Electroactive lens with multiple depth diffractive structures
US-9329309-B2 · May 3, 2016 · US
US10054725B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-10054725-B2 |
| Application number | US-201615074163-A |
| Country | US |
| Kind code | B2 |
| Filing date | Mar 18, 2016 |
| Priority date | Feb 27, 2012 |
| Publication date | Aug 21, 2018 |
| Grant date | Aug 21, 2018 |
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Certain exemplary embodiments can provide a system, machine, device, manufacture, circuit, composition of matter, and/or user interface adapted for and/or resulting from, and/or a method and/or machine-readable medium comprising machine-implementable instructions for, activities that can comprise and/or relate to, switch a diffractive first electro-active lens from a first power state corresponding to a first optical power to a second power state corresponding to a second optical power that differs from said first optical power.
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What is claimed is: 1. An electro-active lens comprising: a Fresnel structure comprising: a first zone defined by a first plurality of concentric rings, each ring from said first plurality of rings defined by a first maximum radial cross-section height, wherein at least one concentric ring in the first plurality of concentric rings has at least one of a rounded outer corner or a rounded inner corner; and a second zone defined by a second plurality of concentric rings, each ring from said second plurality of rings defined by a second maximum radial cross-section height, said first maximum radial cross-section height differing from said second maximum radial cross-section height; and liquid crystal material in optical communication with the Fresnel structure, wherein said first maximum radial cross-section height is substantially equal to a first integer multiple of a quotient corresponding to a predetermined wavelength of light divided into an optical path difference of the electro-active lens. 2. The electro-active lens of claim 1 , wherein: said second maximum radial cross-section height is substantially equal to a second integer multiple of said quotient. 3. The electro-active lens of claim 1 , wherein: the optical path difference equals a difference between a first optical path length of the electro-active lens that corresponds to when said electro-active lens is electrically powered and a second optical path length of said electro-active lens that corresponds to when said electro-active lens is not electrically powered. 4. The electro-active lens of claim 1 , wherein: said Fresnel structure is formed in a first substrate. 5. The electro-active lens of claim 4 , wherein: the first substrate is flooded with the liquid crystal material. 6. The electro-active lens of claim 4 , wherein: the first substrate, in cooperation with a second substrate, sandwiches the liquid crystal material. 7. The electro-active lens of claim 1 , wherein: said electro-active lens forms part of at least one of an ophthalmic lens, a camera, a projector, or a solar concentrator. 8. The electro-active lens of claim 1 , in combination with at least one of another electro-active lens, a refractive electro-active lens, a fluidic lens, or a conventional refractive lens. 9. The electro-active lens of claim 1 , wherein: at least one of said second plurality of concentric rings has a rounded outer corner. 10. The electro-active lens of claim 1 , wherein: at least one of said second plurality of concentric rings has a rounded inner corner. 11. A method comprising: in an electro-active lens comprising a Fresnel structure comprising: a first zone defined by a first plurality of concentric rings, each ring from said first plurality of rings defined by a first maximum radial cross-section height, said first maximum radial cross-section height being substantially equal to a first integer multiple of a quotient corresponding to a predetermined wavelength of light divided into an optical path difference of the electro-active lens, wherein at least one concentric ring in said first plurality of concentric rings has at least one of a rounded outer corner or a rounded inner corner; and a second zone defined by a second plurality of concentric rings, each ring from said second plurality of rings defined by a second maximum radial cross-section height differing from said second maximum radial cross-section height, switching said electro-active lens from a first power state corresponding to a first optical power to a second power state corresponding to a second optical power that differs from said first optical power. 12. The electro-active lens of claim 1 , wherein: the first plurality of rings defines a first peak in a first plane and the second plurality of rings defines a second peak in the first plane. 13. An electro-active lens having a variable optical power, the electro-active lens system comprising: an electro-active material having a variable refractive index to change the variable optical power of the electro-active lens; and a substrate in optical communication with the electro-active material, the substrate defining a structure comprising: a first plurality of rings, each ring in the first plurality of rings having a first height and at least one rounded corner, the first height being substantially equal to a first integer multiple of a quotient corresponding to a predetermined wavelength of light divided into an optical path difference of the electro-active lens; a second plurality of rings, concentric with the first plurality of rings, each ring in the second plurality of rings having a second height greater than the first height and at least one rounded corner. 14. The electro-active lens of claim 13 , wherein each ring in the first plurality of rings has a rounded inner corner and a rounded outer corner. 15. The electro-active lens of claim 14 , wherein each ring in the second plurality of rings has a rounded inner corner and a rounded outer corner. 16. The electro-active lens of claim 15 , wherein the first plurality of rings is closer to a center of the diffractive structure than the second plurality of rings. 17. The electro-active lens of claim 13 , wherein the first plurality of rings defines a first trough in a first plane and the second plurality of rings defines a second trough in a second plane below the first plane. 18. The electro-active lens of claim 17 , wherein the first plurality of rings defines a first peak in a third plane and the second plurality of rings defines a second peak in the third plane.
with discontinuous faces, e.g. Fresnel lens {(diffractive Fresnel lenses G02B5/1876)} · CPC title
having means for producing variable diffraction (controlling the direction of light by means of one or more diffracting elements G02B26/0808; acousto-optical elements G02F1/11, G02F1/33; electro- or magneto-optical diffraction G02F1/292, G02F1/2955) · CPC title
Physics · mapped topic
Electrooptic lenses · CPC title
Plurality of such optical elements formed in or on a supporting substrate · CPC title
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