Passive absorptive resonator laser system and method

Claim 2

A laser system comprising: a means for generating pump light at a first frequency; a laser material in optical communication with said means for generating pump light, said laser material being disposed in an optical resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of said pump light.

Claim 3

The system of claim 1, wherein the reflective surfaces comprise a pair of mirrors each of which are reflective at said first frequency and said second frequency.

Claim 4

The system of claim 2, wherein the reflectivity of a first mirror at the first frequency equals approximately (1-e -2 αL)*(R2), where α is the absorption coefficient of the laser material, L is the distance between the mirrors, and R2 is the reflectivity of a second mirror at the first frequency.

Claim 5

The system of claim 1, wherein the laser material is Nd:YAG.

Claim 6

The system of claim 1, wherein the reflective surfaces are mirrors made of dielectric coatings.

Claim 7

The system of claim 1, wherein the resonator is a ring resonator having three reflective surfaces.

Claim 8

The system of claim 6, wherein a first reflective surface has a reflectivity at the first frequency equal to approximately (1-e -2 αL)*(R2)*R3), where α is the absorption coefficient of the laser material, L is the length of a beampath around the ring resonator, R2 is the reflectivity of the second reflective surface at the first frequency, and R3 is the reflectivity of the third reflective surface at the first frequency.

Claim 11

A laser system comprising: a pump laser generating a pump light at a first frequency; a lens focusing the pump light; a laser material in optical communication with the lens, said laser material being disposed in an optical resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having two reflective mirror coatings which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of said pump light.

Claim 12

A laser system comprising: a pump laser generating a pump light at a first frequency; a lens focusing the pump light; a laser material in optical communication with the lens, said laser material being disposed in an optical resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having two reflective mirror coatings which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of said pump light.

Claim 13

The system of claim 9, wherein the resonator is impedance matched to the pump laser.

Claim 14

A laser system comprising: a pump laser generating a pump light at a first frequency; a lens focusing the pump light; a laser material in optical communication with the lens, said laser material being disposed in an optical ring resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having three reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing more efficient absorption of said pump light.

Claim 15

A laser system comprising: a pump laser generating a pump light at a first frequency; a lens focusing the pump light; a laser material in optical communication with the lens, said laser material being disposed in an optical ring resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having three reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing more efficient absorption of said pump light.

Claim 16

The system of claim 11, wherein the ring resonator is impedance matched to the pump laser.

Claim 17

A laser system comprising: a pump laser generating a pump light at a first frequency; a laser material in optical communication with the lens, said laser material being disposed in an optical resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having a first and a second reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of the pump light, the reflectivities of a first reflective surface at the first frequency equals approximately (1-e -2 αL)*(R2), where α is the absorption coefficient of the laser material, L is the distance between the reflective surfaces, and R2 is the reflectivity of the second reflective surface at the first frequency and is in the range of 80-100%.

Claim 18

A laser system comprising: a pump laser generating a pump light at a first frequency; a laser material in optical communication with the lens, said laser material being disposed in an optical resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having a first and a second reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of the pump light, the reflectivities of a first reflective surface at the first frequency equals approximately (1-e -2 αL)*(R2), where α is the absorption coefficient of the laser material, L is the distance between the reflective surfaces, and R2 is the reflectivity of the second reflective surface at the first frequency and is in the range of 80-100%.

Claim 19

A laser system comprising: a pump laser generating a pump light at a first frequency; a laser material in optical communication with the pump laser, said laser material being disposed in an optical ring resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having three reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of said pump light, a first reflective surface having a reflectivity at the first frequency equal to approximately (1-e -2 αL)*(R2)*(R3), where α is the absorption coefficient of the laser material, L is the length of the beam path around the ring resonator, R2 is the reflectivity of the second reflective surface at the first frequency and is in the range of 80-100%, and R3 is the reflectivity of the third reflective surface at the first frequency and is in the range of 80-100%.

Claim 20

A laser system comprising: a pump laser generating a pump light at a first frequency; a laser material in optical communication with the pump laser, said laser material being disposed in an optical ring resonator, thereby causing said laser material to lase and produce laser light at a second frequency; and said optical resonator having three reflective surfaces which produce reflectivities such that resonance is established in said resonator at approximately said first frequency and approximately said second frequency, thereby providing a more efficient absorption of said pump light, a first reflective surface having a reflectivity at the first frequency equal to approximately (1-e -2 αL)*(R2)*(R3), where α is the absorption coefficient of the laser material, L is the length of the beam path around the ring resonator, R2 is the reflectivity of the second reflective surface at the first frequency and is in the range of 80-100%, and R3 is the reflectivity of the third reflective surface at the first frequency and is in the range of 80-100%.