The present disclosure relates generally to ophthalmic lenses, and more specifically to novel double-sided aspheric phase-ring structured lenses, designs, manufacture, and uses thereof.
Ophthalmology is the field of medicine directed to the anatomy, physiology, and diseases of the human eye. The anatomy of the human eye is rather complex. The main structures of the eye include the cornea, an aspherical clear tissue at the outer front of the eye; the iris, which is the colored part of the eye; the pupil, an adaptable aperture in the iris that regulates the amount of light received in the eye; the crystalline lens, a small clear disk inside the eye that focuses light rays onto the retina; and the retina, a layer that forms the rear or backside of the eye and transforms sensed light into electrical impulses that travel through the optic nerve to the brain. The posterior chamber (i.e., the space between the retina and the lens) is filled with aqueous humour, and the anterior chamber (i.e., the space between the lens and the cornea) is filled with vitreous humour, or a clear, jelly-like substance.
The natural crystalline lens has a flexible, transparent, biconvex structure, and together with the cornea, operates to refract light to be focused on the retina. The lens is flatter on its anterior side than on its posterior side and its curvature is controlled by the ciliary muscles to which the lens connects by suspensory ligaments, called zonules. By changing the curvature of the lens, the focal distance of the eye is changed so as to focus on objects at various distances. To view an object at a short distance from the eye, the ciliary muscles contract, and the lens thickens, resulting in a rounder shape and thus high refractive power. Changing focus to an object at a greater distance requires the relaxation of the lens and thus increasing the focal distance. This process of changing curvature and adapting the focal distance of the eye to form a sharp image of an object at the retina is called accommodation.
In humans, the refractive power of the crystalline lens in its natural environment is approximately 18-20 diopters, roughly one-third of the total optical power of the eye. The cornea provides the remaining 40 diopters of the total optical power of the eye.
With the ageing of the eye, the opaqueness of the lens increases, called a cataract. Some diseases like diabetes, trauma, some medications, and excessive UV light exposure may also cause a cataract. A cataract is painless and results in a cloudy, blurry vision. Treatments for cataracts include surgery, by which the cloudy lens is removed and replaced with an artificial one, generally called an intraocular lens (IOL or IOLs).
Another age-related effect is called presbyopia, which is manifested by difficulty in reading small print or seeing nearby pictures clearly. Presbyopia generally is believed to be caused by a thickening and loss of flexibility of the natural lens inside the eye. Age-related changes also take place in the ciliary muscles surrounding the lens. With less elasticity it becomes harder to focus on objects close to the eye.
A variety of intraocular lenses are also employed for correcting other visual disorders, such as myopia, or nearsightedness when the eye is unable to see distant objects caused by, for example, the cornea having too much curvature. The effect of myopia is that distant light rays focus on a point in front of the retina, rather than directly on its surface. Hyperopia, or farsightedness caused by an abnormally flat cornea, causes light rays entering the eye to focus behind the retina, therefore not allowing the eye to see objects that are close. Astigmatism is another common cause of visual difficulty in which images are blurred due to an irregularly shaped cornea.
In the majority of cases, intraocular lenses (IOLs) are implanted in a patient's eye during cataract surgery to replace the natural crystalline lens and compensate for the loss of optical power of the removed lens. Modern IOL optics are designed to have a multifocal optic for providing short, intermediary and distance vision of objects, also called multifocal IOLs, or more specifically, trifocal lenses. Presbyopia is traditionally corrected by eyeglasses or contact lenses, and patients may also opt for multifocal optics. In some cases, an IOL can include diffractive structures to have not only a far-focus power but also a near-focus power, thereby providing a degree of pseudo-accommodation. However, a variety of aberrations, such as spherical and astigmatic aberrations, can adversely affect the optical performance of such lenses. For example, spherical aberrations can degrade vision contrast, especially for large pupil sizes.
Although multifocal ophthalmic lenses often lead to improved quality of vision for many patients, additional improvements would be beneficial. For example, some pseudophakic patients experience undesirable visual effects (dysphotopsia), such as glare or halos, especially during use in dark environments (e.g., nighttime). Halos may arise when light from the unused focal image creates an out-of-focus image that is superimposed on the used focal image. For example, if light from a distant point source is imaged onto the retina by the distant focus of a bifocal IOL, the near focus of the IOL will simultaneously superimpose a defocused image on top of the image formed by the distant focus. This defocused image may manifest itself in the form of a ring of light surrounding the in-focus image and is referred to as a halo. Another area in need of improvement revolves around the typical bifocality of multifocal lenses. More particularly, since multifocal ophthalmic lenses typically provide for near and far vision, intermediate vision may be compromised.
Accordingly, what is needed is one or more ophthalmic lenses with an extended depth of focus (EDOF) that may simultaneously provide a near focus, intermediate focus, and distance focus, while also addressing the aforementioned adverse effects, such as dysphotopsia (e.g., halo, glare, etc.), thereby providing enhanced contrast and improved visual acuity.
The present disclosure is related to double-sided aspheric ophthalmic lenses with phase-ring structures, which can provide an extended depth of focus, thereby enhancing contrast and improving vision acuity while reducing undesirable visual effects such as glare and halos. The phase-ring structures of the ophthalmic lenses described herein may be designed to provide depth of focus via a non-diffracting beam principle with constructive phasing, thereby maximizing the focal energy in the lens.
In some embodiments, an ophthalmic lens comprising a lens body is provided, the lens body comprising: a first aspheric surface; and a second aspheric surface comprising a base curvature and a phase-ring structure, wherein the phase-ring structure comprises an inner region and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the outer region comprises a second phase-ring surface having a second curvature; and an outer edge of the inner region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region and the outer region causes constructive interference that produces a distance focus and an extended focus.
In some embodiments, a method of treating an ophthalmic disease or disorder in a subject is provided, the method comprising implanting into an eye of the subject an ophthalmic lens comprising a lens body, the lens body comprising: a first aspheric surface; and a second aspheric surface comprising a base curvature and a phase-ring structure, wherein the phase-ring structure comprises an inner region and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the outer region comprises a second phase-ring surface having a second curvature; and an outer edge of the inner region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region and the outer region causes constructive interference that produces a distance focus and an extended focus.
In some embodiments, a method of manufacturing an ophthalmic lens is provided, the method comprising: manufacturing a first aspheric surface; manufacturing a second aspheric surface comprising a base curvature; and generating a phase-ring structure on the second aspheric surface, wherein the phase-ring structure comprises an inner region and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the outer region comprises a second phase-ring surface having a second curvature; and an outer edge of the inner region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region and the outer region causes constructive interference that produces a distance focus and an extended focus.
In some embodiments, an ophthalmic lens comprising a lens body is provided, the lens body comprising: a first aspheric surface; and a second aspheric surface comprising a base curvature and a phase-ring structure, wherein the phase-ring structure comprises an inner region, an intermediate region, and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the intermediate region comprises a second phase-ring surface having a second curvature; the outer region comprises a third phase-ring surface having a third curvature; an outer edge of the inner region is adjacent to an inner edge of the intermediate region; and an outer edge of the intermediate region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region, the intermediate region, and the outer region causes constructive interference that produces a near focus and a distance focus.
In some embodiments, a method of treating an ophthalmic disease or disorder in a subject, the method comprising implanting into an eye of the subject an ophthalmic lens comprising a lens body, the lens body comprising: a first aspheric surface; and a second aspheric surface comprising a base curvature and a phase-ring structure, wherein the phase-ring structure comprises an inner region, an intermediate region, and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the intermediate region comprises a second phase-ring surface having a second curvature; the outer region comprises a third phase-ring surface having a third curvature; an outer edge of the inner region is adjacent to an inner edge of the intermediate region; and an outer edge of the intermediate region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region, the intermediate region, and the outer region causes constructive interference that produces a near focus and a distance focus.
In some embodiments, a method of manufacturing an ophthalmic lens is provided, the method comprising: manufacturing a first aspheric surface; manufacturing a second aspheric surface comprising a base curvature; and generating a phase-ring structure on the second aspheric surface, wherein the phase-ring structure comprises an inner region, an intermediate region, and an outer region, and the inner region comprises a first phase-ring surface having a first curvature; the intermediate region comprises a second phase-ring surface having a second curvature; the outer region comprises a third phase-ring surface having a third curvature; an outer edge of the inner region is adjacent to an inner edge of the intermediate region; and an outer edge of the intermediate region is adjacent to an inner edge of the outer region, wherein refraction of light passing through the inner region, the intermediate region, and the outer region causes constructive interference that produces a near focus and a distance focus.
In some embodiments, a set of ophthalmic lenses is provided, comprising: a first ophthalmic lens comprising a first lens body, the first lens body comprising: a first aspheric surface; and a second aspheric surface comprising a first base curvature and a first optical phase-ring structure, wherein the first optical phase-ring structure comprises a first inner region and a first outer region, and the first inner region comprises a first phase-ring surface; and the outer region comprises a second phase-ring surface; a second ophthalmic lens comprising a second lens body, the second lens body comprising: a third aspheric surface; and a fourth aspheric surface comprising a second base curvature and a second optical phase-ring structure, wherein the second optical phase-ring structure comprises a second inner region, an intermediate region, and a second outer region, and the second inner region comprises a third phase-ring surface; the intermediate region comprises a fourth phase-ring surface; and the second outer region comprises a fifth phase-ring surface; wherein refraction of light passing through the first inner region and the outer region of the first ophthalmic lens causes first constructive interference and refraction of light passing through the second inner region, the intermediate region, and the second outer region causes second constructive interference, thereby collectively producing a near focus, distance focus, and an extended focus.
The present application can be best understood by reference to the following description taken in conjunction with the accompanying figures included in the specification.
The present disclosure relates to double-sided aspheric ophthalmic lenses with phase-ring structures, such as extended depth of focus (EDOF) lenses and multifocal lenses, and methods of designing and manufacturing such lenses. The lenses can include a first aspheric (anterior) surface and a second aspheric (posterior) surface. One of the two surfaces can include a phase-ring structure, and the other surface can optionally include a toric component. The phase-ring structure may comprise a series of concentric regions extending from the center of the lens to the edge of the lens. The transition between regions in the phase-ring structure may be represented by a ring that corresponds to a ridge in the surface profile of the ophthalmic lens. The phase-ring structure is designed to provide the depth of focus via a non-diffracting beam principle with constructive phasing to maximize the focal energy. The multifocal and extended depth of focus lenses described herein may utilize refractive optics, such that the surface profiles of the phase-ring structures comprise sloped walls rather than, for example, vertical walls (or steps) associated with diffractive lens designs. Refractive lenses give focal points using the refractive effect of light waves at the refracting surface comprising boundary surfaces with different refractive indexes. Thus, when refraction of light passes through the one or more regions of the lenses described herein, constructive interference produces an extended depth of focus and improved distance focus, intermediate focus, and near focus.
The double-sided aspheric surface design results in an improvement of the modulation transfer function (MTF) of the lens-eye combination by aberration reduction and vision contrast enhancement as compared to a one-sided aspheric lens. The phase-ring structures described herein can enable an extended depth of focus for ophthalmic lenses, and as a set of lenses may produce continuous vision from a near focus, intermediate focus, and a distance focus. Various phase-ring structures are described in greater detail below with reference to two double-sided aspheric lens designs, hereinafter referred to as an extended depth of focus (EDOF) lens and a multifocal lens.
The height profile illustrated in
In some embodiments, a double-sided aspheric multifocal lens design with phase-ring structures may be provided for extending the depth of focus at least between an intermediate and far focus.
For example,
The real add power of a lens with a phase-ring structure corresponding to the phase profile of
For example, the theoretical add power for a lens not having the phase-ring structure corresponding to the phase profile of
In some embodiments, the inner region of the phase-ring structure may comprise a first phase-ring surface having a first curvature. The curvatures described herein may comprise one or more continuous arcs, parabolas, and/or lines. As shown, the first curvature may be monotonically decreasing (e.g., negative sloping) as it extends outwards from an optical axis of the lens. The first curvature may comprise a first (inner) sloping portion that slopes at a first angle with respect to an optical axis of the ophthalmic lens and a second (outer) sloping portion that slopes at a second angle with respect to the optical axis, each of the first and second sloping portions together sloping monotonically with respect to the optical axis. The first angle may be greater than the second angle such that the slope of the inner sloping portion may be less than that of the outer sloping portion. The inner radius (fin) may be greater than 0 mm and less than or equal to 5 mm, such as 0.30 mm, 0.35 mm, 0.40 mm, 0.45 mm, 0.55 mm, 0.60 mm, 0.65 mm, or 0.70 mm.
In some embodiments, the outer region of the phase-ring structure may comprise a second phase-ring surface having a second curvature. The second curvature may comprise a first (inner) sloping portion that slopes at a third angle with respect to the optical axis of the ophthalmic lens, a second (intermediate) sloping portion that slopes at a fourth angle with respect to the optical axis, and a third (outer) sloping portion that slopes at a fifth angle with respect to the optical axis. As shown, the second curvature may not be monotonically increasing or decreasing in a direction outwards from the optical axis of the lens. Rather, the intermediate sloping portion and the second outer sloping portion may together slope monotonically (e.g., both negative sloping) with respect to the optical axis, while the second inner sloping portion may slope in a direction opposite that of the intermediate sloping portion and the second outer sloping portion, such that the second curvature overall slopes non-monotonically. The fourth angle may be greater than the fifth angle such that the slope of the intermediate sloping portion may be less than that of the outer sloping portion. The outer radius (rout) may be greater than 0 mm and less than or equal to 5 mm, such as 0.70 mm, 0.75 mm, 0.80 mm, 0.85 mm, 0.90 mm, 0.95 mm, 1.00 mm, 1.05 mm, 1.10 mm, 1.15 mm, 1.20 mm, 1.25 mm, or 1.30 mm. The outer radius of the phase profile of the phase-ring structure may be proportional to the inner radius. For example, the relationship between the inner radius and outer radius may be expressed as 1≤rout/rin≤3.
In some embodiments, an outer edge of the inner region of the phase-ring structure may be adjacent to an inner edge of the outer region of the phase-ring structure. As shown in
of 3.0 D. The theorical add power for a lens not having the phase-ring structure corresponding to the phase profile of
The inner radius (rin) of the phase profile in
The phase profile (Φ(n)(r)) of the phase-ring structures corresponding to the schematics provided in
In some embodiments, the phase profile illustrated in
of 3.35 D. The theoretical add power for a lens not having the phase-ring structure corresponding to the phase profile of
The inner radius (rin) of the phase profile in
In some embodiments, the phase profile illustrated in
The inner region may comprise a first phase-ring surface having a first curvature and the outer region may comprise a second phase-ring surface having a second curvature. An outer edge of the inner region may be adjacent to an inner edge of the outer region. The manufactured ophthalmic lens may produce a distance focus and an extended focus. Optionally, at step 1104 an in-situ image quality analysis of the double-sided aspheric phase-ring structured lens may be performed. For example, an ISO Model Eye 2 may be used to measure the through-focus MTF using the TRIOPTICS OptiSpheric® IOL PRO 2 to determine whether a performance of the ophthalmic lens meets predetermined quality criteria.
Lens 1200 can include a light transmissive circular disk-shaped lens body 1201 with an optic diameter 1206 and a center thickness 1210, as well as a pair of haptics 1202 as flexible support for the IOL when implanted into patient's eye, with a total outer diameter 1207. Lens body 1201 can include an anterior surface 1208, a posterior surface 1209, a central zone 1203 and a surrounding area 1204. As mentioned above, lens body 1201 can include an optical axis 1205 extending transverse to the anterior surface 1208 and posterior surface 1209. A person of skill in the art will appreciate that the optical axis 1205 is a virtual axis for purposes of referring to the optical properties of lens 1200. The pair of haptics 1202 can be extended outwardly from the lens body 1201 for supporting the lens 1200 after being implanted in the human eye. In some embodiments, the haptics 1202 of lens 1200 can hold the lens in place in the capsular bag.
In some embodiments, lens body 1201 can take the shape of a biconvex shape. Other shapes of lens body 1201 can include but are not limited to, plano-convex, biconcave, plano-concave shape, or combinations of convex and concave shapes. In some embodiments, both anterior surface 1208 and posterior surface 1209 can feature an aspheric structure, providing a double-sided asphericity for lens 1200.
As mentioned above at least with respect to
In some embodiments, the optic diameter 1206 of lens body 1201 may be greater than or equal to about 4 mm, such as about 4.5 mm, 5 mm, 5.5 mm, 6 mm, 6.5 mm, 7 mm, 7.5 mm, or 8 mm. The total outer diameter 1207 of lens 1200 including the haptics 1202 may be greater than or equal to about 9 mm, such as 10 mm, 11 mm, 12 mm, 13 mm, 14 mm, 15 mm, 16 mm, 17 mm, or 18 mm. Lens body 1201 may have a center thickness 1210 greater than or equal to about 0.8 mm, such as 0.85 mm, 0.9 mm, 0.95 mm, 1.0 mm, 1.05 mm, 1.10 mm, 1.15 mm, or 1.20 mm. One of ordinary skill in the art will recognize that although
The amount of correction that an ophthalmic lens provides is called optical power and is expressed in Diopter (D). The optical power is calculated as the inverse of a focal distance f measured in meters, which can be a respective focal distance from the lens to a respective focal point for far, intermediate, or near vision. Lens body 1201 (and lens body 1601 described in greater detail below) can provide a base optical power of about −15 D to about +55 D.
The ophthalmic lenses of the present disclosure, such as lens 1200 (and lens 1600 described in greater detail below), can be made of flexible material which permits a reduction of their overall apparent girth by temporary deformation, facilitating their insertion through the cornea, thereby advantageously enabling the use of a corneal incision of concomitantly reduced size. In some embodiments, the lens body can include polypropylene, polycarbonate, polyethylene, acryl-butadiene styrene, polyamide, polychlorotrifluoroethylene, polytetrafluoroethylene, polyvinyl chloride, polyvinylidene fluoride, polyvinylchloride, polydimethylsiloxane, polyethylene terephthalate, ethylene tetrafluoroethylene, ethylene chlorotrifluoroethylene, perfluoroalkoxy, polymethylpentene, polymethylmethacrylate, polystyrene, polyetheretherketone, tetrafluoroethylene, polyurethane, poly(methyl methacrylate), poly(2-hydroxyethyl methacrylate), nylon, polyether block amide, silicone or a mixture thereof.
In some embodiments, the lens body can include a hydrophilic polymer made of monomers selected from the group consisting of: 2-acrylamido-2-methylpropane sulfonic acid, 2-hydroxyethyl methacrylate, N-vinylpyrrolidone, vinylbenzyltrimethyl ammonium salt, diethylaminoethyl methacrylate, dimethylaminoethyl acrylate, dimethylaminoethyl methacrylate, diethylaminoethyl acrylate, diethylaminomethyl methacrylate, tertiary butylaminoethyl acrylate, tertiary-butylaminoethyl methacrylate and dimethylaminopropylacrylamide, acrylic acid, methacrylic acid, styrenesulfonic acid and salts thereof, hydroxypropyl acrylate, vinylpyrrolidone, dimethylacrylamide, ethylene glycol monomethacrylate, ethylene glycol monoacrylate, ethylene glycol dimethacrylate, ethylene glycol diacrylate, triethylene glycol diacrylate and triethylene glycol methacrylate. In some embodiments, these hydrophilic monomers are surface grafted onto the polymeric matrix mentioned above to make the lens body. In some embodiments, the ophthalmic lenses of the present disclosure can be made of polymeric compositions according to U.S. Pat. No. 10,494,458, titled “Functionalized hydrophilic and lubricious polymeric matrix and methods of using same,” which is incorporated herein by reference in its entirety.
As mentioned above, the ophthalmic lens of the present disclosure can be an intraocular lens (IOL). The haptics of the IOL according to the present disclosure can be made of polymeric materials including but not limited to polymethacrylate, polypropylene, polyethylene, polystyrene, and polyacrylate.
The surface of the IOL can include spheric, aspheric, and/or toric elements. Spheric surfaces can cause spherical aberration, which is a type of optical imperfection that can cause increased glare and reduced overall quality of vision especially in low light and darkness. Aspheric lenses can correct spherical aberration. Aspherical IOLs can provide improved contrast sensitivity, enhanced functional vision and superior night driving ability.
A toric element is typically used for astigmatic eye correction. Generally, astigmatism is an optical defect in which vision is blurred due to the ocular inability to focus a point object into a sharply focused image on the retina. This inability may be due to an irregular curvature of the cornea and/or lens. The refractive error of the astigmatic eye stems from a difference in degree of curvature, and therefore in degree of refraction, of the different meridians of the cornea and/or the crystalline lens, which causes the eye to have two focal points, one correspondent to each meridian. As used herein, a meridian includes one of two axes that subtend a curved surface, such as the prime meridian on the earth, for example. Meridians may be orthogonal. By way of example, the meridians of the earth may be any orthogonal line of longitude and any line of latitude that curve about the surface of the earth.
For example, in an astigmatic eye, an image may be clearly focused on the retina in the horizontal (sagittal) plane but may be focused behind the retina in the vertical (tangential) plane. In the case where the astigmatism results only from the cornea, the two astigmatism meridians may be the two axes of the cornea. If the astigmatism results from the crystalline lens, the two astigmatism meridians may be the two axes of the crystalline lens. If the astigmatism results from a combination of the cornea and the crystalline lens, the two astigmatism meridians may be the respective axes of the combined lenses of the cornea and the crystalline lens.
An astigmatism arising from the cornea or crystalline lens, or the combination of the two lenses, may be corrected by a lens including a toric component. A toric surface resembles a section of the surface of a football, for which there are two regular radii of curvature, one smaller than another. These radii may be used to correct the defocus in the two meridians of the astigmatic eye. Thus, blurred vision caused by astigmatism may be corrected by corrective lenses or laser vision correction, such as glasses, hard contact lenses, contact lenses, and/or intraocular lenses (IOLs), providing a compensating optic specifically rotated around the optical axis.
In some embodiments, the ophthalmic lenses according to the present disclosure can provide far vision for viewing objects at distances ranging from about infinity to about 6 meters (m). In some embodiments, one or more lenses of the present disclosure can provide near vision for viewing objects at distances less than about 3 m. In some embodiments, the lenses of the present disclosure can provide intermediate vision for viewing objects at distances in a range of about 0.3 m to about 1 m, about 2 m, about 3 m, about 4 m, about 5 m, or about 6 m. As a result, the lens of the present disclosure can advantageously provide a degree of accommodation for different distance ranges, typically referred to as pseudo-accommodation. In some embodiments, when implanted into a patient's eye, the combined power of the eye's cornea and the near, intermediate, and far power of the ophthalmic lens of the present disclosure can allow focusing light emanating from objects within a near, an intermediate, and a far distance range of the patient onto the retina. In some embodiments, the distance focus (f0) and extended focus (f1) provided by the IOLs of the present disclosure can be defined by the following expressions:
is representative of the theoretical add power, and
is representative of the real add power.
In some embodiments, a double-sided aspheric multifocal lens design with phase-ring structures may be provided for improving far and near vision. The multifocal lens may minimize undesirable visual effects, such as dysphotopsia (glare, halos, etc.) experienced during use of ophthalmic lenses, and in specific, during nighttime use.
For example,
The real add power of a lens with a phase-ring structure corresponding to the phase profile of
For example, the theoretical add power for a lens not having the phase-ring structure corresponding to the phase profile of
In some embodiments, the inner region of the phase-ring structure may comprise a first phase-ring surface having a first curvature. The curvatures described herein may comprise one or more continuous arcs, parabolas, and/or lines. As shown, the first curvature may be monotonically decreasing (e.g., negative sloping) as it extends outwards from an optical axis of the lens. The first curvature may comprise a first (inner) sloping portion that slopes at a first angle with respect to an optical axis of the ophthalmic lens and a second (outer) sloping portion that slopes at a second angle with respect to the optical axis. The first sloping portion and the second sloping portion together may slope monotonically with respect to the optical axis of the ophthalmic lens. The first angle may be greater than the second angle such that the slope of the inner sloping portion may be less than that of the outer sloping portion. The inner radius (rin) may be greater than 0 mm and less than or equal to 5 mm, such as 0.30 mm, 0.35 mm, 0.40 mm, 0.45 mm, 0.55 mm, 0.60 mm, 0.65 mm, or 0.70 mm.
In some embodiments, the intermediate region of the phase-ring structure may comprise a second phase-ring surface having a second curvature. The second curvature may comprise a first (inner) sloping portion that slopes at a third angle with respect to the optical axis of the ophthalmic lens and a second (outer) sloping portion that slopes at a fourth angle with respect to the optical axis. As shown, the second curvature may not be monotonically increasing or decreasing in a direction extending outwards from the optical axis of the lens. Rather, the inner sloping portion and the outer sloping portion may slope in different directions. The intermediate radius (rint) may be greater than 0 mm and less than or equal to 5 mm, such as 0.70 mm, 0.75 mm, 0.80 mm, 0.85 mm, 0.90 mm, 0.95 mm, 1.00 mm, 1.05 mm, 1.10 mm, 1.15 mm, 1.20 mm, 1.25 mm, or 1.30 mm.
In some embodiments, the outer region of the phase-ring structure may comprise a third phase-ring surface having a third curvature. The third curvature may comprise a first (inner) sloping portion that slopes at a fifth angle with respect to the optical axis of the ophthalmic lens and a second (outer) sloping portion that slopes at a sixth angle with respect to the optical axis. As shown, the third curvature may not be monotonically increasing or decreasing in a direction outwards from the optical axis of the lens. Rather, the inner sloping portion and the outer sloping portion may slope in different directions. The outer radius (rout) may be greater than 0 mm and less than or equal to 5 mm, such as 0.70 mm, 0.75 mm, 0.80 mm, 0.85 mm, 0.90 mm, 0.95 mm, 1.00 mm, 1.05 mm, 1.10 mm, 1.15 mm, 1.20 mm, 1.25 mm, or 1.30 mm. The outer radius of the phase profile of the phase-ring structure may be proportional to the inner radius. For example, the relationship between the inner radius and outer radius may be expressed as 1≤rout/rin≤3.
In some embodiments, an outer edge of the inner region of the phase-ring structure may be adjacent to an inner edge of the intermediate region of the phase-ring structure. Likewise, an outer edge of the intermediate region may be adjacent to an inner edge of the outer region of the phase-ring structure. As shown in
of 3.35 D. The theoretical add power for a lens not having the phase-ring structure corresponding to the phase profile of
The inner radius (rin) of the phase profile in
The phase profile (Φ(n)(r)) of the phase-ring structures corresponding to the schematics provided in
In some embodiments, the phase profile illustrated in
Lens 1600 may include any one or more features of lens 1200 described above with respect to
In some embodiments, lens body 1601, like lens body 1201, can take the shape of a biconvex shape. Other shapes of lens body 1601 can include but are not limited to, plano-convex, biconcave, plano-concave shape, or combinations of convex and concave shapes. In some embodiments, both anterior surface 1608 and posterior surface 1609 can feature an aspheric structure, providing a double-sided asphericity for lens 1600.
As mentioned above at least with respect to
In some embodiments, the optic diameter 1606 of lens body 1601 may be greater than or equal to about 4 mm, such as about 4.5 mm, 5 mm, 5.5 mm, 6 mm, 6.5 mm, 7 mm, 7.5 mm, or 8 mm. The total outer diameter 1607 of lens 1600 including the haptics 1602 may be greater than or equal to about 9 mm, such as 10 mm, 11 mm, 12 mm, 13 mm, 14 mm, 15 mm, 16 mm, 17 mm, or 18 mm. Lens body 1601 may have a center thickness 1610 greater than or equal to about 0.8 mm, such as 0.85 mm, 0.9 mm, 0.95 mm, 1.0 mm, 1.05 mm, 1.10 mm, 1.15 mm, or 1.20 mm. One of ordinary skill in the art will recognize that although
The phase-ring structures described above and embodied on the extended depth of focus ophthalmic lens and multifocal ophthalmic lens of the present disclosure can be designed using Equations (I) to (IV) as discussed below.
Pupil Function. A pupil function is a lens characteristic function that describes the physical effect of a lens by which it is possible to change the state of light made incident on the lens, and in specific terms, is represented by the product of the amplitude function A(r) and the exponential function of the phase function Φ(n)(r) as noted in Equation (I) below.
Phase Function. A phase function is defined as the function that mathematically expresses the physical effect provided in a lens such as giving changes in the phase of incident light on a lens (position of wave peaks and valleys) using any method. The variable of the phase function is mainly expressed by position r in the radial direction from the center of the lens, and the phase of light made incident on the lens at the point of the position r undergoes a change by the phase function Φ(n)(r) and is emitted from the lens. In specific terms, this is represented by an r−Φ coordinate system. In the present disclosure, phase is noted as Φ, and the unit is radians. One wavelength of light is represented as 2π radians, and a half wavelength as π radians, for example. A distribution of phase in the overall area in which the phase function is provided and expressed in the same coordinate system is called a phase profile, or simply a profile or zone profile. With an r axis of Φ=0 as a reference line, this means that the light made incident at the point of Φ=0 is emitted without changing the phase. Also, for this reference line, when a positive value is used for Φ, this means that progress of the light is delayed by that phase amount, and when a negative value is used for Φ, this means that progress of the light is advanced by that phase amount. In an actual ophthalmic lens, a refracting surface for which a diffractive structure is not given corresponds to this reference line (surface). Light undergoes a phase change based on this phase function and is emitted from the lens.
Amplitude Function. An amplitude function is the function expressed by A(r) in Equation (I) noted above. In the present disclosure, this is defined as a function that represents the change in the light transmission amount when passing through a lens. The variable of the amplitude function is represented as position r in the radial direction from the center of the lens, and represents the transmission rate of the lens at the point of position r. Also, the amplitude function is in a range of 0 or greater to 1 or less, which means that light is not transmitted at the point of A(r)=0, and that incident light is transmitted as it is without loss at the point of A(r)=1.
Zone. In the present disclosure, a zone is used as the minimum unit in a phase-ring structure, element, or diffraction grating provided in a lens. A zone may be circular or annular in shape and may be bounded along an inner radius and/or along an outer radius by a ring. For example, a first zone may be circular in area such that the ring is bounded only along an outer radius (i.e., a first ring), and for each subsequent zone the annular area between the (n−1)th ring and the nth ring may be referred to as the nth zone.
The height profile of the phase-ring structure (Zphase) on the ophthalmic lens can be calculated based on Equation (II) below. In some embodiments, the height may be based on one cycle (2π, which may be about 3.35 μm), the refractive index of the lens and the medium covering the lens, and the wavelength used (e.g., green light, which has a wavelength of about 550 nm).
The outer radius of a particular zone (rn) can be calculated based on Equation (III) below.
Phase function (Φ(n)(r)) can be calculated via Equation (IV) below.
The phase function base profile f(r) could be a linear parabolic sine or polynomial function. A and D are the light distribution parameters. A is the amplitude scale factor; D is the vertical shift, if it is +D, the function moves up, if it is −D, then the function moves down. In some embodiments, A(n) can be a ratio of phase function base profile, and D(n) can be the phase shift of phase function base profile. As shown below with respect to the examples provided herein, the parameter A may correspond to the slope of the phase-ring structure in different zones.
The double-sided aspheric structure (anterior and posterior of the optic area of the ophthalmic lens) is for the correction of the spherical aberration of the lens. The height profile of the aspheric base structure (Zasp) of the lens can be calculated according to the following Equation (V).
When both aspheric and phase-ring structures are placed onto the same surface (anterior surface and/or posterior surface of the ophthalmic lens), according to some embodiments of the present disclosure, the height profile of the combination structure (Ztotal) will be the summation of the height profile of the aspheric base curvature (Zasp) and the height profile of the phase-ring structure (Zphase), as calculated according to the below Equation (VI).
In some embodiments, the above-described ophthalmic lenses can be a contact lens or an intraocular lens (IOL). In some embodiments, the IOL can be an intracorneal IOL, anterior chamber IOL, or posterior chamber IOL. While the haptic arms are illustrated in the embodiment, any suitable haptics fixation structure for the capsular bag or the ciliary sulcus compatible with posterior chamber implantation can also be used in a posterior chamber IOL.
A way of estimating the optical priority of an ophthalmic lens comprises determining experimentally its modulation transfer function (MTF). The MTF of an optical system can be measured according to Annex C of ISO 11979-2, which reflects the proportion of the contrast transmitted through the optical system for a determined spatial frequency of a test pattern, which frequency is defined as “cycles/mm” or “LP/mm”, in which “LP” indicates “line pairs.” Generally, the contrast decreases with an increase in spatial frequency.
Presented below are examples discussing different embodiments of the IOLs contemplated above. The following examples are provided to further illustrate the embodiments of the present disclosure but are not intended to limit the scope of the disclosure. While they are typical of those that might be used, other procedures, methodologies, or techniques known to those skilled in the art may alternatively be used.
The MTF of an extended depth of focus (EDOF) lens and multifocal lens may differ at varying apertures and/or resolution measurements. For example, at an aperture of 2 mm and resolution measurement of 50 LP/mm, an MTF value greater than 0.05 may indicate an EDOF lens design (e.g., curve (2) in
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 2.4 D.
In some embodiments, each of the rings listed in Table 1 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
or about 2.4 D.
In some embodiments, each of the rings listed in Table 2 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 2.4 D.
In some embodiments, each of the rings listed in Table 3 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 3.35 D.
In some embodiments, each of the rings listed in Table 4 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 3.35 D.
In some embodiments, each of the rings listed in Table 5 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 3.0 D.
In some embodiments, each of the rings listed in Table 6 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. Curve (4) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(4) in
of about 3.0 D.
In some embodiments, each of the rings listed in Table 7 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(3) in
of about 3.5 D.
In some embodiments, each of the rings listed in Table 8 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(3) in
of about 3.5 D.
In some embodiments, each of the rings listed in Table 9 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Curve (1) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm. Curve (2) illustrates the MTF at a 2 mm aperture and at a resolution measurement of 50 LP/mm. Curve (3) illustrates the MTF at a 3 mm aperture and at a resolution measurement of 50 LP/mm at a monofocal mode. The curves (1)-(3) in
of about 3.35 D.
In some embodiments, each of the rings listed in Table 10 may correspond to a given point or set of points on a phase profile of a phase-ring structure. For example,
Unless defined otherwise, all terms of art, notations and other technical and scientific terms or terminology used herein are intended to have the same meaning as is commonly understood by one of ordinary skill in the art to which the claimed subject matter pertains. In some cases, terms with commonly understood meanings are defined herein for clarity and/or for ready reference, and the inclusion of such definitions herein should not necessarily be construed to represent a substantial difference over what is generally understood in the art.
As used herein, the singular forms “a,” “an,” and “the” are intended to include the plural forms as well, unless the context clearly indicates otherwise. It is also to be understood that the term “and/or” as used herein refers to and encompasses any and all possible combinations of one or more of the associated listed items. It is further to be understood that the terms “includes, “including,” “comprises,” and/or “comprising,” when used herein, specify the presence of stated features, integers, steps, operations, elements, components, and/or units but do not preclude the presence or addition of one or more other features, integers, steps, operations, elements, components, units, and/or groups thereof.
The numerical ranges disclosed inherently support any range or value within the disclosed numerical ranges, including the endpoints, even though a precise range limitation is not stated verbatim in the specification because this disclosure can be practiced throughout the disclosed numerical ranges.
The foregoing description, for the purpose of explanation, has been described with reference to specific embodiments. However, the illustrative discussions above are not intended to be exhaustive or to limit the invention to the precise forms disclosed. Many modifications and variations are possible in view of the above teachings. The embodiments were chosen and described in order to best explain the principles of the techniques and their practical applications. Others skilled in the art are thereby enabled to best utilize the techniques and various embodiments with various modifications as are suited to the particular use contemplated.
Although the disclosure and examples have been fully described with reference to the accompanying figures, it is to be noted that various changes and modifications will become apparent to those skilled in the art. Such changes and modifications are to be understood as being included within the scope of the disclosure and examples as defined by the claims.
is add power.
The application claims benefit of priority under 35 U.S.C. § 119(e) of U.S. Ser. No. 63/299,635, filed Jan. 14, 2022, the content of which is incorporated by reference in its entirety.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/US2023/060681 | 1/13/2023 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 63299635 | Jan 2022 | US |