Optical objective lens system with variable disk thickness feature

Claim 2

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the correction lens system comprising a single positive lens element to divergent light rays coming from the light source, whereby the single positive lens element is moved toward the light source when the thickness of the disk increases, while the single positive lens element is moved toward an image point when the thickness of the disk decreases, and wherein the following relationships are required, f.sub.c >5 f.sub.M 1 r.sub.2 <0 2 where f C represents the focal length of the single positive lens element, f M represents the focal length of the objective lens, and r 2 represents the radius of curvature of the single positive lens element on the image side.

Claim 3

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the correction lens system comprising two positive lens elements to divergent light rays coming from the light source, whereby the two positive lens elements are moved toward the light source when the thickness of the disk increases, while the two positive lens elements are moved toward an image point when the thickness of the disk decreases, and wherein the correction lens system comprises two positive lens elements, whereby the following relationships are required, f.sub.CT >4 f.sub.M 3 r.sub.2 <0, r.sub.4 <0 4 where f CT represents the focal length of the compound lens of the two lens elements, r 1 , r 2 , r 3 , and r 4 represent radii of curvature of the spherical surfaces of the compound lens in that order from the light source, and f M represents the focal length of the objective lens.

Claim 4

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the correction lens system comprising two positive lens elements to divergent light rays coming from the light source, whereby the two positive lens elements are moved toward the light source when the thickness of the disk increases, while the two positive lens elements are moved toward an image point when the thickness of the disk decreases, and wherein the correction lens system comprises two positive lens elements, whereby the following relationships are required, f.sub.CT >4 f.sub.M 3 r.sub.2 <0, r.sub.4 <0 4 where f CT represents the focal length of the compound lens of the two lens elements, r 1 , r 2 , r 3 , and r 4 represent radii of curvature of the spherical surfaces of the compound lens in that order from the light source, and f M represents the focal length of the objective lens.

Claim 5

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the collection lens system comprises a first negative lens element and a second positive lens element to parallel light rays coming in from a collimator, and the aberration is improved by moving the first negative lens element and/or the second positive lens element on the optical axis, thus by modifying the distance on the optical axis between the first negative lens element and the second positive lens element and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, and wherein the following relationships are required, -f.sub.C1 <f.sub.C2 5 r.sub.1 <0 6 1.3 r.sub.2 <|r.sub.3 | 7 2 f.sub.M <-f.sub.C1 8 where f C1 is the focal length of the first negative lens element, f C2 is the focal length of the second positive lens element, f M is the focal length of the objective lens, and r 1 , r 2 , r 3 , and r 4 are radii of curvature of the first negative lens element and the second positive lens element in that order.

Claim 6

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the collection lens system comprises a first negative lens element and a second positive lens element to parallel light rays coming in from a collimator, and the aberration is improved by moving the first negative lens element and/or the second positive lens element on the optical axis, thus by modifying the distance on the optical axis between the first negative lens element and the second positive lens element and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, and wherein the following relationships are required, -f.sub.C1 <f.sub.C2 5 r.sub.1 <0 6 1.3 r.sub.2 <|r.sub.3 | 7 2 f.sub.M <-f.sub.C1 8 where f C1 is the focal length of the first negative lens element, f C2 is the focal length of the second positive lens element, f M is the focal length of the objective lens, and r 1 , r 2 , r 3 , and r 4 are radii of curvature of the first negative lens element and the second positive lens element in that order.

Claim 7

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the collection lens system comprises a first positive lens element and a second negative lens element to parallel light rays coming in from a collimator, and the aberration is improved by moving the first positive lens element and/or the second negative lens element on the optical axis, thus by modifying the distance on the optical axis between the first positive lens element and the second negative lens element and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk.

Claim 8

An optical objective lens system with a variable disk thickness feature comprising a correction lens system having one or more lens elements, a positive objective lens and a disk arranged in that order from the side of a light source, in which one or more lens elements of the correction lens system are moved on an optical axis to improve an aberration that has increased as a result of a variation in thickness of the disk and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk, whereby the objective lens improves the aberration with a combination of a reference disk thickness and a reference object distance, in which the object distance L IM with respect to the objective lens is based on infinity light rays (L IM =∞) that are parallel light rays, finite light rays (L IM <0) that are divergent light rays, or convergent light rays (L IM >0), wherein the collection lens system comprises a first positive lens element and a second negative lens element to parallel light rays coming in from a collimator, and the aberration is improved by moving the first positive lens element and/or the second negative lens element on the optical axis, thus by modifying the distance on the optical axis between the first positive lens element and the second negative lens element and the objective lens is moved by a slight distance on the optical axis to be in-focus state in response to the movement of the image point resulting from the variation in the thickness of the disk.

Claim 9

An optical objective lens system with a variable disk thickness feature according to claim 4, the distance on the optical axis between the first positive lens element and the second negative lens element is shortened when the thickness of the disk increases, while the distance on the optical axis between the first positive lens element and the second negative lens element, constituting the correction lens system, is lengthened when the thickness of the disk decreased.

Claim 10

An optical objective lens system with a variable disk thickness feature according to claim 4, the following relationships are required, f.sub.C1 >-f.sub.C2 9 1/r.sub.1 +1/r.sub.2 >0 10 1/f.sub.C2 <1/r3<0 11 3.4 f.sub.M <-f.sub.C2 12 where f C1 is the focal length of the first positive lens element, f C2 is the focal length of the second negative lens element, f M is the focal length of the objective lens, and r 1 , r 2 , r 3 , and r 4 are radii of curvature of the first positive lens element and the second negative lens element in that order.