T obtained by summing up a refractive power of the cornea and a power of the intraocular lens increases in an area from the lens center O to the position r1 of the first boundary, the total power T is equal to a total power T o at the lens center O in an area from the position r2 of the second boundary to the position r3 of the outermost edge of the third region, and the total power T is equal to a value resulting from adding one or more positive constant powers to the total power T o in an area from the position r1 of the first boundary to the position r2 of the second boundary.
4. The intraocular lens according to claim 3 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
5. An intraocular lens comprising
at least three visual acuity correction regions that are concentric with a lens center O at which a predetermined base power is set, and that are adjacent to each other,
wherein the visual acuity correction regions are set as a first region including the lens center O, and a second region and a third region disposed in this order radially from the first region,
when r1 is a position of a first boundary between the first region and the second region, and r2 is a position of a second boundary between the second region and the third region, as viewed radially from the lens center O,
the first region is a region for correcting a visual acuity for far vision or a visual acuity for vision between far vision and intermediate vision,
the second region is a region for correcting a visual acuity for intermediate vision or a visual acuity for near vision,
the third region is a region for correcting the visual acuity for far vision,
a change in power is discontinuous on the first boundary and the second boundary,
a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1Low of the first region on the first boundary is less than 50% of a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1High of the second region on the first boundary,
an average value (exceeding 0 D) of the base difference values within the first region from the lens center O to the position r1 of the first boundary is greater than 5 times an average value (exceeding 0 D) of the base difference values within the first region from a lens center O of a virtual spherical lens having a base power at the lens center O to the position r1,
a power P B2High of the second region on the second boundary is greater than the base power, and a power P B2Low of the third region on the second boundary is less than the base power, and
the first region and the second region are sized such that, assuming that all light rays for a spatial frequency of 50 line pairs/mm pass through a virtual cornea and the intraocular lens,
a depth of focus is substantially the same as or deeper than a depth of focus of the virtual spherical lens for an aperture diameter of 2.5 mm or less,
a depth of focus is at least 10% deeper than the depth of focus of the virtual spherical lens for an aperture diameter of 3 to 4 mm, and
a contrast peak is present at a defocus value in a range from −0.25 D to 0.25 D for an aperture diameter of 5 mm or more.
6. The intraocular lens according to claim 5 ,
wherein the second region has a power resulting from adding one or more positive constant powers to a reference aspheric power, in an area from the position r1 to the position r2, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
7. The intraocular lens according to claim 6 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
8. The intraocular lens according to claim 5 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
9. An intraocular lens comprising
at least three visual acuity correction regions that are concentric with a lens center O at which a predetermined base power is set, and that are adjacent to each other,
wherein the visual acuity correction regions are set as a first region including the lens center O, and a second region and a third region disposed in this order radially from the first region,
when r1 is a position of a first boundary between the first region and the second region, and r2 is a position of a second boundary between the second region and the third region, as viewed radially from the lens center O,
the first region is a region for correcting a visual acuity for far vision or a visual acuity for vision between far vision and intermediate vision,
the second region is a region for correcting a visual acuity for intermediate vision or a visual acuity for near vision,
the third region is a region for correcting the visual acuity for far vision,
a change in power is discontinuous on the first boundary and the second boundary,
a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1Low of the first region on the first boundary is less than 50% of a base difference value (exceeding 0 D) obtained by subtracting the base power from a power P B1High of the second region on the first boundary,
an average value (exceeding 0 D) of the base difference values within the first region from the lens center O to the position r1 of the first boundary is greater than 5 times an average value (exceeding 0 D) of the base difference values within the first region from a lens center O of a virtual spherical lens having a base power at the lens center O to the position r1,
a power P B2High of the second region on the second boundary is greater than the base power, and a power P B2Low of the third region on the second boundary is less than the base power, and
the power is reduced in the third region so as to provide a negative longitudinal spherical aberration that cancels at least part of a positive longitudinal spherical aberration caused by a cornea,
a sag value of an anterior surface, a sag value of a posterior surface, or sag values of both the anterior surface and the posterior surface of the intraocular lens are represented by the following polynomial equation:
z
=
cr
2
1
+
1
-
(
1
+
k
)
c
2
r
2
+
a
1
r
2
+
a
2
r
4
+
a
3
r
6
+
a
4
r
8
+
…
+
a
n
r
2
n
[
Math
.
1
]
Z: sag value
c: curvature of lens center (=1/R[m])
k: conic constant
r: distance from lens center, i.e., radius
a 1 , a 2 , . . . , a n-1 , a n : coefficient
the power of each of the regions is represented by the following polynomial equation:
P i =c 0,i +c 1,i r 1 +c 2,i r 2 +c 3,i r 3 +c 4,i r 4 + . . . +c n,i r n [Math. 2]
P i : power of i-th region
r: distance from lens center, i.e., radius
c 0,i , c 1,i , . . . , c n-1,i , c n,i : coefficient
the power of the second region is represented by the following equation:
P 2 =A+P 3 [Math. 3]
P 2 : power of second region
P 3 : power of third region
A: addition power relative to reference aspheric power
A is a value obtained by subtracting, from the power of the second region at a predetermined position r within the second region, a reference aspheric power, at the position r, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of the positive longitudinal spherical aberration caused by the cornea, and
the power of the third region is represented by the following polynomial equation:
P 3 =c 0,3 +c 1,3 r 1 +c 2,3 r 2 +c 3,3 r 3 +c 4,3 r 4 + . . . +c n,3 r n [Math. 4]
P 3 : power of third region
r: distance from lens center, i.e., radius
c 0,3 c 1,3 . . . , c n-1,3 c n,3 : coefficient.
10. The intraocular lens according to claim 9 ,
wherein, in an area from the position r1 of the first boundary to the position r2 of the second boundary, a total power T obtained by summing up the refractive power of the cornea and the power of the intraocular lens is constituted by one or more constant values, and a visual acuity when viewing an object at one or more distances from an intermediate vision distance to a near vision distance is corrected using the total power T.
11. The intraocular lens according to claim 10 ,
wherein the second region has a power resulting from adding one or more positive constant powers to a reference aspheric power, in an area from the position r1 to the position r2, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
12. The intraocular lens according to claim 11 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
13. The intraocular lens according to claim 10 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
14. The intraocular lens according to claim 9 ,
wherein the second region has a power resulting from adding one or more positive constant powers to a reference aspheric power, in an area from the position r1 to the position r2, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
15. The intraocular lens according to claim 14 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.
16. The intraocular lens according to claim 9 ,
wherein an area from the position r2 of the second boundary to a position r3 of an outermost edge of the third region as viewed radially from the lens center O has a power equal to a reference aspheric power, from the position r2 to the position r3, of a virtual aspheric lens that has a base power at the lens center O, and that cancels the whole of a positive longitudinal spherical aberration caused by a cornea.