Prism polarizer

Claim 2

A prism polarizer for separating an incident light beam having P-polarization and S-polarization light rays, comprising: a pair of anisotropic crystal prisms, wherein each prism has a boundary surface, the boundary surface of a first prism of said pair faced to the boundary surface of the second prism, thus defining a facing plane; wherein each comprises a crystal which has an optical axis and an optical characteristic such that the difference between the square of the refractive index for light rays having a polarization plane parallel to the optical axis, and the square of the refractive index for light rays having a polarization plane perpendicular to the optical axis, is larger than 1; the angle of incidence of a beam, exiting one of said prisms, upon the boundary surface of said beam-exiting prism being equal to the Brewster angle for the refractive index for the P-polarization rays, so that the P-polarization rays are transmitted through said boundary surface of said beam-exiting prism, while the S-polarization rays are totally reflected at said boundary surface of said beam-exiting prism, thereby said incident beam being separated into two polarized beams, and wherein each prism is formed so that each of said two separated polarized beams is totally reflected within each respective prism and the separated polarized beams exit said respective prisms parallel with each other.

Claim 3

A prism polarizer according to claim 1, wherein each prism has an inlet end surface inclined with respect to the plane perpendicular to an inlet beam and each prism has an outlet end surface inclined with respect to the plane perpendicular to an outlet beam.

Claim 4

A prism polarizer according to claim 1, wherein each prism is made of titanium dioxide.

Claim 5

A prism polarizer according to claim 1, wherein a layer of air is formed between said boundary surfaces defining said facing plane of said pair of prisms.

Claim 6

A prism polarizer according to claim 1, wherein the S-polarized beam reflected at said boundary surface is again totally reflected within the prism so that this S-polarized beam leaves the prism parallel with said facing plane.

Claim 7

A prism polarizer according to claim 5, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is directly transmitted to said boundary surface and is incident on said boundary surface at the Brewster angle, without being reflected within the prism.

Claim 8

A prism polarizer according to claim 5, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is totally reflected once within the prism before said inlet beam is incident upon said boundary surface at the Brewster angle.

Claim 9

A prism polarizer according to claim 5, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is totally reflected two or more times within the prism before said inlet beam is incident upon said boundary surface at the Brewster angle.

Claim 10

An optical circulator comprising: two prism polarizers for separating incident light beams having P-polarization and S-polarization light rays, each prism polarizer including a pair of anisotropic crystal prisms, wherein each prism has a boundary surface, the boundary surface of a first prism of said pair faced to the boundary surface of the second prism, thus defining a facing plane; wherein each prism comprises a crystal which has an optical axis such that the difference between the square of the refractive index for light rays having a polarization plane parallel to the optical axis, and the square of the refractive index for light rays having a polarization plane perpendicular to the optical axis, is larger than 1; the angle of incidence of a beam, exiting one of said prisms, upon the boundary surface of said beam-exiting prism being equal to the Brewster angle for the refractive index for the P-polarization rays, so that the P-polarization rays are transmitted through said boundary surface of said beam-exiting prism, while the S-polarization rays are totally reflected at said boundary surface of said beam-exiting prism, thereby said incident beam being separated into two polarized beams, and wherein each prism of said pair of prisms has an inlet end surface and an outlet end surface, and each of said two separated polarized beams is totally reflected within each respective prism and the separated polarized beams exit said respective prisms parallel with each other; the outlet end surfaces of said two polarizers are faced to each other; a rotatory polarization device disposed between the two polarizers and arranged so that said device rotates the polarization plane of a polarized beam from one direction by 90°, while said device does not rotate the polarization plane of a polarized beam from the reverse direction; and wherein said inlet end surfaces of said prisms are used as an inlet and an outlet of said optical circulator.

Claim 11

An optical circulator comprising: two prism polarizers for separating incident light beams having P-polarization and S-polarization light rays, each prism polarizer including a pair of anisotropic crystal prisms, wherein each prism has a boundary surface, the boundary surface of a first prism of said pair faced to the boundary surface of the second prism, thus defining a facing plane; wherein each prism comprises a crystal which has an optical axis such that the difference between the square of the refractive index for light rays having a polarization plane parallel to the optical axis, and the square of the refractive index for light rays having a polarization plane perpendicular to the optical axis, is larger than 1; the angle of incidence of a beam, exiting one of said prisms, upon the boundary surface of said beam-exiting prism being equal to the Brewster angle for the refractive index for the P-polarization rays, so that the P-polarization rays are transmitted through said boundary surface of said beam-exiting prism, while the S-polarization rays are totally reflected at said boundary surface of said beam-exiting prism, thereby said incident beam being separated into two polarized beams, and wherein each prism of said pair of prisms has an inlet end surface and an outlet end surface, and each of said two separated polarized beams is totally reflected within each respective prism and the separated polarized beams exit said respective prisms parallel with each other; the outlet end surfaces of said two polarizers are faced to each other; a rotatory polarization device disposed between the two polarizers and arranged so that said device rotates the polarization plane of a polarized beam from one direction by 90°, while said device does not rotate the polarization plane of a polarized beam from the reverse direction; and wherein said inlet end surfaces of said prisms are used as an inlet and an outlet of said optical circulator.

Claim 12

An optical circulator according to claim 9, wherein each prism has an inlet end surface inclined with respect to the plane perpendicular to an inlet beam entering said at least one prism and each prism has an outlet end surface inclined with respect to the plane perpendicular to an outlet beam entering said at least one prism.

Claim 13

An optical circulator according to claim 9, wherein each prism of said pair of prisms is made of titanium dioxide.

Claim 14

An optical circulator according to claim 9, wherein a layer of air is formed between said boundary surfaces defining said facing plane of said pair of prisms.

Claim 15

An optical circulator according to claim 9, wherein the S-polarized beam reflected at said boundary surface is again totally reflected within the prism so that this S-polarized beam leaves the prism parallel with said facing plane.

Claim 16

An optical circulator according to claim 13, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is directly transmitted to said boundary surface and is incident on said boundary surface at the Brewster angle, without being reflected within the prism.

Claim 17

An optical circulator according to claim 13, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is totally reflected once within the prism before said inlet beam is incident upon said boundary surface at the Brewster angle.

Claim 18

An optical circulator according to claim 13, wherein at least one prism of said pair of prisms is of quadrilateral sectional shape, and formed so that an inlet beam entering said at least one prism is totally reflected two or more times within the prism before said inlet beam is incident upon said boundary surface at the Brewster angle.