Monolithic total internal reflection optical resonator

Claim 2

A monolithic resonator comprising: (a) means defining a block of a solid-state medium for resonating optical radiation having at least three facets for supporting optical radiation as a Gaussian beam internally of said block, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which the facets are to be located to cause total internal reflection of a Gaussian beam; and (b) coupling means positioned adjacent said block for transmission of a beam of optical radiation between said coupling means and said block via frustrated total internal reflection.

Claim 3

The monolithic resonator of claim 1 wherein said block generally has a polyhedral shape providing a ring path for a Gaussian beam.

Claim 4

The monolithic resonator of claim 1 further including means for varying the distance between said block and said coupling means to correspondingly vary the optical coupling therebetween.

Claim 5

The monolithic resonator of claim 1 wherein at least one of said facets is convex.

Claim 6

The monolithic resonator of claim 1 wherein the material of said block is selected to provide non-linear interaction of optical radiation therewith.

Claim 7

The monolithic resonator of claim 1 further including means for changing the resonant frequency of the Gaussian beam supported in said block.

Claim 8

The monolithic resonator of claim 6 further including a laser for directing optical radiation having at least one unknown frequency at said coupling means to be fed by the latter into said block, and said means for changing the resonant frequency of the Gaussian beam supported in said block includes means for sweeping said frequency.

Claim 9

The monolithic resonator of claim 1 wherein the material of said block is selected to be linear.

Claim 10

The monolithic resonator of claim 8 wherein said material is silica.

Claim 11

The monolithic resonator of claim 9 wherein said coupling means also is positioned relative to said block to cause radiation that has oscillated within said block as a Gaussian beam to transfer to said coupling means via frustrated total internal reflection for leaving said resonator.

Claim 12

A monolithic resonator comprising: (a) a one piece polyhedral block of a solid-state medium for resonating optical radiation, which block is adapted to support oscillation of optical radiation as a Gaussian beam and has at least three facets for optically interacting internally of said block with said beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation; (b) an optical radiation coupler positioned adjacent said polyhedral block so as to cause radiation to enter said block for said oscillation via frustrated total internal reflection; and (c) means for changing the frequency of the radiation which resonates in said block.

Claim 13

A monolithic resonator comprising: (a) a one piece polyhedral block of a solid-state medium for resonating optical radiation, which block is adapted to support oscillation of optical radiation as a Gaussian beam and has at least three facets for optically interacting internally of said block with said beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation; (b) an optical radiation coupler positioned adjacent said polyhedral block so as to cause radiation to enter said block for said oscillation via frustrated total internal reflection; and (c) means for changing the frequency of the radiation which resonates in said block.

Claim 14

The monolithic resonator of claim 11 further including means for varying the distance between at least one of said facets and said coupler to correspondingly vary the optical coupling therebetween.

Claim 15

The monolithic resonator of claim 11 wherein the material of said block is selected to be non-linear.

Claim 16

The monolithic resonator of claim 11 wherein the material of said block is selected to be linear.

Claim 17

The monolithic resonator of claim 11 wherein said material is silica.

Claim 18

The monolithic resonator of claim 15 wherein said body comprises fused silica.

Claim 19

The monolithic resonator of claim 11 further including a laser for directing optical radiation having at least one unknown frequency at said coupler to be fed by the latter into said block, and wherein said changing means include means for sweeping the frequency of the radiation which resonates in said block.

Claim 20

A spectrum analyzer comprising: (a) means for supplying an output beam of optical radiation that includes at least one unknown frequency; (b) a one piece polygonal block of a solid-state medium for resonating optical radiation, which block is adapted to support optical radiation as a Gaussian beam therein and has at least three facets for optically interacting internally of said block with said Gaussian beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation as a Gaussian beam; (c) an optical radiation input/output coupler positioned in the path of said output beam and adjacent said polygonal block so as to cause radiation from said beam to enter said block via frustrated total internal reflection for oscillation therein as a Gaussian beam and to leave said block through said coupler via frustrated total internal reflection; (d) means for sweeping the frequency of the optical radiation which can resonate in said block; and (e) means for detecting resonance of optical radiation in said block, thereby to indicate said unknown frequency.

Claim 21

A spectrum analyzer comprising: (a) means for supplying an output beam of optical radiation that includes at least one unknown frequency; (b) a one piece polygonal block of a solid-state medium for resonating optical radiation, which block is adapted to support optical radiation as a Gaussian beam therein and has at least three facets for optically interacting internally of said block with said Gaussian beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation as a Gaussian beam; (c) an optical radiation input/output coupler positioned in the path of said output beam and adjacent said polygonal block so as to cause radiation from said beam to enter said block via frustrated total internal reflection for oscillation therein as a Gaussian beam and to leave said block through said coupler via frustrated total internal reflection; (d) means for sweeping the frequency of the optical radiation which can resonate in said block; and (e) means for detecting resonance of optical radiation in said block, thereby to indicate said unknown frequency.

Claim 22

The spectrum analyzer of claim 18 wherein at least one facet of said block is convex to enhance stability of the resonator modes of said Gaussian beam.

Claim 23

The spectrum analyzer of claim 18 wherein said block of a solid-state resonating medium is fused silica.

Claim 24

A non-linear optical device comprising: (a) means for supplying a beam of optical radiation having a frequency to be converted; (b) a one piece polyhedral block of a non-linear solid-state medium for resonating optical radiation, which block is adapted to support oscillation of optical radiation at a frequency associated with the frequency of said beam, as a Gaussian beam and has at least three facets for optically interacting internally of said block with said Gaussian beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation within said block as a Gaussian beam; and (c) an optical radiation coupler positioned in the path of said Gaussian beam and adjacent said polyhedral block so as to cause radiation from said Gaussian beam to couple with said block via frustrated total internal reflection.

Claim 25

A non-linear optical device comprising: (a) means for supplying a beam of optical radiation having a frequency to be converted; (b) a one piece polyhedral block of a non-linear solid-state medium for resonating optical radiation, which block is adapted to support oscillation of optical radiation at a frequency associated with the frequency of said beam, as a Gaussian beam and has at least three facets for optically interacting internally of said block with said Gaussian beam, the material of said block at said facets having an index of refraction selected relative to the index of refraction of the medium within which said facets are to be located to cause total internal reflection of radiation within said block as a Gaussian beam; and (c) an optical radiation coupler positioned in the path of said Gaussian beam and adjacent said polyhedral block so as to cause radiation from said Gaussian beam to couple with said block via frustrated total internal reflection.

Claim 26

The non-linear optical device of claim 21 wherein said block is adapted to support oscillation of optical radiation at said converted frequency as a Gaussian beam.

Claim 27

The non-linear optical device of claim 21 wherein said block is adapted to support oscillation of optical radiation as a Gaussian mode at a frequency which interacts with said Gaussian beam.

Claim 28

In a method of producing a high Finesse resonator Gaussian beam of optical radiation, the steps of: (a) providing a block of a solid state resonating medium, which block is shaped to Support oscillation of optical radiation as a Gaussian beam and has at least three facets for optically interacting internally of said block with said beam; and (b) polishing each of said facets to cause total internal reflection thereat of a Gaussian beam within said block when said facets are located within a portion of a medium having a particular index of refraction selected relative to the index of refraction of the material of said block.

Claim 29

In a method of producing a high Finesse resonator Gaussian beam of optical radiation, the steps of: (a) providing a block of a solid state resonating medium, which block is shaped to Support oscillation of optical radiation as a Gaussian beam and has at least three facets for optically interacting internally of said block with said beam; and (b) polishing each of said facets to cause total internal reflection thereat of a Gaussian beam within said block when said facets are located within a portion of a medium having a particular index of refraction selected relative to the index of refraction of the material of said block.

Claim 30

The method of claim 24 further including the step of providing a convex outward curve on at least one of said facets to enhance the stability of the resonator modes of a Gaussian beam oscillating within said block.

Claim 31

The method of claim 24 wherein said step of polishing includes polishing each of said facets to the finish necessary to provide a total scattering loss for a selected frequency of optical radiation within said block that is less than the intrinsic absorption within said block of said frequency.

Claim 32

A high Finesse resonator of optical radiation produced by the method of claim 24.