Lens structure having low pass filter characteristic
원문보기
IPC분류정보
국가/구분
United States(US) Patent
등록
국제특허분류(IPC7판)
G02B-003/02
H04N-005/225
출원번호
US-0029419
(2011-02-17)
등록번호
US-8385005
(2013-02-26)
발명자
/ 주소
Smith, George E.
출원인 / 주소
Avago Technologies ECBU IP (Singapore) Pte. Ltd.
인용정보
피인용 횟수 :
2인용 특허 :
8
초록
A lens structure includes a surface devoid of cusps that includes a seamless profile wherein the surface includes at least one segmented parabolic function forming a filtering surface for producing a controlled amount of spherical aberration.
대표청구항▼
1. A lens structure comprising: a surface devoid of cusps that includes a seamless profile wherein the surface includes at least one segmented parabolic function forming a filtering surface for producing a controlled amount of spherical aberration, the segmented parabolic function comprising at leas
1. A lens structure comprising: a surface devoid of cusps that includes a seamless profile wherein the surface includes at least one segmented parabolic function forming a filtering surface for producing a controlled amount of spherical aberration, the segmented parabolic function comprising at least two half-cycles bounded by at least two quarter cycles, each half-cycle being symmetric with respect to any other half-cycle. 2. The lens structure of claim 1, further comprising: a first outer lens surface configured to receive light waves incident thereon;a second outer lens surface configured to transmit light waves transmitted through the lens structure from the first lens surface; anda changeable aperture operably associated with the lens, wherein at least one of the first outer lens surface and the second outer lens surface is defined by the seamless profile comprising a plurality of adjoining concave and convex segments having sag perturbations disposed therealong, the seamless profile and sag perturbations being configured to reduce spatial aliasing in an image produced by the lens along a focal plane associated therewith so as to pass predetermined lower spatial frequencies and reject predetermined higher spatial frequencies, the lens, the first and second outer lens surfaces, and the aperture having an optical axis associated therewith, each of the plurality of adjoining segments being defined by a parabolic function unique thereto and being rotationally symmetric in respect of the optical axis, the first and second outer lens surfaces being symmetric about the optical axis, the sag perturbations being configured to provide a controlled amount of spherical aberration such that the amount of spherical aberration provided by the lens is substantially independent of changes in the aperture. 3. The lens structure of claim 2, wherein the seamless profile has between 1 and 8 half cycles of sag perturbations disposed therealong. 4. The lens structure of claim 2, wherein the seamless profile further includes at least one of one quarter cycle of sag perturbations and one half cycle of sag perturbations disposed therealong. 5. The lens structure of claim 2, wherein the sag perturbations have maximum slopes and minimum slopes of substantially the same magnitude. 6. The lens structure of claim 2, wherein first portions of the lens are configured to over-correct for spherical aberration and second portions of the lens are configured under-correct for spherical aberration. 7. The lens structure of claim 2, wherein the seamless profile follows a first parabolic function and a second parabolic function in a family of parabolic functions having the same slope at a selected radius value in respect of the optical axis. 8. The lens structure of claim 2, wherein the seamless profile follows a first parabolic function and a second parabolic function in a family of parabolic functions having the same magnitude at a selected radius value in respect of the optical axis. 9. The lens structure of claim 2, wherein the spherical aberration produced by at least portions of the lens is under-corrected. 10. The lens structure of claim 2, wherein the spherical aberration produced by at least portions of the lens is over-corrected. 11. A method for forming a lens structure, comprising: forming a surface devoid of cusps that includes a seamless profile, wherein the surface is defined by a segmented parabolic function comprising at least two half-cycles bounded by at least two quarter cycles, each half-cycle being symmetric with respect to any other half-cycle, the surface forming a filtering surface for producing a controlled amount of spherical aberration. 12. The method of claim 11, further comprising: providing a first outer lens surface configured to receive light waves incident thereon;providing a second outer lens surface configured to transmit light waves transmitted through a lens from the first outer lens surface; andproviding an aperture operably associated with the lens, wherein at least one of the first outer lens surface and the second outer lens surface is defined by a seamless profile comprising a plurality of adjoining concave and convex segments having sag perturbations disposed therealong, the seamless profile and sag perturbations being configured to at least one of reduce spatial aliasing and increase spherical aberration in an image produced by the lens along a focal plane associated therewith so as to pass predetermined lower spatial frequencies and reject predetermined higher spatial frequencies, the lens, the first and second outer lens surfaces and the aperture having an optical axis associated therewith, each of the plurality of adjoining segments being defined by a parabolic function unique thereto and being rotationally symmetric in respect of the optical axis, the first and second outer lens surfaces being symmetric about the optical axis, the sag perturbations being configured to provide a controlled amount of spherical aberration such that the amount of spherical aberration provided by the lens is substantially independent of changes in the aperture. 13. The method of claim 12, further comprising over-correcting spherical aberration in an image produced by the lens. 14. The method of claim 12, further comprising under-correcting spherical aberration in an image produced by the lens. 15. The method of claim 12, further comprising providing first portions of the lens to over-correct for spherical aberration and providing second portions of the lens to under-correct for spherical aberration. 16. A lens structure comprising: a surface devoid of cusps that includes a seamless profile wherein the surface includes at least one segmented parabolic function forming a filtering surface for producing a controlled amount of spherical aberration, the segmented parabolic function comprising at least two half-cycles bounded by at least two quarter cycles, each half-cycle being symmetric with respect to any other half-cycle; anda changeable aperture operably associated with the lens structure, wherein a surface of the lens structure is defined by the seamless profile comprising a plurality of adjoining concave and convex segments having sag perturbations disposed therealong, the seamless profile and sag perturbations being configured to reduce spatial aliasing in an image produced by the lens along a focal plane associated therewith so as to pass predetermined lower spatial frequencies and reject predetermined higher spatial frequencies. 17. The lens structure of claim 16, wherein the seamless profile has between 1 and 8 half cycles of sag perturbations disposed therealong. 18. The lens structure of claim 16, wherein the seamless profile further includes at least one of one quarter cycle of sag perturbations and one half cycle of sag perturbations disposed therealong. 19. The lens structure of claim 16, wherein first portions of the lens structure are configured to over-correct for spherical aberration and second portions of the lens are configured under-correct for spherical aberration. 20. The lens structure of claim 16, wherein the seamless profile follows a first parabolic function and a second parabolic function in a family of parabolic functions having the same slope at a selected radius value in respect of the optical axis.
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