Controlled frequency high power laser

Claim 2

A frequency controller laser comprising: means for providing laser radiation of a predetermined frequency; a laser medium; means for defining a regenerative path for laser radiation encompassing said laser medium; means for exciting said laser medium to a lasing condition whereby radiation from said medium travels on said path; means for amplifying the radiation within said laser medium and including an unstable cavity with said laser medium positioned therebetween and extending to between peripheral positions of said unstable cavity; means for maintaining a predetermined frequency relationship between said radiation of predetermined frequency and the laser radiation on said regenerative path in response to the lasing of said laser medium and in the absence of radiation of said predetermined frequency on said regenerative path.

Claim 3

The frequency controlled laser of claim 1 wherein said unstable cavity includes first and second mirrors having central apertures therethrough co-extensive with portions of said regenerative path either side of said laser medium.

Claim 4

The frequency controlled laser of claim 2 wherein said first mirror is concave and wherein said second mirror is convex.

Claim 5

The frequency controlled laser of claim 3 wherein said first and second mirrors are configured to provide standing wave patterns in the radiation in the laser medium between said first and second mirrors.

Claim 6

The frequency controlled laser of claim 1 further including a plurality of said means for defining a regenerative path, and corresponding laser mediums, excitation means, and means for maintaining a predetermined frequency relationship each in combination with means for diverting a portion of said laser radiation of predetermined frequency to corresponding ones of the plural means for maintaining a preset frequency relationship.

Claim 7

The frequency controlled laser of claim 1 wherein said means for maintaining a predetermined frequency relationship between said laser radiation of predetermined frequency and the laser radiation on said path includes means transmissive to said radiation along a frequency dependent angle positioned to pass the radiation of said predetermined frequency at an angle therefor and to pass the radiation on said path at an angle corresponding to its frequency.

Claim 8

The frequency controlled laser of claim 6 wherein said maintaining means includes means for positionally controlling said transmissive means to regulate the angle of passage therethrough for said radiation of predetermined frequency.

Claim 9

The frequency controlled laser of claim 6 wherein said transmissive means includes a filter providing a pattern of interference rings, a ring lying along said regenerative path and with a ring lying along the path of said radiation of predetermined frequency.

Claim 10

The frequency controlled laser of claim 8 wherein said radiation of predetermined frequency has a frequency corresponding to an absorption line for one material and the radiation on said regenerative path has a frequency separated from the other radiation of predetermined frequency by a frequency corresponding to a selected number of rings.

Claim 11

The frequency controlled laser of claim 9 wherein said transmissive means is constructed to provide said radiation on said regenerative path corresponding to a different absorption line for a second material.

Claim 12

The frequency controlled laser of claim 10 wherein said one material and said second material are the U-238 and U-235 isotopes of uranium.

Claim 13

The frequency controlled laser of claim 1 wherein said regenerative path includes means for reducing divergence in the radiation therealong.

Claim 14

The frequency controlled laser of claim 1 wherein said medium includes a solution flowing in a direction with the direction thereof, the direction of said regenerative path therethrough, and the direction of excitation thereof all mutually orthogonal.

Claim 15

A frequency locked laser amplifier comprising: a source of laser radiation of a predetermined frequency; a laser medium; an unstable cavity bounding said laser medium and comprising a concave mirror to one side of said laser medium and a convex mirror on an opposite side of said laser medium; said concave and convex mirrors having apertures therethrough; means for defining a closed path for the circulation of laser radiation through said apertures of said concave and convex mirrors and through said laser medium; a frequency selective element in the path of radiation of said closed path for laser radiation; means responsive to said radiation of predetermined frequency for controlling said frequency selective element to maintain a predetermined frequency relationship between said radiation of predetermined frequency and the radiation circulating in said closed path and to avoid transfer of radiation between said closed path and the path for the radiation of predetermined frequency; said laser medium extending through said unstable cavity beyond the region between the apertures in said concave and convex mirrors; said concave and convex mirrors in association with the apertures therethrough providing frequency control over the radiation passing from the region between said apertures in said laser medium to the region between reflective portions of said concave and convex mirrors for amplification therein at the frequency of radiation circulating in said closed path; said concave and convex mirrors providing an output beam of amplified laser radiation of the frequency of radiation circulating in said closed path.

Claim 16

A frequency locked laser amplifier comprising: a source of laser radiation of a predetermined frequency; a laser medium; an unstable cavity bounding said laser medium and comprising a concave mirror to one side of said laser medium and a convex mirror on an opposite side of said laser medium; said concave and convex mirrors having apertures therethrough; means for defining a closed path for the circulation of laser radiation through said apertures of said concave and convex mirrors and through said laser medium; a frequency selective element in the path of radiation of said closed path for laser radiation; means responsive to said radiation of predetermined frequency for controlling said frequency selective element to maintain a predetermined frequency relationship between said radiation of predetermined frequency and the radiation circulating in said closed path and to avoid transfer of radiation between said closed path and the path for the radiation of predetermined frequency; said laser medium extending through said unstable cavity beyond the region between the apertures in said concave and convex mirrors; said concave and convex mirrors in association with the apertures therethrough providing frequency control over the radiation passing from the region between said apertures in said laser medium to the region between reflective portions of said concave and convex mirrors for amplification therein at the frequency of radiation circulating in said closed path; said concave and convex mirrors providing an output beam of amplified laser radiation of the frequency of radiation circulating in said closed path.

Claim 17

The frequency locked laser of claim 14 wherein said concave and convex mirrors are cylindrical.

Claim 18

The frequency locked laser of claim 14 wherein said mirrors are dimensioned to provide an overlap between reflecting radiation such that a standing wave pattern develops.

Claim 19

The frequency locked laser of claim 14 wherein said controlling means includes a Fabry-Perot filter.

Claim 20

The frequency locked laser of claim 14 further including a transverse flow channel bordering said medium.

Claim 21

A frequency controlled laser comprising: means for providing first laser radiation; means for controlling the laser radiation to a frequency determined by an absorbtion line for a first isotope type of a material; a laser medium; means for defining a regenerative path for laser radiation encompassing said medium; means for exciting said laser medium to a lasing condition whereby radiation from said medium travels on said path; said controlling means including means for maintaining a frequency in said radiation on said regenerative path at a frequency corresponding to an absorption frequency for a further isotope type of said material in response to the control of said controlling means and in the absence, on said regenerative path, of radiation of said frequency determined by said first isotope type of said material.

Claim 22

A frequency controlled laser comprising: means for providing first laser radiation; means for controlling the laser radiation to a frequency determined by an absorbtion line for a first isotope type of a material; a laser medium; means for defining a regenerative path for laser radiation encompassing said medium; means for exciting said laser medium to a lasing condition whereby radiation from said medium travels on said path; said controlling means including means for maintaining a frequency in said radiation on said regenerative path at a frequency corresponding to an absorption frequency for a further isotope type of said material in response to the control of said controlling means and in the absence, on said regenerative path, of radiation of said frequency determined by said first isotope type of said material.

Claim 23

The laser of claim 19 wherein said material includes uranium.

Claim 24

The laser of claim 20 wherein said first isotope is the U-238 isotope and said further isotope is the U-235 isotope.

Claim 25

The frequency controlled laser of claim 21, wherein said maintaining means includes means for providing an interference pattern in response to said laser radiation of frequency determined by said first isotope type and of laser radiation on said regenerative path wherein the ring spacing for the radiation corresponds to the frequency difference between the absorption lines for said first and further isotope types.