Piezo-electrically tuned optical resonator and laser using same

Claim 2

In a method for piezo-electrically tuning an optical resonator, the steps of: applying a voltage across a piezo-electric element having an interface bonded to and overlaying at least a portion of a solid state member of an optical resonator such that the applied voltage tends to change the area of the bonded interface for transmitting a resultant field of forces into the overlaid portion of the solid state member of the optical resonator through the bonded interface for producing a stress-related change in the index of refraction and the dimensions of at least a portion of the optical resonator for tuning the frequency for an optical resonant mode of said optical resonator.

Claim 3

The method of claim 1 wherein the solid state member of the optical resonator is an optically transparent faceted member of solid state material with the facets disposed and arranged for reflecting optical wave energy therebetween within the faceted member to define a monolithic optical resonator tuned by the applied voltage.

Claim 4

The method of claim 2 including making the optical transparent faceted member of a laser gain material; optically pumping the laser gain material to produce lasant transitions and emission of lasant radiation; resonating the emitted lasant radiation within the monolithic optical resonator; and coupling a portion of the resonated lasant radiation out of the monolithic optical resonator for providing a monolithic laser source of lasant radiation, the frequency of which is tunable in response to the amplitude of the applied voltage.

Claim 5

The method of claim 3 including the step of: arranging and disposing the facets of the faceted member of solid state gain material for reflecting the optical wave energy therebetween and around in a closed path to define an optical ring laser tuned by the applied voltage.

Claim 6

The method of claim 4 including the step of: arranging one of the facets of the faceted member of solid state laser gain material to be outof and generally overlaying the closed path of the resonated lasant radiation to define a tuning facet; and bonding the piezo-electric element to the tuning facet through which the piezo-electrically produced tuning force fields are transmitted into the ring laser for frequency tuning same.

Claim 7

In a piezo-electrically tuned optical resonator: optical resonator means for resonating optical wave energy therein and including a solid state optically transparent member for passing therethrough the resonated optical wave energy and said transparent member having a tuning facet for passing therethrough tuning forces for tuning the resonant frequency of the resonated optical wave energy; and piezo-electric means including a piezo-electric member bonded in force-exchanging relation with said tuning facet of said optically transparent member of said optical resonator means and being responsive to a voltage applied across said piezo-electric member for transmitting resultant force vectors directed predominantly parallel to the surface of said tuning facet into said optically transparent member through said tuning facet for producing a stress-related change in the index of refraction and dimensional change of said optically transparent member for tuning the frequency of an optically resonant mode of said optical resonator means.

Claim 8

In a piezo-electrically tuned optical resonator: optical resonator means for resonating optical wave energy therein and including a solid state optically transparent member for passing therethrough the resonated optical wave energy and said transparent member having a tuning facet for passing therethrough tuning forces for tuning the resonant frequency of the resonated optical wave energy; and piezo-electric means including a piezo-electric member bonded in force-exchanging relation with said tuning facet of said optically transparent member of said optical resonator means and being responsive to a voltage applied across said piezo-electric member for transmitting resultant force vectors directed predominantly parallel to the surface of said tuning facet into said optically transparent member through said tuning facet for producing a stress-related change in the index of refraction and dimensional change of said optically transparent member for tuning the frequency of an optically resonant mode of said optical resonator means.

Claim 9

The optical resonator of claim 6 wherein said optically transparent member of said optical resonator means is faceted with said facets disposed and arranged for reflecting optical wave energy therebetween within said faceted member to define a monolithic optical resonator tuned by the voltage applied to said piezo-electric means.

Claim 10

The optical resonator of claim 7 wherein said facets are disposed and arranged for reflecting optical wave energy therebetween and around in a closed path within said faceted member to define a monolithic optical ring resonator.

Claim 11

The optical resonator of claim 7 wherein said member is made of a laser gain material; optical pumping means for optical pumping said laser gain material for producing lasant transitions and emission of lasant radiation for exciting a resonant optical mode of said optical resonator means; and output coupling means for coupling a portion of the resonated lasant radiation out of said monolithic optical resonator for providing a monolithic laser source of lasant radiation, the frequency of which is tunable in response to the amplitude of the voltage applied to said piezo-electric means.

Claim 12

The optical resonator of claim 9 wherein said facets are disposed and arranged for reflecting optical wave energy therebetween and around a closed path within said faceted member to define a monolithic optical ring resonator.

Claim 13

The optical resonator of claim 10 wherein said tuning facet of said faceted member of laser gain material is disposed out of and generally overlaying the closed path of the resonated lasant radiation; and said piezo-electric element being bonded to and overlaying said tuning facet.

Claim 14

The optical resonator of claim 10 including: magnet means for applying a magnetic field to said monolithic laser ring resonator for producing a Faraday rotation effect therein to preferentially attenuate resonated lasant optical radiation travelling in a direction counter to said output optical energy within said optical resonator.

Claim 15

In a ring laser: a faceted member of optically transparent lasant material; a plurality of said facets of said member of lasant material being disposed and oriented for reflecting optical energy internally to said member around in a non-planar closed ray path within said member to define an optical ring resonator; a coupler one of said internally reflecting facets serving to couple input and output optical energy into and out of said ring resonator along divergent input and output ray paths; a magnet for applying a magnetic field to said faceted member for producing a Faraday rotation effect therein to preferentially attenuate optical wave energy travelling within said resonator in a direction counter to that of the output optical energy; a source of optical pumping energy directing said pumping energy into said faceted member through said coupler facet and along said input ray path; and a sheet of piezo-electric material bonded to a tuning one of said facets of said faceted member for transmitting tuning force vectors predominantly directed in the plane of the surface of and through said tuning facet in response to an applied voltage for tuning the frequency of the output optical energy.

Claim 16

In a ring laser: a faceted member of optically transparent lasant material; a plurality of said facets of said member of lasant material being disposed and oriented for reflecting optical energy internally to said member around in a non-planar closed ray path within said member to define an optical ring resonator; a coupler one of said internally reflecting facets serving to couple input and output optical energy into and out of said ring resonator along divergent input and output ray paths; a magnet for applying a magnetic field to said faceted member for producing a Faraday rotation effect therein to preferentially attenuate optical wave energy travelling within said resonator in a direction counter to that of the output optical energy; a source of optical pumping energy directing said pumping energy into said faceted member through said coupler facet and along said input ray path; and a sheet of piezo-electric material bonded to a tuning one of said facets of said faceted member for transmitting tuning force vectors predominantly directed in the plane of the surface of and through said tuning facet in response to an applied voltage for tuning the frequency of the output optical energy.