TWI555522B - An extended depth of focus (edof) lens to increase pseudo-accommodation by utilizing pupil dynamics - Google Patents

Description

Use of pupil dynamics to enhance pseudo-adjusted extended depth of focus (EDOF) crystals (1) Related application

The present invention is related to U.S. Patent Application entitled "Accommodative IOL with Toric Optic and Extended Depth of Focus," which is hereby incorporated by reference. This application is incorporated herein by reference.

Field of invention

The present invention relates to extended depth of focus (EDOF) crystals that utilize pseudo dynamics to enhance pseudo adjustment.

Background of the invention

The present invention relates generally to ophthalmic crystals and, more particularly, to artificial hydrocrystals that provide enhanced vision via controlled changes in phase shift across a transition region provided on at least one of the surfaces of the crystals ( IOL).

Artificial water crystals (IOL) are typically implanted into the patient's eye during cataract surgery to replace natural crystals. Under the influence of the ciliary muscles, The optical power of the natural crystallite can be varied to provide an accommodation power to view the object from the eye at different distances. However, many IOLs provide a single focus capability that does not require adjustment power. It is also known that multi-focus IOLs can provide both long-range optical power as well as near-field optical power (eg, by using a diffractive structure) to obtain a pseudo-regulating force.

There remains a need, however, for an improved IOL that provides false adjustment of optical power and provides a clear light image over a wide range of pupil sizes. In general, when designing an IOL and a crystal, the optical properties can be measured by using a so-called "model eye" or by a calculation method such as a predictive ray tracing method. Typically, such assays and calculations are performed based on light from a narrow specific region of the visible spectrum from which the pigment is minimized. This narrow area is commonly referred to as the "design wavelength."

Summary of invention

In one aspect of the invention, there is provided an ophthalmic hydrocell (e.g., an IOL) comprising a light member having a front surface and a rear surface disposed adjacent the optical axis. At least one of the surfaces (e.g., the front surface) has a contour that represents a feature by overlapping the base contour and the auxiliary contour. The auxiliary profile may include at least two regions (eg, an inner region and an outer region) and a transition region between the regions, wherein an optical path difference across the transition region (ie, within the transition region and outer radial direction) The optical path difference between the boundaries is equivalent to a non-integer fraction of the design wavelength (eg, a wavelength of about 550 nm) (example 1⁄2).

The transition region of the auxiliary profile may extend from an inner radial boundary to an outer radial boundary. In many embodiments, the inner radial boundary of the transition region corresponds to a radial boundary outside the inner region, and the radial boundary outside the transition region Corresponds to the inner radial boundary of the area outside the auxiliary contour. In many embodiments, the transition region is adapted to monotonically vary the optical path difference relative to a radial boundary within the transition region that is a variable radial distance from the optical axis. The characteristic of a monotonous change in the optical path difference can be represented by a continuous increase or decrease in the radial distance as a variable, which in some cases is a region where no change is present (high hill region). By way of example, the characteristics of the monotonic change can be represented by a linear change or by the continuous occurrence of a linear change separated by one or more high hills.

In some embodiments, the contour (Z _sag ) of the surface formed by the superposition of the base contour and the auxiliary contour can be defined by the following relationship: Z _sag = Z _base + Z _aux , where: Z _sag indicates The drop in surface relative to the optical axis is a function of the radial distance from the optical axis, and wherein: Where: r represents the radial distance from the optical axis, c represents the fundamental curvature of the surface, k represents the conic constant; a ₂ is the second-order deformation constant, a ₄ is the fourth-order deformation constant, and a ₆ is the sixth-order Deformation constant, and where: Where: r ₁ represents the radial boundary within the transition region, r ₂ represents the radial boundary outside the transition region, and wherein: Δ is defined by the following relationship: Wherein: n ₁ represents the refractive index of the material forming the optical member, n ₂ represents the refractive index of the medium surrounding the optical member, λ represents the design wavelength (for example, 550 nm), and α represents a non-integer fraction (for example, 1⁄2).

In certain other embodiments, the contour (Z _sag ) of the surface of the crystal having the auxiliary profile can be defined by the following relationship: Z _sag = Z _base + Z _aux where: Z _sag indicates the surface relative to the optical axis The drop is a function of the radial distance from the optical axis, and where: Wherein: r for the radial distance from the optical axis, c denotes curvature of the surface of the base, k is the conic constant; a ₂ is a second order deformation constant, a ₄ is a fourth order deformation constant, a ₆ is a sixth order Deformation constant, and where: Where: r represents the radial distance from the optical axis of the crystal, r _1a represents the inner diameter of the first substantially linear portion of the transition region of the auxiliary contour; r _1b represents the outer diameter of the first linear portion, r _2a represents the inner diameter of the second substantially linear portion of the transition region of the auxiliary profile, and r _2b represents the outer diameter of the second linear portion, and wherein Δ ₁ and Δ _{2 are} each defined according to the following relationship : Wherein: n ₁ represents the refractive index of the material forming the optical member, n ₂ represents the refractive index of the medium surrounding the optical member, λ represents the design wavelength (for example, 550 nm), and α ₁ represents a non-integer fraction (for example, 1⁄2), And α ₂ represents a non-integer fraction (for example, 1⁄2).

By way of example, in the above relationship, the basic curvature c may be in the range of about 0.0152 mm ^-1 to about 0.0659 mm ^-1 , and the conic constant k may be in the range of about -1162 to about -19, a ₂ may be from about -0.00032 mm ^-1 to about 0.0 mm in the range of ^-1, a ₄ may range from about 0.0 mm ^{to 3} to about -0.000053 (-5.3 × 10 ^-5) mm ^-3 of, and a ₆ It may range from about 0.0 mm ^{to 5} to about 0.000153 (1.53 × 10 ^-4) of ^-5 mm.

In another aspect, an ophthalmic hydrocrystal (e.g., an IOL) comprising a light member having a front surface and a rear surface disposed adjacent the optical axis is disclosed. At least one of the surfaces includes at least one inner refractive region, at least one outer refractive region, and a refractive transition region extending from a radial boundary outside the inner region to a radially inner boundary of the outer region. The transition region can be adjusted such that at a design wavelength (e.g., 550 nm), the radiation phase incident thereon can monotonically vary between the inner radial boundary and the outer radial boundary to be between the boundaries A phase shift is generated that represents a feature by a non-integer fraction of the design wavelength. Although in some cases the non-integer fraction is less than 1, in other cases it is greater than one.

In certain embodiments, the front and rear surfaces have a base profile adapted to impart a nominal refractive power to the crystal, such as a power in the range of from about -15 to about +50 diopters.

In a related aspect, the surface having the transition region can have The radial diameter is in the range of from about 1 mm to about 5 mm, and the transition region can be in the form of an annular region having a radial extent in the range of from about 0 to about 1 mm.

In another aspect, in the ophthalmic crystal of the above, the light member has a through-focus that is asymmetrical with respect to a focal plane of the light member in a range of apertures ranging from about 1.5 mm to about 6 mm. Modulation transfer function.

In another aspect, an ophthalmic hydrocele (e.g., an IOL) is disclosed that includes a light member having a front surface and a rear surface disposed adjacent the optical axis, wherein each surface includes a base surface contour. A pattern of surface variations is superimposed on a base surface contour of at least one of the surfaces to create a transition region extending between the inner and outer surface regions. The transition region may cause the optical member to have an asymmetric cross-in incidence of light (e.g., light having a design wavelength (e.g., 550 nm)) into the optical member via an aperture having a diameter in the range of from about 1.5 mm to about 6 mm. Focal modulation transfer function.

In certain embodiments, the above-described crystallites can have from about 0.25 diopters to about 1.75 of light (in terms of the design wavelength) suitable for injection through the aperture having a diameter in the range of from about 1.5 mm to about 6 mm. Depth of field in the range of diopter.

In certain embodiments, the above-described crystallites may have a substantially symmetric transfocal transfer transfer function suitable for light incident on the light member at a design wavelength via an aperture having a diameter of less than about 2 millimeters, and Asymmetric transfocus modulation transfer function for larger apertures. In some cases, the light member is adapted to pass through a diameter having a diameter in the range of from about 1.5 mm to about 6 mm. The depth of field of view of the light incident in the aperture (in terms of the design wavelength) in the range of from about 0.25 D to about 1.75 D.

In another aspect, the present invention provides an ophthalmic crystal (eg, an IOL) comprising a light member having a front surface and a back surface, wherein each surface has a contour that enables the light member to obtain a nominal optical power The basic outline. At least one of the surfaces has a contour defined by the addition of an auxiliary surface profile to its nominal surface profile, wherein the auxiliary profile is by a central region, an outer region, and a transition region extending between the inner and outer regions. Represents a feature. The auxiliary profile can be adjusted to produce a phase shift between the effective optical power and the nominal optical power suitable for having a design wavelength and incident on the light member via an aperture having a size within a predetermined range, such as at about Phase shift from 0.25D to about 1.75D. The effective optical power can be characterized by a spike of a trans-focus modulation transfer function of the optical component at the design wavelength and aperture.

In a related aspect, in the above-described crystal, the auxiliary contour is adapted to enhance the depth of field of the light member.

In another aspect, an ophthalmic crystal (e.g., an IOL) is disclosed that includes a light member having a front surface and a rear surface disposed adjacent the optical axis. At least one of the surfaces includes at least one inner refractive region and at least one outer refractive region, wherein the contour of the surface is configured to cause incident radiation from an outer boundary of the inner region to an inner boundary of the outer region (eg, at a design wavelength) The next incident radiation) results in a monotonically varying phase shift to obtain a phase shift within the two boundaries, which is a non-integer fraction of a design wavelength (eg, 550 nm). In some cases, the surface profile can be configured from about 0.75 mm to about 2.5 nm. A phase shift occurs within the radial distance of the circumference. Moreover, in some cases, the phase shift can extend the depth of focus displayed by the optical member to a value in the range of about 0.25D to about 1.75D.

In a related aspect, the radial derivative of the contour of the surface exhibits discontinuity below the outer boundary of the inner region.

The invention may be further understood by reference to the following embodiments and the accompanying drawings.

1,2‧‧‧Fixed components

10,24‧‧‧Artificial Crystals (IOL)

12,26‧‧‧Lights

14,28‧‧‧ front surface

16,30‧‧‧Back surface

18‧‧‧Inside refraction area

20‧‧‧Outer annular refractive area

22‧‧‧Circular transition zone

32‧‧‧ Flat central area

34‧‧‧flat outer area

36‧‧‧Transition area

36a, 36c‧‧‧ linear change

36b‧‧‧High Hill Area

Radial boundary within IB‧‧

OA‧‧‧ optical axis

OB‧‧‧ outer radial boundary

r ₁ ‧‧‧ Radial boundary within the transition zone

r ₂ ‧‧‧ Radial boundary outside the transition zone

r _1a ‧‧‧ indicates the inner diameter of the first substantially linear portion of the transition region of the auxiliary profile

r _1b ‧‧‧ indicates the outer diameter of the first linear part

r _2a ‧‧‧ indicates the inner diameter of the second substantially linear portion of the transition region of the auxiliary profile

r _2b ‧‧‧ indicates the outer diameter of the second linear part

△‧‧‧ is defined by Eq.(5)

△ ₁ , △ ₂ ‧‧‧ is defined by Eq. (8)

1A is a schematic cross-sectional view of an IOL in accordance with an embodiment of the present invention.

Figure 1B is a schematic top plan view of the front surface of the IOL shown in Figure 1A.

2A is a diagrammatic depicting the phase promotion induced in the wavefront incident on the surface of the lens in accordance with an embodiment of the present invention by a transition region provided on the surface in accordance with the teachings of the present invention. .

2B is a graphical depiction of the phase delay induced in the wavefront incident on the surface of the crystal crystal in a practice according to an embodiment of the present invention, via a transition region provided on the surface in accordance with the teachings of the present invention. .

Figure 3 is a graphical representation of the contour of at least one surface of a crystallite according to an embodiment of the invention, which may be characterized by the superposition of a base profile and an auxiliary profile.

4A-4C provides a hypothetical MTF graph for calculating a hypothetical crystal for use in different pupil sizes in accordance with an embodiment of the present invention.

5A-5F provide a calculated cross-focus MTF graph for a hypothetical crystal according to certain embodiments of the present invention, wherein each crystal has a base profile and an auxiliary profile that can define a transition region. A surface of a feature in which different optical path differences (OPD) within the other crystals provide different OPDs between the inner and outer regions of the auxiliary contour.

Figure 6 is a schematic cross-sectional view of an IOL in accordance with another embodiment of the present invention.

Figure 7 is a graphical representation depicting the contour of the front surface as a superposition of the base contour and the auxiliary contour including the double step transition region, and Figure 8 represents a double step transition region for use in accordance with an embodiment of the present invention. The hypothetical crystal is calculated to calculate the measured trans-focus monochrome MTF chart.

A detailed description

The present invention is generally directed to ophthalmic crystals (such as IOLs) and methods of using such crystals to correct vision. In the following examples, salient features of different aspects of the invention relating to artificial water crystals (IOL) are discussed. The teachings of the present invention are also applicable to other ophthalmic crystals, such as contact lenses. The term "artificial crystal" and its abbreviation "IOL" are used interchangeably herein to describe the interior of an implantable eye to replace the natural crystal of the eye or to enhance vision, whether or not the natural crystal is removed. Intracorneal crystals and phakic intraocular lenses are examples of artificial water crystals that can be implanted into the eye without removing natural crystals. in In many embodiments, the crystallite can include a controlled pattern of surface modulation that selectively produces an optical path difference between the inner and outer portions of the optical member of the crystal, whereby the crystal can provide a small and large pupil Clear image of diameter and pseudo-adjustment for viewing objects in the diameter of the middle pupil.

1A and 1B graphically depict an artificial water crystal (IOL) 10 including an optical member 12 having a front surface 14 and a rear surface 16 disposed adjacent the optical axis OA, in accordance with an embodiment of the present invention. As shown in FIG. 1B, the front surface 14 includes an inner refractive region 18, an outer annular refractive region 20, and an annular transition region 22 extending between the inner and outer refractive regions. The rear surface 16 is in the form of a flat convex surface. In some embodiments, the light member 12 can have a diameter D in the range of from about 1 mm to about 5 mm, although other diameters can be used.

The representative IOL 10 also includes one or more fixation members 1 and 2 (e.g., haptics) that can assist in placement within the eye.

In this embodiment, the front and rear surfaces each comprise a convex base profile, but in other embodiments a concave or flat base profile may be used. As discussed further below, although the contour of the back surface is defined by only a base contour, the contour of the front surface is defined by the addition of an auxiliary contour to its base contour to create the inner, outer and transition regions described above. The base profile of the two surfaces together with the refractive index of the material from which the optical member is formed may provide the optical member with a nominal optical power defined by an auxiliary profile other than the front surface free A single focus refractive power of a generally identified optical member formed from the same material of the same basic profile of the front and back surfaces. The nominal optical power of the optical member can also be considered to have a less than The single-focus refractive power of the small aperture optical member 12 having the diameter of the diameter of the central portion of the front surface.

The auxiliary profile of the front surface can adjust the nominal optical power, such as, for example, the peak axial position of the trans-focusing transfer function of the optical component calculated or measured at a design wavelength (eg, 550 nm) The actual optical power of the optical component, represented by the length of focus, may deviate from the nominal optical power of the crystal, particularly in terms of apertures (bores) in the medium range as further described below. In many embodiments, the change in optical power is designed to improve near vision for a pupil size. In some cases, the nominal optical power of the optical member can range from about -15D to about +50D, and preferably ranges from about 6D to about 34D. Moreover, in some cases, the change in standard optical power of the optical component caused by the auxiliary profile of the front surface may range from about 0.25 D to about 2.5 D.

With continued reference to Figures 1A and 1B, the transition region 22 is in the form of an annular region radially from the inner radial boundary (IB) (which in this case corresponds to the radial boundary outside the inner refractive region 18) Extending to the outer radial boundary (OB) (which in this case corresponds to the inner radial boundary of the outer refractive region). Although in some cases one or both boundaries may include discontinuities (e.g., a step) within the contour of the front surface, in many embodiments, the boundary of the contour of the front surface is continuous, but the path of the contour The number of guides (i.e., the rate of change of surface sag as a function of the radial distance from the optical axis) can exhibit a discontinuity at each boundary. In some cases, the transition region may have an annular width in the range of from about 0.75 mm to about 2.5 mm. In some cases, the ratio of the annular width of the transition region to the radial diameter of the front surface may It is in the range of from about 0 to about 0.2.

In many embodiments, the transition region 22 of the front surface 14 can be shaped such that the phase of the radiation incident thereon can vary monotonically between its inner boundary (IB) and outer boundary (OB). That is, the phase may be progressively increased or progressively decreased by increasing the incremental radial distance from the optical distance across the transition region to obtain a non-zero phase difference between the outer region and the inner region. In some embodiments, the transition region can include a high hill portion that is interspersed between the phase portions of the progressive increase or decrease, wherein the phase can remain substantially constant.

In many embodiments, the transition region is configured to cause a phase shift between two parallel rays, one of which is incident outside the transition region and the other of which is incident within the boundary of the transition region. Is a non-integer rational fraction of a design wavelength (eg, a design wavelength of 550 nm). By way of example, this phase shift can be defined according to the following relationship: OPD=(A+B)λ E _q (1B) where: A represents an integer, B represents a non-integer rational fraction, and λ represents a design wavelength (eg, 550 nm).

By way of example, the total phase shift across the transition region can be , Etc., where λ represents the design wavelength, for example 550 nm. In many embodiments, the phase shift can be a periodic function of the wavelength of the incident radiation, where the periodicity corresponds to a wavelength.

In many embodiments, the transition region can result in distortion of the wavefront from which the optical element responds to incident radiation (ie, the wavefront appearing from the surface behind the light member), which can be made relative to its nominal The effective focusing power of the crystal of the focusing force changes. Moreover, the distortion of the wavefront can enhance the aperture diameter for use in including the transition region, particularly for the depth of focus of a light member having a diameter aperture as discussed further below. For example, the transition region may cause a phase shift between a wavefront appearing from a portion other than the light member and a wavefront appearing from within the light member. Such a phase shift may cause radiation from the light member to interfere with radiation occurring from an internal portion of the light member, the interference position being that the radiation emerging from the internal portion of the light may be focused, and thus may be enhanced, for example, by The highest MTF-related asymmetric MTF (modulation transfer function) profile represents the position of the focal depth of the feature. The terms "depth of focus" and "depth of field of view" are used interchangeably and are known to be familiar to those skilled in the art when they refer to the distance of objects and image spaces on which images can be resolved. . Any further explanation is required to the extent that the depth of focus may refer to the peak of the transfocus modulation transfer function (MTF) of the crystallite measured relative to a 3 mm aperture and green light (eg, light having a wavelength of about 550 nm). The degree of defocusing, where at a spatial frequency of about 50 lines/mm (lp/mm), the MTF exhibits a degree of contrast of at least about 15%. Other definitions are also applicable and it should be understood that the depth of field can be affected by a number of factors including, for example, the size of the aperture, the amount of light that forms the image, and the underlying capabilities of the crystal itself.

As a further clarification, Figure 2A shows the borrowing in a graphical manner. a segment having a wavefront generated by a transition region between an inner portion and an outer portion of the surface and a front surface of the IOL according to an embodiment of the present invention, and a segment of the wavefront incident on the surface, and The reference spherical wavefront (indicated by the dashed line) that minimizes the RMS (square root) error of the actual wavefront. The transition region may result in a phase advancement of the wavefront (relative to a phase shift corresponding to a putative similar surface that does not contain the transition region), which may be in front of the retinal plane (in the absence of the transition region, at the nominal of the IOL) The focus plane of the front of the focus plane converges on the wavefront. 2B is a graphical representation of a focal plane in which the transition region may cause a phase delay of the incident wavefront, which may be outside the retinal plane (in the absence of the transition region, outside the nominal focal plane of the IOL) Converging the wavefront.

As an illustration, in this practice, the basic outline of the front and/or back surface can be defined by the following relationship: Where: c represents the curvature of the contour, k represents the conic constant, and wherein: f(r ² , r ⁴ , r ⁶ , ...) represents a higher order function constituting the base contour. By way of example, the function f can be defined by the following relation: f ( r ² , r ⁴ , r ⁶ ,...)= a ₂ r ² + a ₄ r ⁴ + a ₆ r ⁶ +... Eq (3) where: a ₂ is the second-order deformation constant, a ₄ is the fourth-order deformation constant, and a ₆ is the sixth-order deformation constant, and may include another higher-order term.

By way of example, in some embodiments, the parameter c can range from about 0.0152 mm ^-1 to about 0.0659 mm ^-1 within the range, the parameter k can be in the range from about -1162 to about -19, a ₂ may be about within ¹ to about 0.0 mm -0.00032 mm ^-1, a ₄ may range from about 0.0 mm to ³ mm ^-1 to about -0.000053 (-5.3 × 10 ^-5), and a ₆ may be about 0.0 mm ^{- 5} to about 0.000153 (1.53 × 10 ^-4 ) mm ^-5 range.

The use of a certain degree of asphericity within the front and/or rear base contour of the feature, for example by the conic constant k, can improve the spherical aberration effect of the large aperture size. In terms of large pore size, such asphericity can offset the optical effect of the transition region to some extent, so that a clearer MTF can be obtained. In certain other embodiments, the base contour of one or both surfaces may be toric (i.e., it may exhibit different bend radii along two orthogonal directions of the surfaces) to improve astigmatic aberrations.

As described above, in the present exemplary embodiment, the contour of the front surface 14 can be defined by a base contour (such as a contour defined by E _q (1)), and an auxiliary contour. In this practice, the auxiliary contour (Z _aux ) can be defined by the following relationship: Where: r ₁ represents the radial boundary within the transition region, r ₂ represents the radial boundary outside the transition region, and wherein: △ is defined by the following relationship: Wherein: n ₁ represents the refractive index of the material forming the optical member, n ₂ represents the refractive index of the medium surrounding the optical member, λ represents the design wavelength, and α represents a non-integer fraction, for example, 1⁄2.

In other words, in the present embodiment, the contour of the front surface (Z _sag ) is defined by the superposition of the base contour (Z _base ) and the auxiliary contour (Z _aux ) as defined below, and is illustrated graphically. 3 in the figure: Z _sag = Z _base + Z _aux Eq. (6)

In the present embodiment, the auxiliary contour defined by the above relational expressions (4) and (5) represents the feature by a substantially linear phase shift across the transition region. More specifically, the auxiliary profile may provide a phase shift that increases linearly from the inner boundary of the transition region to its outer boundary, and the optical path difference between the inner and outer boundaries corresponds to a non-integer fraction of the design wavelength.

In many embodiments, a crystallite in accordance with the teachings of the present invention, such as the above-described crystallite 10, can provide good hyperopic performance by effectively acting as a single-focusing crystal, and does not result in a diameter range in the central region of the crystallite. The optical effect caused by the phase shift of the small pupil diameter (for example, the pupil diameter of 2 mm). In the middle pupil diameter (for example, from about 2 mm to about 4 millimeters) In the case of a pupil diameter in the range of meters (e.g., a pupil diameter of about 3 mm), optical effects caused by the phase shift (e.g., changes in the wavefront leaving the crystal) can enhance functional near and intermediate vision. In the case of large pupil diameters (e.g., pupil diameters in the range of from about 4 mm to about 5 mm), the crystallites also provide good long-range performance because the phase shift only indicates the portion of the front surface that is in contact with the incident light. A small part.

By way of illustration, Figures 4A-4C show the optical properties of hypothetical crystals suitable for different pupil sizes in accordance with an embodiment of the present invention. It is assumed that the crystal has a front surface defined by the above relation (6), and a surface after the feature is represented by a flat convex base contour (for example, a plane defined by the above relation (2)). In addition, the crystallite has a diameter of 6 mm and its transition region extends between boundaries having an inner diameter of about 2.2 mm to an outer diameter of about 2.6 mm. The base curvature of the front and back surfaces is selected to provide the optical component with a nominal optical power of 21D. Furthermore, it has been assumed that the medium surrounding the crystal has a refractive index of about 1.336. Tables 1A-1C below list various parameters of the light piece of the crystal and various parameters of its front and back surfaces.

In more detail, in each of the 4A-4C diagrams, a cross-focus modulation transfer (MTF) chart corresponding to the following modulation frequency is provided: 25 line pairs/mm, 50 line pairs/mm, 75 line pairs/mm. And 100 lines/mm. The MTF shown in Figure 4A for a pupil diameter of about 2 mm means that the crystallite can provide good optical performance, for example for outdoor activities, with a focal depth of about 0.7 D, and the MTF is symmetrical near the focal plane. Sex. With respect to the pupil diameter of 3 mm, the MTFs shown in Fig. 4B are each asymmetrical with the focal plane of the crystal (i.e., relative to zero defocus), and its peaks are shifted in the negative defocus direction. . Such a transfer can provide a false adjustment force to aid in near vision (eg, for reading). Moreover, the width of these MTFs is greater than the width displayed by the MTF calculated for the 2 mm pupil diameter, which represents a better performance for mid-range vision. For a larger pupil diameter of 4 mm (Fig. 4C), the width and asymmetry of the MTFs are reduced relative to the calculated MTF width of the 3 mm diameter. It is also shown in low light conditions, such as for night driving, good Good farsightedness.

The optical effect of the phase shift can be adjusted by varying various parameters associated with the region, such as its radial extent and the rate at which the incident light is phase shifted. By way of example, the transition area defined by the above relation (3) shows that the loan can be borrowed. The defined slope, which can be varied to adjust the performance of the light member having such a transition region on its surface, is particularly suitable for the size of the middle pupil.

As an illustration, the 5A-5F diagram shows that it is formed by superimposing an auxiliary contour defined by the relational expression (2) and the auxiliary contour defined by the relational expressions (4) and (5). 3 For the hypothetical crystal of the front surface of the surface profile shown in the figure, the measured transpose modulation transfer function (MTF) is calculated at a modulation frequency of 3 mm and a modulation frequency of 50 lines/mm. ). It has been assumed that the optical member is formed of a material having a refractive index of 1.554. Moreover, the basic curvature of the front and back surfaces is selected such that the optical member has a nominal optical power of about 21D.

As a reference for providing an optical effect from which the transition region can be more easily understood, FIG. 5A shows an MTF for a light member having a disappearance Δz, that is, a phase shift lacking a phase shift according to the teachings of the present invention. Such a conventional light member having flat front and rear surfaces exhibits an MTF curve symmetrically disposed near the focus plane of the light member and exhibits a focal depth of about 0.4D. While Fig. 5B shows an MTF suitable for a light member according to an embodiment of the present invention, the front surface includes a transition region characterized by a radial extent of about 0.01 mm and Δz = 1 μm. The MTF chart shown in Figure 5B shows a greater depth of focus of about 1D, which indicates that the light piece can provide enhanced depth of field. And relative to the light The focal plane of the piece is asymmetrical. In fact, the peak of this MTF chart is closer to the light than its focus plane. It provides effective optical power enhancement to aid in close reading.

Since the transition region must be steeper (the radial extent is maintained at 0.01 mm) to obtain ΔZ = 1.5 μm (Fig. 5C), the MTF can be further widened (i.e., the optical member can provide a larger field of view). Depth) and its peaks may be further from the light member than the focal plane of the light member. As shown in Fig. 5D, the MTF suitable for an optical component having a transition region characterized by ΔZ = 2.5 μm is the same as the MTF as shown in Fig. 5A suitable for a light member having ΔZ = 0.

In fact, the MTF pattern can be repeated for each design wavelength. By way of example, an embodiment in which the design wavelength is 550 nm and the optical member is formed of Acrysof material (crosslinked copolymer of 2-phenylethyl acrylate and 2-phenylethyl methacrylate) In the example, ΔZ = 2.5 μm. For example, the MTF curve as shown in FIG. 5E corresponding to ΔZ=3.5 μm is the same as the MTF curve shown in FIG. 5B of ΔZ=1.5, and corresponds to ΔZ=4 μm as shown in FIG. 5F. The MTF curve shown in the figure is the same as the MTF curve shown in Fig. 5C corresponding to ΔZ = 1.5 μm. The optical path difference (OPD) corresponding to ΔZ of Z _aux defined by the above relation (3) can be defined by the following relationship: optical path difference (OPD) = (n _{2 -} n) ΔZ Eq. 7) wherein: n ₁ represents the refractive index of the material forming the optical member, and n ₂ represents the refractive index of the material surrounding the optical member. Thus, with n ₂ =1.552, n ₁ = 1.336, and ΔZ of 2.5 microns, an OPD equivalent to 1 λ can be obtained at a design wavelength of about 550 nm. In other words, the representative MTF chart shown in the 5A-5F graph can be repeated for the ΔZ variation of 1λ OPD.

Various methods can be used to obtain the transition region in accordance with the teachings of the present invention, and are limited to the above-described representative regions defined by relation (4). Moreover, although in some cases the transition region includes a surface portion that changes in mildness, in other cases it may be formed by a plurality of surface segments separated from one another by one or more steps.

FIG. 6 graphically depicts an IOL 24 in accordance with another embodiment of the present invention including a light member 26 having a front surface 28 and a back surface 30. Similar to the previous embodiment, the contour of the front surface is characterized by a superposition of a base profile and an auxiliary profile, but wherein the auxiliary profile is different from the above-described auxiliary profile of the previous embodiment.

As illustrated in Figure 7, the contour (Z _sag ) of the _front surface 28 of the IOL 24 described above is formed by the superposition of a base profile (Z _base ) and an auxiliary profile (Z _aux ). In more detail, in the present practice method, the contour of the front surface 28 of the can by the above relation (6) as follows replication of _{defined: Z sag = Z base + Z} aux wherein the base profile (Z _base) may be based on the relationship Defined by equation (2). However, the auxiliary contour (Z _aux ) is defined by the following relationship: Where r represents the radial distance from the optical axis of the crystal, and the parameters r _1a , r _1b , r _2a and r _2b are described in Figure 7, and are defined as follows: r _1a represents the transition of the auxiliary contour The inner diameter of the first substantially linear portion of the region.

r _1b represents the outer diameter of the first linear portion, r _2a represents the inner diameter of the second substantially linear portion of the transition region of the auxiliary contour, and r _2b represents the outer diameter of the second linear portion, and Wherein Δ ₁ and Δ ₂ can each be defined according to the above relation (8).

With continued reference to Fig. 7, in the present embodiment, the auxiliary profile _Zaux includes flat central and outer regions 32 and 34, and a double step transition region 36 connectable to the central and outer regions. In more detail, the transition region 36 includes a linearly varying portion 36a extending from a radially outer boundary of the central region 32 to a high hill region 36b (which extends from the radial position r _1a to another radial position r _1b ). The Takaoka region 36b from the radial position r _1b and then extends to a radial position r _2a, r _2a at the position which can be connected to another linearly varying region 36c, which may be in the radial position r _2b extending radially outwardly to an outer Area 34. The linearly varying portions 36a and 36c of the transition region may have similar or different slopes. In many practices, the total phase shift provided across the two transition regions is a non-integer fraction of a design wavelength (eg, 550 nm).

The contour of the rear surface 30 can be defined by the above relation (2) for Z _base having a suitable choice of various parameters including the radius of curvature c. The radius curvature of the base contour of the front surface and the curvature of the back surface together with the refractive index of the material forming the crystal lens may cause the crystallite to have a nominal refractive power, for example, in the range of about -15D to about +50D, or about Optical power in the range of 6D to about 34D, or in the range of about 16D to about 25D.

This representative IOL 24 can provide a number of benefits. For example, it can make the small pupil size get clear distance vision, and the optical effect of the double-step transition region helps to enhance the functional near and intermediate vision. Moreover, in many practices, the IOL can achieve good telephoto performance for large pupil sizes. By way of illustration, Fig. 8 shows that at different pupil sizes, according to an embodiment of the invention, there is a front surface (the outline of which is defined by the above relation (2) and the auxiliary contour of the front surface is by the above relation (8) And define) and the transfocal MTF graph calculated by the hypothetical light piece that flattens the convex back surface. These MTF graphs are for monochromatic incident radiation having a wavelength of 550 nm. Tables 2A-2C below provide parameters for the front and back surfaces of the light member.

These MTF charts demonstrate a pupil diameter of about 2 mm which is equal to the diameter of the central portion of the front surface. The optical member can provide a single focus refractive power and has a relatively small depth of focus of about 0.5 D (which is defined as the full width at half maximum). In other words, it provides good distance viewing performance. When the pupil size is increased to about 3 mm, the optical effect of the transition region becomes apparent in the trans-focus MTF. In more detail, the 3 mm MTF is significantly wider than the 2 mm MTF, which represents an increase in depth of field.

With continued reference to Figure 8, when the pupil diameter is even further increased to approximately 4 mm, the incident light encounters not only the central and transitional regions, but also a portion of the region outside the front surface.

Various techniques and materials can be used to assemble the IOLs of the present invention. For example, the light member of the IOL of the present invention can be formed from a variety of biocompatible polymer materials. Some suitable biocompatible materials include, but are not limited to: soft Acrylic polymers, hydrogels, polymethyl methacrylate, polybenzazole, polystyrene, cellulose, ethyl butyrate or other biocompatible materials. By way of example, in one embodiment, the optical member is formed from a soft acrylic polymer (crosslinked copolymer of 2-phenylethyl acrylate and 2-phenylethyl methacrylate) conventionally known as Acrysof. The fixing members (touch members) of the IOLs may also be formed of a suitable biocompatible material such as those described above. Although in some cases, the optical member and the stationary member of the IOL can be assembled in the form of a unitary unit, in other cases, they can be formed separately and combined using techniques known in the art.

Various assembly techniques known in the art, such as casting, can be used to assemble the IOLs. In some cases, a patent application in the application filed on December 21, 2007, entitled "Lens Surface With Combined Diffractive, Toric and Aspheric Components," may be used and its serial number is in No. 11/963,098. The assembly technique is such that the front and back surfaces of the IOL get the desired contour.

A person skilled in the art can understand that various changes can be made to the above embodiments without departing from the scope of the invention.

1‧‧‧Fixed components

2‧‧‧Fixed components

10‧‧‧Artificial Crystals (IOL)

12‧‧‧Lights

14‧‧‧ front surface

16‧‧‧Back surface

OA‧‧‧ optical axis

Claims (14)

A single-focus intraocular lens comprising a light member having a front surface and a rear surface disposed adjacent to the optical axis, at least one of the surfaces comprising at least one internal refractive region having a nominal optical power, having a nominal At least one outer refractive region of the optical power, and a refractive transition region disposed between the inner refractive region and the outer refractive region, the transition region extending from one of the inner radial boundaries to an outer radial boundary, wherein The transition region is adapted to monotonically change an incident radiation phase thereon from the inner boundary to the outer boundary to produce a phase shift between the outer and inner boundaries, characterized by a visible spectrum The design wavelength is selected to be a non-integer fraction such that an incoming wavefront of a first portion of the inner refractive region and an incoming wavefront of a second portion of the outer refractive region converge to produce a nominal optical power Different effective optical powers are used to establish a depth of focus. A single focused intraocular lens as claimed in claim 1, wherein the transition region is adapted to provide a monotonic change in optical path difference from the outer boundary of the inner region as an increasing diameter from the optical axis A function of distance. A single-focus intraocular lens as claimed in claim 2, wherein the monotonic change is characterized by a linear change in surface height Z _tps relative to a refractive surface and defines the nominal optical power as follows: r ₁ denotes a radial boundary within the transition region, r ₂ denotes a radial boundary outside the transition region, and wherein: Δ is defined by the following relationship: Wherein: n ₁ represents the refractive index of the material forming the optical member, n ₂ represents the refractive index of the medium surrounding the optical member when positioned in use or on the eye, λ represents the design wavelength, and α represents the selected non- Integer fraction. A single-focus intraocular lens as claimed in claim 2, wherein the monotonic change is characterized by a continuous linear change separated by one or more high hills, and wherein the change in surface height Z _aux relative to a refractive surface The nominal optical power is defined as follows: Where: r represents the radial distance from the optical axis of the crystal, r _1a represents the inner diameter of the first substantially linear portion of the transition region; r _1b represents the outer diameter of the first linear portion, r _2a represents An inner diameter of the second substantially linear portion of the transition region, and r _2b represents an outer diameter of the second substantially linear portion, and wherein Δ ₁ and Δ _{2 are} each defined according to the following relationship: And Wherein: n ₁ represents the refractive index of the material forming the optical member, n ₂ represents the refractive index of the medium surrounding the optical member, λ represents the design wavelength, α ₁ represents the first non-integer fraction, and α ₂ represents the second non-integer integer A score, the sum of the first and second non-integer scores is the selected non-integer score. A single focused intraocular lens as claimed in claim 1 wherein the selected non-integer fraction is less than one. A single focused intraocular lens as claimed in claim 1 wherein the selected non-integer fraction is greater than one. A single focused intraocular lens as claimed in claim 1 wherein the transition region comprises an annular region. A single focused intraocular lens of claim 7, wherein the annular region has a radial width of less than 1 mm. A single focused intraocular lens of claim 1, wherein the at least one surface has a radial diameter in the range of 1 mm to 5 mm. A single-focus intraocular lens as claimed in claim 1 wherein the design wavelength is 550 nm. A single focus intraocular lens as claimed in claim 1, wherein the light member has a transfocus modulation function for at least a portion of a range of aperture sizes between 1.5 mm and 6 mm. The focusing plane of the light member is asymmetrical. A single-focus intraocular lens as claimed in claim 1, wherein the effective optical power is a transfocal modulation function of a light member having a design wavelength in a range of apertures between 1.5 mm and 6 mm. Peaks are characteristic. A single focused intraocular lens as claimed in claim 12, wherein the depth of field is characterized by a full width at 15% contrast within the transfocus modulation transfer function. A single focused intraocular lens as claimed in claim 1 wherein the difference in effective power relative to the nominal optical power is between 0.25 D and 1.75 D.