Infrared polarization rotator and optical switch

Claim 2

An infrared polarization rotator comprising a medium, means for applying to said medium a linearly polarized beam of light to be polarization rotated, means for applying to said medium substantially collinearly with said beam a control beam of circularly polarized light, the frequencies of the beams being adjusted so that the frequency of one beam is nearly equal to the frequency of a one-photon transition between the ground state of a two-photon transition of the medium and some intermediate state and so that the sum of the frequencies of the two beams is sufficiently close to the frequency of said two-photon transition for substantial resonance dispersion to be produced as the beams traverse the medium, the polarization of the beams being selected in accordance with the requirements of the quantum-mechanical angular momentum selection rule which applies to said two-photon transition, characterized in that said medium is a crystalline solid the index of refraction of which does not substantially vary azimuthally about the direction of propagation of the radiation to be polarization rotated, said crystal having a structure of excited states of excitons, which exciton states are involved in said one-photon and two-photon transitions.

Claim 3

A polarization rotator according to claim 1 in which the medium is an uniaxial crystal.

Claim 4

A polarization rotator according to claim 1 in which the medium is a crystal of the wurzite type.

Claim 5

A polarization rotator according to claim 1 in which the medium is CdS.

Claim 6

A polarization rotator according to claim 1 in which the medium is a cubic crystal.

Claim 7

A polarization rotator according to claim 1 in which the medium is a compound selected from the group consisting of ZnS, CuCl, AgI, ZnSe, CdTe, and ZnTe.

Claim 8

An infrared polarization rotator comprising a medium, means for applying to said medium a beam of linearly polarized infrared radiation to be polarization rotated, means for applying to said medium substantially collinearly with said beam a control beam of linearly polarized light, the frequencies of the beams being adjusted so that the frequency of one beam is nearly equal to the frequency of a one-photon transition between the ground state of a two-photon transition of the medium and some intermediate state and so that the sum of the frequencies of the two beams is sufficiently close to the frequency of said two-photon transition for substantial resonance dispersion to be produced as the beams traverse the medium, characterized in that said medium is a birefringent solid crystal having a structure of excited states of excitons, which exciton states are involved in said one-photon and two-photon transitions, said crystal being oriented with its optic axis perpendicular to the direction of travel of said beams, said linearly polarized control beam of light being oriented so that its plane of polarization is substantially perpendicular to the optic axis, said beam of linearly polarized infrared radiation being oriented so that its plane of polarization is neither parallel nor perpendicular to the optic axis.

Claim 9

An infrared polarization rotator comprising a medium, means for applying to said medium a beam of linearly polarized infrared radiation to be polarization rotated, means for applying to said medium substantially collinearly with said beam a control beam of linearly polarized light, the frequencies of the beams being adjusted so that the frequency of one beam is nearly equal to the frequency of a one-photon transition between the ground state of a two-photon transition of the medium and some intermediate state and so that the sum of the frequencies of the two beams is sufficiently close to the frequency of said two-photon transition for substantial resonance dispersion to be produced as the beams traverse the medium, characterized in that said medium is a birefringent solid crystal having a structure of excited states of excitons, which exciton states are involved in said one-photon and two-photon transitions, said crystal being oriented with its optic axis perpendicular to the direction of travel of said beams, said linearly polarized control beam of light being oriented so that its plane of polarization is substantially perpendicular to the optic axis, said beam of linearly polarized infrared radiation being oriented so that its plane of polarization is neither parallel nor perpendicular to the optic axis.

Claim 10

A polarization rotator according to claim 7 in which the medium is a crystal of the wurzite type.

Claim 11

A polarization rotator according to claim 7 in which the medium is CdS.

Claim 12

A polarization rotator according to claim 7 in which the medium is crystal composed of two elements, one from group two of the periodic table of the elements and one from group six.

Claim 13

A polarization rotator according to claim 7 in which the medium is a crystal composed of three elements, one from group one of the periodic table of the elements, one from group three and one from group six.

Claim 14

A polarization rotator according to claim 7 in which the medium is a crystal selected from the class of compounds consisting of CdSe and ZnO.

Claim 15

A polarization rotator according to claim 7 in which the medium is a crystal selected from the class of compounds consisting of CuGaS 2 , CuInS 2 , and AgGaSe 2 .

Claim 16

A polarization rotator according to claim 7 in which the medium is a uniaxial crystal.