Aspherical lens for use in optical equipment

Claim 2

A single aspherical lens having spherical surface means and aspherical surface means for receiving parallel rays of incident light in one of the surface means, diverging or converging the rays of light while the rays of light are in the lens, and emanating parallel rays of emergent light from the other surface means.

Claim 3

A single aspherical lens according to claim 1 wherein the rays of incident light and the rays of emergent light are parallel to each other.

Claim 4

An aspherical lens according to claim 1, wherein said three-dimensional coordinate systems in an XYZ three-dimensional coordinate system and said aspherical lens being rotationally symmetrical around a Z-axis, said spherical surface being given by the following equations (a) and said aspherical surface by the following equations (b): (a) the coordinates (x 1 , y 1 , z 1 ) in the XYZ three dimensional coordinate system of a point on the spherical surface being expressed by: x.sub.1 =r.sub.0 sin θ cos φ y.sub.1 =r.sub.0 sin θ sin φ z.sub.1 =r.sub.0 cos θ where r 0 is the radius of curvature of the spherical surface, θ is the angle (-90°≦θ≦90°) formed in a plane containing the Z-axis and normal to an X-Y plane and between the Z-axis and a line connecting the origin of the coordinate system and at the point on the spherical surface, and θ is the angle (0°≦φ≦180°) formed in a plane parallel to the X-Y plane and between an X-axis and a line connecting said point and the Z-axis; and (b) the coordinates (x 2 , Y 2 , z 2 ) in the XYZ three-dimensional coordinate system of a point on the aspherical surface being expressed by: ##EQU5## where θ x is the angle at which incident light parallel to the Z-axis is refracted by the lens surface, δ is the thickness of the lens along a path therein of incident light parallel to the Z-axis and refracted by the lens surface, δ 0 is the thickness of the lens on the Z-axis, and n λ is the refractive index of the of the lens material with respect to light having a wavelength λ.

Claim 5

An aspherical lens for optical equipment, made of a transparent lens material and rotationally symmetrical around one axis of a three-dimensional coordinate system, said aspherical lens having a spherical and an aspherical surface along said one axis and the distance along each path of light between said spherical and aspherical surfaces is so determined that an incident angle of a light ray, parallel to said one axis at an incident point, on one of the spherical and aspherical surfaces becomes equal to an emergent angle of said light ray at an emergent point on the other of said surfaces, thereby diverging or converging parallel rays of incident light as emergent light rays parallel to said rays of incident light with a single lens.

Claim 6

An aspherical lens for optical equipment, made of a transparent lens material and rotationally symmetrical around one axis of a three-dimensional coordinate system, said aspherical lens having a spherical and an aspherical surface along said one axis and the distance along each path of light between said spherical and aspherical surfaces is so determined that an incident angle of a light ray, parallel to said one axis at an incident point, on one of the spherical and aspherical surfaces becomes equal to an emergent angle of said light ray at an emergent point on the other of said surfaces, thereby diverging or converging parallel rays of incident light as emergent light rays parallel to said rays of incident light with a single lens.

Claim 7

An aspherical lens according to claim 4, wherein said three-dimensional coordinate system is an XYZ three-dimensional coordinate system and said aspherical lens being rotationally symmetrical around a Z-axis, said spherical surface being given by the following equations (a) and said aspherical surface by the following equations (b): (a) the coordinates (x 1 , y 1 , z 1 ) in the XYZ three-dimensional coordinate system of a point on the spherical surface being expressed by: x.sub.1 =r.sub.0 sinθ cosφ y.sub.1 =r.sub.0 sinθ sinφ z.sub.1 =r.sub.0 cosθ where r 0 is the radius of curvature of the spherical surface, θ is the angle (-90°≦θ≦90°) formed in a plane containing the Z-axis and normal to an X-Y plane and between the Z-axis and a line connecting the origin of the coordinate system and the point on the spherical surface, and φ is the angle (0°≦φ≦180°) formed in a plane parallel to the X-Y plane and between an X-axis and a line connecting said point and the Z-axis; and (b) the coordinates (x 2 , y 2 , z 2 ) in the XYZ three-dimensional coordinate system of a point on the aspherical surface being expressed by: ##EQU6## where θ x is the angle at which incident light parallel to the Z-axis is refracted by the lens surface, δ is the thickness of the lens along a path therein of incident light parallel to the Z-axis and refracted by the lens surface, δ 0 is the thickness of the lens on the Z-axis, and nλ is the refractive index of the lens material with respect to light having a wavelength λ.