Single-frequency monolithic nonplanar ring laser and method for determining same

Claim 2

A monolithic nonplanar ring laser resonator constructed from a single piece of optically isotropic solid state laser material characterized by a non-zero Verdet constant and several facets which determine a closed internal nonplanar optical path including six points of reflection for propagating light around said internal nonplanar optical path, said optical path being symmetrical about a plane which passes between the two most widely separated points of reflection.

Claim 3

The laser resonator of claim 1 wherein said six points of reflection include: five total internal reflections within the laser host material; and one coupler reflection which explicitly avoids total internal reflection for admitting pump energy into said resonator and for coupling laser emission out of said resonator.

Claim 4

The laser resonator as claimed in claim 2 wherein one of said six points of reflection is displaced from the plane which all other reflections share in common for inducing image rotation and an associated reciprocal polarization rotation for light propagating around said internal nonplanar optical path.

Claim 5

The laser resonator as claimed in claim 3 further includes: means for applying a magnetic field substantially aligned with a major axis of the resonator for inducing non-reciprocal polarization rotation, said non-reciprocal polarization rotation combining with total internal reflection differential phase shifts and said associated reciprocal polarization rotation to produce a propagation direction dependent degree of net polarization rotation.

Claim 6

The laser resonator as claimed in claim 4 wherein said coupler reflection includes a multi-layered dielectric coating for providing partial transmission of useful laser output and for providing partial polarization to discriminate between differentially rotated internal polarization states.

Claim 7

The laser resonator as claimed in claim 1 including an external laser source for providing a laser pumping source of suitable wavelength and appropriate focusing optics for efficiently end-pumping said monolithic nonplanar ring laser.

Claim 8

A laser resonator as claimed in claim 6 wherein the refractive index of the laser host material is greater than 1.471.

Claim 9

A laser resonator as claimed in claim 7 wherein said facets are angled to reduce output beam astigmatism and eccentricity.

Claim 10

A laser resonator as claimed in claim 7 wherein said facets are angled to improve mode overlap between a fundamental laser mode and said laser source pump beam and promote fundamental transverse mode lasing.

Claim 11

A laser resonator as claimed in claim 7 wherein the laser host material is Neodymium-doped glass.

Claim 12

The laser resonator as claimed in claim 10 wherein said facets are angled for providing a net differential loss greater than 10 ppm for available magnetic field strengths to achieve unidirectional lasing in laser glass.

Claim 13

The laser resonator as claimed in claim 10 wherein said facets are angled for providing a net differential loss greater than 100 ppm for available magnetic field strengths to achieve unidirectional lasing in YAG.

Claim 14

The laser resonator as claimed in claim 10 wherein the refractive index is approximately 1.52, the Verdet constant is approximately 1.1×10 -3 rad/mm.Telsa, the internal angle of incidence at said coupler reflection is approximately 38°, a first and fifth total internal reflection angles are approximately 65°, a second and fourth total internal reflection angles are approximately 61.7°, a third total internal reflection angle is approximately 68.6°, an out of plane tilt angle is approximately 5.05° and the overall length of said resonator is approximately 8.6 mm.

Claim 15

The laser resonator as claimed in claim 7 wherein the external laser source is a semiconductor diode laser.

Claim 16

The laser resonator as claimed in claim 7 wherein unidirectional single frequency lasing is obtained when said applied magnetic field strength exceeds approximately 30 Gauss.

Claim 17

An Nd:glass monolithic nonplanar ring oscillator having an optically isotropic solid state laser body for propagating laser radiation about a nonplanar ring path internal to said laser body and a coupler for input of pmp radiation and output of a portion of said laser radiation from said laser body, comprising: means for propagating said laser radiation about said ring light path so that said light ring path comprises six reflections, said six reflections including five total internal reflections and one reflection at said coupler, said six reflection nonplanar ring light path being formed by the geometry of said laser body, said laser body being made out of Nd:glass and said light ring path being symmetric about a perpendicular plane intersecting said ring light path; and means for applying a magnetic field to said Nd:glass laser body, said magnetic field operating in conjunction with the geometry of said laser body and a partial polarizer means located in said ring light path to induce unidirectional traveling wave oscillation of said emitted laser radiation.

Claim 18

An Nd:glass monolithic nonplanar ring oscillator having an optically isotropic solid state laser body for propagating laser radiation about a nonplanar ring path internal to said laser body and a coupler for input of pmp radiation and output of a portion of said laser radiation from said laser body, comprising: means for propagating said laser radiation about said ring light path so that said light ring path comprises six reflections, said six reflections including five total internal reflections and one reflection at said coupler, said six reflection nonplanar ring light path being formed by the geometry of said laser body, said laser body being made out of Nd:glass and said light ring path being symmetric about a perpendicular plane intersecting said ring light path; and means for applying a magnetic field to said Nd:glass laser body, said magnetic field operating in conjunction with the geometry of said laser body and a partial polarizer means located in said ring light path to induce unidirectional traveling wave oscillation of said emitted laser radiation.

Claim 19

The Nd:glass monolithic nonplanar ring oscillator of claim 16 comprises means for inducing single frequency unidirectional traveling wave oscillation of said laser radiation including at least one of said reflections being at an oblique angle from a multi-layer dielectric output coupler and a partial polarization means for producing high loss in one direction of propagation and low loss in the other direction of propagation of said light in said symmetric ring path, said single frequency unidirectional oscillation being produced by the combined effects of said symmetric nonplanar ring path, the applied magnetic field and said partial polarizer means.

Claim 20

The Nd:glass monolithic nonplanar ring oscillator of claim 17 wherein the partial polarizer means are located at said coupler.

Claim 21

The Nd:glass monolithic nonplanar ring oscillator of claim 18 wherein said applied magnetic field exceeds 30 Gauss.

Claim 22

The Nd:glass monolithic nonplanar ring oscillator of claim 19 wherein the range of the angle of incidence at said coupler reflection for optimal performance of said Nd:glass laser body having said six reflections is 37°-41°.

Claim 25

The method for a monolithic nonplanar ring oscillator of claim 21 further comprises the step of: designating an optimal range of angle of incidence of said pumping beam to be between 30 and 39 degrees for said six reflection nonplanar ring when said laser material has an index of refraction of approximately 1.6.

Claim 26

The method for a monolithic nonplanar ring oscillator of claim 21 further comprises the step of: designating an optimal range of angle of incidence of said pumping beam to be between 41 and 43 degrees for said six reflection nonplanar ring when said laser material has an index of refraction of approximately 1.48.

Claim 27

The method for a monolithic nonplanar ring oscillator of claim 21 further comprising the step of: designating an optimal range of angle of incidence at said pumping beam to be between 25 and 27 degrees for said six reflection nonplanar ring when said laser material has an index of refraction of approximately 1.7.

Claim 28

The method for a monolithic nonplanar oscillator of claim 21 further comprises the step of: designating an optimal range of angle of incidence of said pumping beam to be between 37 and 41 degrees for said six reflection nonplanar ring when said laser material has an index of refraction of approximately 1.5.