Infra-red lenses

Claim 2

An infra-red lens of very high aperture greater than F/0.75 comprising from front to back in the order given at least one positive meniscus first element convex towards the front, a negative meniscus second element concave towards the front, a positive meniscus third element convex towards the front and a positive fourth element having a front surface convex towards the front, all of said elements being spaced apart.

Claim 3

A lens according to claim 1 having a single positive meniscus element convex towards the front in front of the negative meniscus element.

Claim 4

A lens according to claim 1 having two positive meniscus elements convex towards the front in front of the negative meniscus element.

Claim 5

A five element lens according to claim 3 wherein the front-most positive meniscus element has a focal length of about +7F (where F is the focal length of the complete lens).

Claim 6

A lens according to claim 1 wherein the back element having a front surface convex towards the front is a meniscus element.

Claim 7

A lens according to claim 1 wherein the back element having a front surface convex towards the front has a back surface curvature greater than or equal to zero and of the opposite sign as the curvature of said front surface.

Claim 8

A lens according to claim 1 wherein said at least one positive meniscus element is of a material selected from the group consisting of germanium and silicon.

Claim 9

A lens according to claim 1 wherein the negative meniscus element is of a material having a dispersion at least as high as germanium.

Claim 10

A lens according to claim 1 wherein the positive meniscus element behind the negative meniscus element is of a material selected from the group consisting of germanium and silicon.

Claim 11

A lens according to claim 1 wherein the back positive element having a front surface convex towards the front is of germanium.

Claim 12

A lens according to claim 1, wherein, the rear surface of said third element is of greater curvature than its front surface.

Claim 13

A lens according to claim 1, wherein, the radius of curvature of the rear surface of said third element is less than the focal length of the lens.

Claim 14

A lens according to claim 1, wherein, the rear surface of said third element is of greater curvature than its front surface, and the radius of curvature of the rear surface of said third element is less than the focal length of the infra-red lens.

Claim 15

A lens according to claim 13, wherein, the radius of curvature of the rear surface of said fourth element is less than the focal length of the infra-red lens.

Claim 16

A lens according to claim 1, wherein, the radius of curvature of the rear surface of said fourth element is less than the focal length of said infra-red lens.

Claim 17

A lens according to claim 1, wherein, the radius of curvature of the front surface of said fourth element is greater than the radius of curvature of the rear surface of said third element.

Claim 18

A four element lens according to claim 2 wherein all four elements are of germanium.

Claim 19

A four element lens according to claim 2 wherein (as considered from front to back) the first and third elements are of germanium and the second element is of a material having a dispersion higher than that of germanium.

Claim 20

A four element lens according to claim 2 wherein (as considered from front to back) the first element is of silicon, the second element is of a material of higher dispersion than silicon, and the third element is of a material selected from the group consisting of germanium and silicon.

Claim 21

A four element lens according to claim 2 wherein the individual elements (considered from front to back) have focal lengths in the respective ranges +1.5F to +1.8F, -1.3F to -3.2F, +0.7F to +2.9F, and +0.6F to +0.7F (where F is the focal length of the complete lens).

Claim 22

A four element lens according to claim 20 wherein the spaces between the individual elements (as considered from front to back) are in the respective ranges 0.6F to 0.9F, 0.3F to 0.4F and about 0.1F (where F is the focal length of the complete lens).

Claim 23

In an infra-red lens basically of triplet configuration having a front component comprising at least one positive meniscus element convex towards the front, a middle component comprising a negative meniscus element concave towards the front, and a positive rear component, the improvement wherein the positive rear component comprises a pair of spaced apart lens elements the front one of which is a positive meniscus element convex towards the front and the rear one of which is a positive element having a front surface convex towards the front, thereby increasing the aperture of the lens to greater than F/0.75.

Claim 24

In an infra-red lens basically of triplet configuration having a front component comprising at least one positive meniscus element convex towards the front, a middle component comprising a negative meniscus element concave towards the front, and a positive rear component, the improvement wherein the positive rear component comprises a pair of spaced apart lens elements the front one of which is a positive meniscus element convex towards the front and the rear one of which is a positive element having a front surface convex towards the front, thereby increasing the aperture of the lens to greater than F/0.75.

Claim 25

In an infra-red lens basically of triplet configuration having a front component comprising at least one positive meniscus element convex towards the front, a middle component comprising a negative meniscus element concave towards the front whose front concave surface provides positive third order spherical aberration which counteracts the aggregate of the negative third order contributions from the other lens elements, the aperture of the lens being limited by the excess positive transverse fifth order spherical aberration which arises at said front concave surface as a result of said positive third order spherical aberration, and a positive rear component, the improvement wherein said positive rear component comprises a pair of separate lens elements the front one of which is a positive meniscus element convex towards the front and the rear one of which is a positive element having a front surface convex towards the front, thereby limiting the negative third order spherical aberration contribution of said rear component and hence the amount of positive third order spherical aberration required from said front concave surface, so that the resulting excess positive transverse fifth order spherical aberration arising at said front concave surface is of a limited value which allows a very high aperture greater than F/0.75 to be attained.

Claim 26

In an infra-red lens basically of triplet configuration having a front component comprising at least one positive meniscus element convex towards the front, a middle component comprising a negative meniscus element concave towards the front whose front concave surface provides positive third order spherical aberration which counteracts the aggregate of the negative third order contributions from the other lens elements, the aperture of the lens being limited by the excess positive transverse fifth order spherical aberration which arises at said front concave surface as a result of said positive third order spherical aberration, and a positive rear component, the improvement wherein said positive rear component comprises a pair of separate lens elements the front one of which is a positive meniscus element convex towards the front and the rear one of which is a positive element having a front surface convex towards the front, thereby limiting the negative third order spherical aberration contribution of said rear component and hence the amount of positive third order spherical aberration required from said front concave surface, so that the resulting excess positive transverse fifth order spherical aberration arising at said front concave surface is of a limited value which allows a very high aperture greater than F/0.75 to be attained.

Claim 27

An infra-red lens of very high aperture comprising from front to back in the order given at least one positive meniscus element convex towards the front, a negative meniscus element concave towards the front and spaced from said at least one positive meniscus element, the front concave surface of said negative meniscus element providing positive third order spherical aberration which counteracts the aggregate of the negative third order contributions from the other lens elements and the resulting excess positive transverse fifth order spherical aberration arising at said front concave surface determining the aperture of the lens, and a pair of lens elements spaced from said negative meniscus element, the front element of said pair being a positive meniscus element convex towards the front and the rear element of said pair being a positive element having a front surface convex towards the front, the negative third order spherical aberration contribution of said lens pair being of a limited value at which the counteracting positive third order spherical aberration provided by said front concave surface results in a limited amount of excess positive transverse fifth order spherical aberration providing a very high aperture greater than F/0.75.

Claim 28

An infra-red lens of very high aperture comprising from front to back in the order given at least one positive meniscus element convex towards the front, a negative meniscus element concave towards the front and spaced from said at least one positive meniscus element, the front concave surface of said negative meniscus element providing positive third order spherical aberration which counteracts the aggregate of the negative third order contributions from the other lens elements and the resulting excess positive transverse fifth order spherical aberration arising at said front concave surface determining the aperture of the lens, and a pair of lens elements spaced from said negative meniscus element, the front element of said pair being a positive meniscus element convex towards the front and the rear element of said pair being a positive element having a front surface convex towards the front, the negative third order spherical aberration contribution of said lens pair being of a limited value at which the counteracting positive third order spherical aberration provided by said front concave surface results in a limited amount of excess positive transverse fifth order spherical aberration providing a very high aperture greater than F/0.75.