Intraocular Lens (IOL) Based On Metasurface

Abstract

An intraocular lens (IOL) based on a metasurface, includes: a front optical lens, a rear optical lens, an equatorial plane, and an optical loop. The front optical lens and the rear optical lens are connected through the equatorial plane. The optical loop is connected with the equatorial plane. A metasurface structure is arranged on the equatorial plane. The metasurface structure includes a plurality of nanostructure units with a phase distribution of a planar axicon lens. A Gaussian beam is generated based on a biconvex lens structure of a conventional IOL, and the phase distribution of the planar axicon lens is loaded through a geometric phase of the metasurface structure, such that a Bessel-Gaussian beam is generated. When the beam is propagated in a free space, a cross section of the beam is not changed along with a propagation distance, such that the Bessel-Gaussian beam keeps a relatively consistent focal plane within a certain propagation distance, thereby realizing characteristics of long focal depth, adjustable refraction, and achromatism.

Claims

1. An intraocular lens (IOL) based on a metasurface, comprising: a front optical lens, a rear optical lens, an equatorial plane, and an optical loop, wherein the front optical lens and the rear optical lens are connected through the equatorial plane, the optical loop is connected with the equatorial plane, and a metasurface structure is arranged on the equatorial plane; and the metasurface structure comprises a plurality of nanostructure units with a phase distribution of a planar axicon lens.

2. The IOL based on the metasurface according to claim 1, wherein each of the plurality of nanostructure units in the metasurface structure is distributed according to φ.sub.axicon=2*α, wherein α is a rotation angle of the nanostructure unit, φ.sub.axicon is the phase distribution of the planar axicon lens, and * is a multiplication sign.

3. The IOL based on the metasurface according to claim 2, wherein a phase distribution formula of the planar axicon lens is: $\{\begin{array}{c}{\phi }_{\mathrm{axicon}}=\sqrt{x^2+y^2}\times 2\pi /\lambda \times \sin \beta ,\\ \beta ={\tan }^{-1}\left(R/f\right)\end{array}$ wherein φ.sub.axicon is the phase distribution of the planar axicon lens, x and y are position coordinates of a two-dimensional coordinate system with a center of the planar axicon lens as an origin respectively, λ is an incident wavelength, f is a focal length corresponding to a maximum aperture R of the metasurface structure and is a focal length under static refractive power +58.64D, and β is a maximum angle corresponding to the metasurface structure.

4. The IOL based on the metasurface according to claim 2, wherein structural dimensions of the plurality of nanostructure units are determined by an incident wavelength.

5. The IOL based on the metasurface according to claim 4, wherein when the incident wavelength λ=600 nm, each nanostructure unit has a height H of 300 nm, a width W of 110 nm, a length L of 310 nm, and a lattice constant d of 470 nm.

6. The IOL based on the metasurface according to claim 2, wherein the metasurface structure comprises 212,345,780 nanostructure units and is arranged with a total of 2,660 rings.

7. The IOL based on the metasurface according to claim 6, wherein the plurality of nanostructure units are made of polymethyl methacrylate (PMMA).

8. The IOL based on the metasurface according to claim 2, wherein a refractive index of each nanostructure unit is in a visible light range of [1.46, 1.49].

9. The IOL based on the metasurface according to claim 1, wherein a thickness of the metasurface structure is 300 nm.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0019] To describe the embodiments of the present disclosure or the technical solutions in the prior art more clearly, the accompanying drawings required in the embodiments are briefly introduced below. Obviously, the accompanying drawings described below are only some embodiments of the present disclosure. Those of ordinary skill in the art may further obtain other accompanying drawings based on these accompanying drawings without creative effort.

[0020] FIG. 1 is a front view of a structure of an IOL based on a metasurface of the present disclosure;

[0021] FIG. 2 is a side view of a structure of the IOL based on a metasurface of the present disclosure;

[0022] FIG. 3 is a schematic diagram of a nanostructure unit in a metasurface structure of the present disclosure; and

[0023] FIG. 4 is an optical path diagram of a Bessel beam generated by an axicon lens in the present disclosure.

[0024] Reference Numerals:

[0025] 1, equatorial plane, 2, metasurface structure, 3, optical loop, 4, front optical lens, and 5, rear optical lens.

DETAILED DESCRIPTION OF THE EMBODIMENTS

[0026] The technical solutions of the embodiments of the present disclosure are clearly and completely described below with reference to the accompanying drawings. Apparently, the described embodiments are merely a part rather than all of the embodiments of the present disclosure. All other embodiments obtained by those of ordinary skill in the art based on the embodiments of the present disclosure without creative efforts shall fall within the protection scope of the present disclosure.

[0027] An objective of the present disclosure is to provide an IOL based on a metasurface to realize functions of long focal depth, adjustable refraction, and achromatism.

[0028] To make the above-mentioned objective, features, and advantages of the present disclosure clearer and more comprehensible, the present disclosure will be further described in detail below in conjunction with the accompanying drawings and specific embodiments.

[0029] In recent years, the progress of nanotechnology has enabled a manipulation of materials at an atomic level, which is helpful to the development of new optical materials. In 1999, a concept of metamaterial was proposed by Professor Rodger M. Walser from the University of Texas. The metamaterial is a three-dimensional artificial composite material constructed by subwavelength artificial microstructures (artificial atoms) with specific electromagnetic properties in a certain arrangement, showing a strong ability to control electromagnetic waves, and realizing physical phenomena and functions that cannot be achieved by natural materials. Through structural adjustment, the metamaterial can in principle be designed with any permittivity and magnetic conductivity, thus producing many wave manipulation effects that cannot be achieved by natural materials. But as a 3D structure, metamaterials are designed to be still overly complicated, and optical materials should be thinner and more efficient. Thus, a concept of metasurface came into being. In short, the metasurfaces can be viewed as a 2D version of metamaterials, which is constructed by planar subatoms. These atoms purposely select electromagnetic responses in a specific order and use abrupt phase transitions on the surface of the structure to transmit or reflect waves. Therefore, the present disclosure adopts the most advanced metasurface technology in the current optical field to construct a novel IOL with functions of long focal depth and achromatism under stepless zoom.

[0030] As shown in FIG. 1 to FIG. 2, the present disclosure provides an IOL based on a metasurface, including: a front optical lens 4, a rear optical lens 5, an equatorial plane 1, and an optical loop 3. The front optical lens 4 and the rear optical lens 5 are connected through the equatorial plane 1. The optical loop 3 is connected with the equatorial plane 1. A metasurface structure 2 is arranged on the equatorial plane 1. The metasurface structure 2 includes a plurality of nanostructure units with a phase distribution of a planar axicon lens. In the present disclosure, the phase distributions of the planar axicon lens at different positions are attached to the nanostructure units of the metasurface structure through the design of the metasurface structure 2, such that a Bessel-Gaussian beam is generated. When the Bessel-Gaussian beam propagates in a free space, a cross section of the beam is not changed along with the propagation distance, such that the Bessel-Gaussian beam keeps a relatively consistent focal plane within a certain propagation distance, thereby realizing characteristics of long focal depth, adjustable refraction, and achromatism.

[0031] In an optional embodiment, each of the plurality of nanostructure units in the metasurface structure 2 of the present disclosure is distributed according to φ.sub.axicon=2*α, where α is a rotation angle of the nanostructure unit, φ.sub.axicon is the phase distribution of the planar axicon lens, and * is a multiplication sign. In the present embodiment, a phase distribution formula of the planar axicon lens is:

[00002]$\{\begin{array}{c}{\phi }_{\mathrm{axicon}}=\sqrt{x^2+y^2}\times 2\pi /\lambda \times \sin \beta ,\\ \beta ={\tan }^{-1}\left(R/f\right)\end{array}$

[0032] where φ.sub.axicon is the phase distribution of the planar axicon lens, x and y are position coordinates of a two-dimensional coordinate system with a center of the planar axicon lens as an origin respectively, λ is an incident wavelength, f is a focal length corresponding to a maximum aperture R of the metasurface structure and is a focal length under static refractive power +58.64D, that is, f=17.053 mm, and β is a maximum angle corresponding to the metasurface structure, that is, R=2.5 mm, and β=tan.sup.−(2.5/17.053)=8.34°.

[0033] In an optional embodiment, structural dimensions of the plurality of nanostructure units of the present disclosure are determined by an incident wavelength. In the present embodiment, taking the incident wavelength λ=600 nm as an example, each nanostructure unit has a height H of 300 nm, a width W of 110 nm, a length L of 310 nm, and a lattice constant d of 470 nm, as shown in FIG. 3.

[0034] In an optional embodiment, the plurality of nanostructure units of the present disclosure are made of PMMA. The nanostructure unit has a refractive index in a visible light range of [1.46, 1.49].

[0035] On an equatorial plane of a conventional IOL, the nanostructure units of a metasurface structure are constructed by techniques such as photolithography or nanoimprinting, and are orderly arranged according to a formula between the phase and the rotation angle of the nanostructure unit (i.e. φ.sub.axicon=2*α). In the present embodiment, the metasurface structure 2 is arranged with a total of 2,660 rings, and designed with 212,345,780 nanostructure units. The frontal schematic distribution diagram of the metasurface structure 2 is shown in FIG. 1. Since the feature size of the metasurface structure 2 is too small, feature structure details of the metasurface structure 2 cannot be reasonably displayed when compared with macroscopic objects such as the IOLs. Therefore, the designed metasurface structure is partially magnified by 133 times.

[0036] In the present embodiment, as shown in FIG. 2, the front and rear of the equatorial plane 1 are optical lens surfaces of aspherical surfaces of conventional IOLs, and a layer of metasurface structure 2 with a thickness of 300 nm is provided on the equatorial plane.

[0037] The IOL based on a metasurface provided by the present disclosure takes three-dimensional surface contour parameters presented by the human eye lens under the standard eye static refraction power +58.64D as a design standard of the three-dimensional surface contour model of the IOL. On this basis, the metasurface is designed on the equatorial plane of the IOL. Different from the fact that a Gaussian beam is generated based on a biconvex lens structure of the conventional IOL, the phase distribution of the planar axicon lens is loaded through a geometric phase of the metasurface structure, such that a Bessel-Gaussian beam is generated. A cross section of the beam is not changed along with a propagation distance, such that the Bessel-Gaussian beam keeps a relatively consistent focal plane within a certain propagation distance, thereby realizing characteristics of a long focal depth, adjustable refraction, and achromatism, as shown in FIG. 4.

[0038] Various embodiments of the present specification are described in a progressive manner, each embodiment focuses on differences from other embodiments, and the same and similar parts between the various embodiments may be referred to each other.

[0039] In this specification, some specific examples are used for illustration of the principles and implementations of the present disclosure. The description of the foregoing embodiments is used to help illustrate the method of the present disclosure and the core ideas thereof. In addition, those of ordinary skill in the art can make various modifications in terms of specific implementations and the scope of application in accordance with the ideas of the present disclosure. In conclusion, the content of the present description shall not be construed as limitations to the present disclosure.