Field curvature corrector

Claim 2

An optical system which (a) forms an image of an object, (b) has a positive power, and (c) has a limiting principal ray associated with the system's maximum field of view, said system comprising: at least one positive lens element; and a field curvature corrector unit having a positive power and at least one aspheric surface; wherein: (i) the exact field curvature (EFC) of said field curvature corrector unit computed along at least one principal ray of the optical system is positive, where the exact field curvature of the field curvature corrector unit is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the unit, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface; and (ii) the system is free of lens elements having a negative power which provide substantial correction of the field curvature of the lens system.

Claim 3

An optical system which (a) forms an image of an object, (b) has a positive power, and (c) has a limiting principal ray associated with the system's maximum field of view, said system comprising: at least one positive lens element; and a field curvature corrector unit having a positive power and at least one aspheric surface; wherein: (i) the exact field curvature (EFC) of said field curvature corrector unit computed along at least one principal ray of the optical system is positive, where the exact field curvature of the field curvature corrector unit is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the unit, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface; and (ii) the system is free of lens elements having a negative power, other than lens elements having a negative power which are associated with a color correcting doublet.

Claim 4

An optical system which (a) forms an image of an object, (b) has a positive power, and (c) has a limiting principal ray associated with the system's maximum field of view, said system comprising: at least one positive lens element; and a field curvature corrector unit having a positive power and at least one aspheric surface; wherein: (i) the exact field curvature (EFC) of said field curvature corrector unit computed along at least one principal ray of the optical system is positive, where the exact field curvature of the field curvature corrector unit is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the unit, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface; and (ii) the system is free of lens elements having a negative power, other than lens elements having a negative power which are associated with a color correcting doublet.

Claim 5

The optical system of claim 1 or 2 wherein the at least one principal ray of the optical system is the limiting principal ray.

Claim 6

The optical system of claim 1 or 2 wherein the field curvature corrector unit has a positive EFC for substantially all principal rays corresponding to relative field heights greater than about 0.8.

Claim 7

The optical system of claim 1 or 2 wherein the field curvature corrector unit has a positive EFC for substantially all principal rays whose heights at the surfaces of the unit are greater than about 2.5 times the heights of the axial marginal ray at those surfaces.

Claim 8

The optical system of claim 1 or 2 wherein Y/Y is greater than about 3.0 for all of the surfaces of the field curvature corrector unit, where Y is the height of the limiting principal ray at the surface and Y is the height of the axial marginal ray at the surface.

Claim 9

The optical system of claim 1 or 2 wherein the optical system has an aperture stop, a long conjugate side, and a short conjugate side and wherein the field curvature corrector unit is on the short conjugate side of the aperture stop.

Claim 10

The optical system of claim 1 or 2 wherein the field curvature corrector unit consists of a single lens element.

Claim 11

An optical system which forms an image of an object, said system having an image end, an object end, and a limiting principal ray associated with the system's maximum field of view, said system comprising: (a) a first unit at the object end which (i) forms an intermediate image of the object, (ii) has a positive power, and (iii) has an exit pupil, said first unit comprising a first field curvature corrector subunit and a second power subunit, said first field curvature corrector subunit having a positive power and comprising at least one aspheric surface; and (b) a second unit at the image end which reimages the intermediate image to form the image of the object, said second unit having an entrance pupil and a positive power; wherein the exact field curvature (EFC) of said first field curvature corrector subunit computed along at least one principal ray of the optical system is positive, where the exact field curvature of the field curvature corrector subunit is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the subunit, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface.

Claim 12

An optical system which forms an image of an object, said system having an image end, an object end, and a limiting principal ray associated with the system's maximum field of view, said system comprising: (a) a first unit at the object end which (i) forms an intermediate image of the object, (ii) has a positive power, and (iii) has an exit pupil, said first unit comprising a first field curvature corrector subunit and a second power subunit, said first field curvature corrector subunit having a positive power and comprising at least one aspheric surface; and (b) a second unit at the image end which reimages the intermediate image to form the image of the object, said second unit having an entrance pupil and a positive power; wherein the exact field curvature (EFC) of said first field curvature corrector subunit computed along at least one principal ray of the optical system is positive, where the exact field curvature of the field curvature corrector subunit is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the subunit, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface.

Claim 13

The optical system of claim 9 further comprising a pupil imaging unit located in the vicinity of the intermediate image which images the exit pupil of the first lens unit into the vicinity of the entrance pupil of the second lens unit.

Claim 14

The optical system of claim 9 or 10 wherein the at least one principal ray of the optical system is the limiting principal ray.

Claim 15

The optical system of claim 9 or 10 wherein the field curvature corrector subunit has a positive EFC for substantially all principal rays corresponding to relative field heights greater than about 0.8.

Claim 16

The optical system of claim 9 or 10 wherein the field curvature corrector subunit has a positive EFC for substantially all principal rays whose heights at the surfaces of the subunit are greater than about 2.5 times the heights of the axial marginal ray at those surfaces.

Claim 17

The optical system of claim 9 or 10 wherein Y/Y is greater than about 3.0 for all of the surfaces of the field curvature corrector subunit, where Y is the height of the limiting principal ray at the surface and Y is the height of the axial marginal ray at the surface.

Claim 18

The optical system of claim 9 or 10 wherein the optical system has an aperture stop, a long conjugate side, and a short conjugate side and wherein the field curvature corrector subunit is on the short conjugate side of the aperture stop.

Claim 19

The optical system of claim 9 or 10 wherein the field curvature corrector subunit consists of a single lens element.

Claim 20

The optical system of claim 9 or 10 wherein the second power subunit provides for correction of axial chromatic aberration.

Claim 21

The optical system of claim 17 wherein the second power subunit comprises a positive lens element and a negative lens element.

Claim 22

The optical system of claim 9 or 10 wherein the second unit consists of only positive lens elements.

Claim 23

The optical system of claim 19 wherein the second lens unit consists of a single positive lens element.

Claim 24

A compounded magnifier comprising an objective lens element having a positive power, an eyepiece lens element having a positive power, and a field curvature corrector element having a positive power, wherein the exact field curvature (EFC) of said field curvature corrector element computed along at least one principal ray of the magnifier is positive, where the exact field curvature of the field curvature corrector element is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the element, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface.

Claim 25

A compounded magnifier comprising an objective lens element having a positive power, an eyepiece lens element having a positive power, and a field curvature corrector element having a positive power, wherein the exact field curvature (EFC) of said field curvature corrector element computed along at least one principal ray of the magnifier is positive, where the exact field curvature of the field curvature corrector element is given by: EFC=-Σ(n'-n)c/nn' where the summation is taken over the surfaces of the element, and for each of said surfaces, n is the index of refraction on the object side of the surface, n' is the index of refraction on the image side of the surface, and c is the curvature of the surface at the intersection of the surface with the principal ray, c being positive if the center of curvature is on the image side of the surface.

Claim 26

The compounded magnifier of claim 21 further comprising a positive field lens element.

Claim 27

The compounded magnifier of claim 21 or 22 wherein the magnifier has an aperture stop and the field curvature corrector element is located at a substantial distance from the aperture stop.

Claim 28

The compounded magnifier of claim 23 wherein the magnifier has an object end and the field curvature corrector element is located in the region of said object end.

Claim 29

The compound magnifier of claim 21 or 22 further comprising a color correcting doublet.

Claim 30

The compound magnifier of claim 21 or 22 wherein the at least one principal ray of the magnifier is the limiting principal ray associated with the magnifier's maximum field of view.