Infinite large-aperture lens system with aspherical surfaces

Claim 2

An infinite lens system for receiving light having parallel rays and wavelengths between 1300 nm and 1550 nm and for collimating light having wavelengths between 1300 nm and 1550 nm, said lens system comprising a large-aperture lens with first and second aspherical surfaces represented by equation (1), the lens also having a shape and formed from a glass fulfilling the conditions of equations (2) to (4) Z=[C.sub.i Y.sup.2 /[1+(1-(1+K.sub.i)C.sub.i.sup.2 Y.sup.2).sup.1/2 ]]+E.sub.i Y.sup.4 +F.sub.i Y.sup.6 +G.sub.i Y.sup.8 +H.sub.i Y.sup.10( 1) 1.0<(f/NA)<3.0 (2) 1.2<r.sub.1 /[(n-1)f]<2.3 (3) n>1.70, ν>30.0 (4) where, Z: Distance from a plane vertical to an optical axis passing the apex to one of the first and second aspherical surfaces Y: Height from the optical axis of the lens C i : Curvature of the aspherical surface apex of the i-th surface (1/r i ) K i : Conical constant of the i-th surface E i to H i : Coefficients of aspherical surfaces of the fourth- to tenth-order of the i-th surface NA: Numerical aperture f: Focal length d: Lens thickness r i : Radius of curvature of aspherical surface apex of the i-th surface n: Refractive index of the glass at wavelengths between 1300 nm and 1550 nm ν: Abbe number of the glass at wavelengths between 1300 nm and 1550 nm, wherein i=1 and 2 for said first and second aspherical surfaces, respectively, and said lens has a magnification factor β of zero.

Claim 3

A lens according to claim 1, wherein the lens is made from a glass which has a high refractive index and a glass transformation temperature Tg exceeding 580° C.

Claim 4

A lens according to claim 2, wherein the lens is produced by precision press-molding.

Claim 5

An infinite lens system for use with light having parallel rays and wavelengths between 1300 nm and 1550 nm and for collimating light having wave-lengths between 1300 nm and 1550 nm, said lens system comprising a large-aperture lens having first and second aspherical surfaces meeting the requirements of equation (1) Z=[C.sub.i Y.sup.2 /[1+(1-(1+K.sub.i)C.sub.i.sup.2 Y.sup.2).sup.1/2 ]]+E.sub.i Y.sup.4 +F.sub.i Y.sup.6 +G.sub.i Y.sup.8 +H.sub.i Y.sup.10( 1) wherein the improvement comprises said large-aperture lens also having a shape and formed from a glass fulfilling the conditions of equations (2) to (4) 1.0<(f/NA)<3.0 (2) 1.2<r.sub.1 /[(n-1)f]<2.3 (3) n>1.70, ν>30.0 (4) where, Z: Distance from a plane vertical to an optical axis passing the apex to one of the first and second aspherical surfaces Y: Height from the optical axis of the lens C i : Curvature of the aspherical surface apex of the i-th surface (1/r i ) K i : Conical constant of the i-th surface E i to H i : Coefficients of aspherical surfaces of the fourth- to tenth-order of the i-th surface NA: Numerical aperture f: Focal length r i : Radius of curvature of aspherical surface apex of the i-th surface n: Refractive index of the glass at wavelengths between 1300 nm and 1550 nm ν: Abbe number of the glass at wavelengths between 1300 nm and 1550 nm, wherein i=1 and 2 for said first and second aspherical surfaces, respectively, and said lens has a magnification factor β of zero.

Claim 6

An infinite lens system for use with light having parallel rays and wavelengths between 1300 nm and 1550 nm and for collimating light having wave-lengths between 1300 nm and 1550 nm, said lens system comprising a large-aperture lens having first and second aspherical surfaces meeting the requirements of equation (1) Z=[C.sub.i Y.sup.2 /[1+(1-(1+K.sub.i)C.sub.i.sup.2 Y.sup.2).sup.1/2 ]]+E.sub.i Y.sup.4 +F.sub.i Y.sup.6 +G.sub.i Y.sup.8 +H.sub.i Y.sup.10( 1) wherein the improvement comprises said large-aperture lens also having a shape and formed from a glass fulfilling the conditions of equations (2) to (4) 1.0<(f/NA)<3.0 (2) 1.2<r.sub.1 /[(n-1)f]<2.3 (3) n>1.70, ν>30.0 (4) where, Z: Distance from a plane vertical to an optical axis passing the apex to one of the first and second aspherical surfaces Y: Height from the optical axis of the lens C i : Curvature of the aspherical surface apex of the i-th surface (1/r i ) K i : Conical constant of the i-th surface E i to H i : Coefficients of aspherical surfaces of the fourth- to tenth-order of the i-th surface NA: Numerical aperture f: Focal length r i : Radius of curvature of aspherical surface apex of the i-th surface n: Refractive index of the glass at wavelengths between 1300 nm and 1550 nm ν: Abbe number of the glass at wavelengths between 1300 nm and 1550 nm, wherein i=1 and 2 for said first and second aspherical surfaces, respectively, and said lens has a magnification factor β of zero.