Optical element and optical system
Abstract
The optical element includes a base member configured to have an optical surface, a concave-convex structure configured to have an average pitch smaller than a shortest wavelength of a use wavelength range, and an intermediate layer formed between the optical surface and the concave-convex structure, made of a material different from that of the concave-convex structure, and having a refractive index between those of the base member and the material of the concave-convex structure. The optical surface is formed into a shape having a rotational symmetry axis. A thickness of the intermediate layer or each of thicknesses of the intermediate layer and the concave-convex structure varies so as to increase as a distance from the rotational symmetry axis increases. The optical element has good anti-reflection performance not only at a central part of the optical surface having a small curvature radius but also at a peripheral part thereof.
Claims
exact text as granted — not AI-modified1 . An optical element comprising:
a base member configured to have an optical surface; a concave-convex structure configured to have an average pitch smaller than a shortest wavelength of a use wavelength range; and an intermediate layer formed between the optical surface and the concave-convex structure, made of a material different from that of the concave-convex structure, and having a refractive index between those of the base member and the material of the concave-convex structure, wherein the optical surface is formed into a shape having a rotational symmetry axis, and wherein a thickness of the intermediate layer or each of thicknesses of the intermediate layer and the concave-convex structure varies so as to increase as a distance from the rotational symmetry axis increases.
2 . The optical element according to claim 1 , wherein the concave-convex structure varies in structure in its thickness direction.
3 . The optical element according to claim 1 , wherein the following condition is satisfied:
λ/(8× n )≦ Dc ≦(2×λ)/ n
where Dc represents the thickness of the intermediate layer at a position of the rotational symmetry axis, n represents the refractive index of the intermediate layer, and λ represents the shortest wavelength of the used wavelength range.
4 . The optical element according to claim 1 , wherein the following conditions are satisfied:
0.3 ≦n ×sin(θ( h ))<1
Dc<D ( h )< Dc /cos(θ( h ))
where Dc represents the thickness of the intermediate layer at a position of the rotational symmetry axis, n represents the refractive index of the intermediate layer, D(h) represents the thickness of the intermediate layer at a h-position away from the rotational symmetry axis by a distance h, and θ(h) represents an angle that a light ray reaching the intermediate layer at the h-position in parallel with the rotational symmetry axis forms in the intermediate layer with a normal to a concave-convex structure-side most superficial surface of the intermediate layer at the h-position.
5 . An optical system comprising:
an optical element; wherein the optical element comprising: a base member configured to have an optical surface; a concave-convex structure configured to have an average pitch smaller than a shortest wavelength of a use wavelength range; and an intermediate layer formed between the optical surface and the concave-convex structure, made of a material different from that of the concave-convex structure, and having a refractive index between those of the base member and the material of the concave-convex structure, wherein the optical surface is formed into a shape having a rotational symmetry axis, and wherein a thickness of the intermediate layer or each of thicknesses of the intermediate layer and the concave-convex structure varies so as to increase as a distance from the rotational symmetry axis increases.
6 . The optical system according to claim 5 , wherein the following conditions are satisfied:
0.3 ≦n ×sin(ψ( h ))<1
Dc<D ( h )< Dc /cos(ψ( h ))
where Dc represents the thickness of the intermediate layer at a position of the rotational symmetry axis, n represents the refractive index of the intermediate layer, D(h) represents the thickness of the intermediate layer at a h-position away from the rotational symmetry axis by a distance h, and ψ(h) represents an angle that a light ray having an average incident angle among all light rays passing through the h-position of the intermediate layer in the optical system forms in the intermediate layer with a normal to a concave-convex structure-side most superficial surface of the intermediate layer at the h-position.
7 . The optical system according to claim 5 , further comprising:
an aperture stop; wherein the following conditions are satisfied:
0.3 ≦n ×sin(ζ( h ))<1
Dc<D ( h )< Dc /cos(ζ( h ))
where Dc represents the thickness of the intermediate layer at a position of the rotational symmetry axis, n represents the refractive index of the intermediate layer, D(h) represents the thickness of the intermediate layer at a h-position away from the rotational symmetry axis by a distance h, and ζ(h) represents an angle that a light ray passing through the h-position of the intermediate layer and a center of the aperture stop in the optical system forms in the intermediate layer with a normal to a concave-convex structure-side most superficial surface of the intermediate layer at the h-position.
8 . An optical apparatus comprising:
an optical system configured to include an optical element; wherein the optical element comprising: a base member configured to have an optical surface; a concave-convex structure configured to have an average pitch smaller than a shortest wavelength of a use wavelength range; and an intermediate layer formed between the optical surface and the concave-convex structure, made of a material different from that of the concave-convex structure, and having a refractive index between those of the base member and the material of the concave-convex structure, wherein the optical surface is formed into a shape having a rotational symmetry axis, and wherein a thickness of the intermediate layer or each of thicknesses of the intermediate layer and the concave-convex structure varies so as to increase as a distance from the rotational symmetry axis increases.Cited by (0)
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