# US 5,708,672 A · Dual wavelength solid state laser > Agents: this data is available as JSON from the patentgrep API and MCP server — see https://patentgrep.com/llms.txt - Number: US 5,708,672 A - Document ID: US5708672A - Status: Granted - Kind: A - Application number: 08/593,251 - Filed: 1996-01-29 - Granted: 1998-01-13 - Earliest claimed: 1996-01-29 - Assignees: Laser Power Corporation - Inventors: Maurice A. Pessot; David E. Hargis - Web page: https://patentgrep.com/patent/US5708672A ## CPC - H01S 3/0627: {the resonator being monolithic, e.g. microlaser} - H01S 3/0604: {in the form of a plate or disc} - H01S 3/0809: {Two-wavelenghth emission} - H01S 3/094053: {Fibre coupled pump, e.g. delivering pump light using a fibre or a fibre bundle} - H01S 3/09415: {the pumping beam being parallel to the lasing mode of the pumped medium, e.g. end-pumping} - H01S 3/1611: {neodymium} - H01S 3/1673: {YVO4 [YVO]} - H01S: DEVICES USING THE PROCESS OF LIGHT AMPLIFICATION BY STIMULATED EMISSION OF RADIATION [LASER] TO AMPLIFY OR GENERATE LIGHT; DEVICES USING STIMULATED EMISSION OF ELECTROMAGNETIC RADIATION IN WAVE RANGES OTHER THAN OPTICAL ## Abstract A dual wavelength continuous wave (cw) solid state microlaser device that provides simultaneous laser action at a first and a second wavelength. The laser comprises a solid state gain material including a rare earth element having a first gain transition at the first wavelength and a second gain transition at the second wavelength. The gain material defines a block having a first face and a second, opposite face. A first reflective surface that is substantially reflective at both the first and second wavelengths is closely coupled to the first face. An output coupler provides a second reflective surface that is partially reflective at both the first and the second wavelengths, which is oriented with respect to the first reflective face to define an optical cavity through the first and second faces of the solid state gain material. An optical pump source is provided to end pump the solid state gain material with continuous pump radiation at a pump wavelength that is highly absorptive by the gain material. In some embodiments, the first reflective surface may be formed directly on the first face of the solid state gain material, and the second reflective surface may be formed directly on the second face of the solid state gain material. The resultant laser beam comprises two wavelengths each of which is believed to have a single longitudinal mode. In some embodiments the solid state gain material comprises a uniaxial crystal oriented within the optical cavity to provide polarized emissions for the first and second wavelengths. ## Claims ### Claim 1 A dual wavelength continuous wave (cw) solid state laser device comprising: a solid state gain material having a first gain transition at a first wavelength and a second gain transition at a second wavelength, said gain material defining a block having a first face and a second, opposite face; a first reflective surface closely coupled to said first face, said first reflective surface being substantially reflective at both said first and said second wavelengths; and an output coupler including a second reflective surface that is partially reflective at both said first and said second wavelengths, said second reflective face oriented with respect to said first reflective face to define an optical cavity through said first and second faces of said solid state gain material. ### Claim 2 (depends on 1) The solid state laser device of claim 1, and further comprising an optical pump source optically coupled through said first reflective face to end-pump said solid state gain material with continuous pump radiation at a pump wavelength that is highly absorptive by said gain material. ### Claim 3 (depends on 2) The solid state laser device of claim 2, wherein said first face of said solid state gain material is highly transmissive to said pump radiation and wherein said first reflective surface is formed on said first face. ### Claim 4 (depends on 2) The solid state laser device of claim 2, and further comprising an optical fiber having a first end coupled to said optical pump source and a second end coupled to said first reflective surface, so that said pump radiation is supplied through said optical fiber to pump said solid state gain material. ### Claim 5 (depends on 1) The solid state laser device of claim 1, wherein said first reflective surface is formed on said first face of said gain material. ### Claim 6 (depends on 5) The solid state laser device of claim 5, wherein said second reflective surface is formed on said second face of said gain material. ### Claim 7 (depends on 1) The solid state laser device of claim 1, wherein said second reflective surface is formed on said second face of said gain material. ### Claim 8 (depends on 1) The solid state laser device of claim 1, wherein said solid state gain material comprises a rare earth element. ### Claim 9 (depends on 8) The solid state laser device of claim 8, wherein said rare earth element comprises neodymium. ### Claim 10 (depends on 8) The solid state laser device of claim 8, wherein said solid state gain material comprises Nd:YVO.sub.4. ### Claim 11 (depends on 1) The solid state laser device of claim 1, wherein said solid state gain material comprises a uniaxial crystal oriented within said optical cavity to provide said first and second lasing polarizations for said first and said second wavelengths. ### Claim 12 (depends on 11) The solid state device of claim 11, wherein said uniaxial crystal is doped with a rare earth element. ### Claim 13 (depends on 12) The solid state laser device of claim 12, wherein said rare earth element comprises neodymium. ### Claim 14 (depends on 12) The solid state laser device of claim 12, wherein said uniaxial crystal comprises Nd:YVO.sub.4. ### Claim 15 A dual wavelength continuous wave (cw) solid state laser device comprising: a solid state gain material having a first gain transition at a first wavelength and a second gain transition at a second wavelength, said gain material defining a block having a first face and a second, opposite face, said first face having a reflective surface formed thereon that is substantially reflective at both said first and said second wavelengths; and an output coupler including a second reflective surface that is partially reflective at both said first and said second wavelengths, said second reflective face being oriented with respect to said first reflective face to define an optical cavity through said first and second faces of said solid state gain material. ### Claim 16 (depends on 15) The solid state laser device of claim 15, wherein said output coupler is formed on said second face of said gain material. ### Claim 17 (depends on 15) The solid state laser device of claim 15, and further comprising an optical pump source optically coupled through said first reflective face to end-pump said solid state gain material with continuous pump radiation at a pump wavelength that is highly absorptive by said gain material, and wherein said first face is highly transmissive to said pump radiation. ### Claim 18 (depends on 17) The solid state laser device of claim 17, and further comprising an optical fiber having a first end coupled to said optical pump source and a second end coupled to said first face of said gain material, so that said pump radiation is supplied through said optical fiber to pump said solid state gain material. ### Claim 19 (depends on 15) The solid state laser device of claim 15, wherein said solid state gain material comprises a rare earth element. ### Claim 20 (depends on 19) The solid state laser device of claim 19, wherein said rare earth element comprises neodymium. ### Claim 21 (depends on 19) The solid state laser device of claim 19, wherein said solid state gain material comprises Nd:YVO.sub.4. ### Claim 22 (depends on 19) The solid state laser device of claim 19, wherein said solid state gain material comprises a uniaxial crystal oriented within said optical cavity to provide said first and second lasing polarizations for said first and said second wavelengths. ### Claim 23 (depends on 22) The solid state device of claim 22, wherein said uniaxial crystal is doped with a rare earth element. ### Claim 24 (depends on 22) The solid state laser device of claim 22, wherein said rare earth element comprises neodymium. ### Claim 25 (depends on 23) The solid state laser device of claim 23, wherein said uniaxial crystal comprises Nd:YVO.sub.4. ### Claim 26 A dual wavelength continuous wave (cw) solid state laser device comprising: a solid state gain material comprising a rare earth element having a first gain transition at a first wavelength and a second gain transition at a second wavelength, said gain material defining a block having a first face and a second, opposite face, said first face having a reflective surface formed thereon that is substantially reflective at both said first and said second wavelengths; an optical pump source optically coupled through said first face to end-pump said solid state gain material with continuous pump radiation at a pump wavelength that is highly absorptive by said gain material; and an output coupler including a second reflective surface that is partially reflective at both said first and said second wavelengths, said second reflective face oriented with respect to said first reflective face to define an optical cavity through said first and second faces of said solid state gain material. ### Claim 27 (depends on 26) The solid state laser device of claim 26, wherein said output coupler is formed on said second face of said gain material. ### Claim 28 (depends on 26) The solid state laser device of claim 26, and further comprising an optical fiber having a first end coupled to said optical pump source and a second end coupled to said first face of said gain material, so that said pump radiation is supplied through said optical fiber to pump said solid state gain material. ### Claim 29 (depends on 26) The solid state laser device of claim 26, wherein said solid state gain material comprises Nd:YVO.sub.4. ### Claim 30 (depends on 29) The solid state laser device of claim 29, wherein said first wavelength is approximately 1064 nm and said second wavelength is approximately 1342 nm. ### Claim 31 A method of generating continuous wave (cw) laser radiation in a cavity including a block of solid state laser material comprising the steps of: a) continuously end-pumping the block of solid state laser material with pump radiation; b) within said cavity, simultaneously generating substantial first cw laser radiation at a first wavelength and substantial second cw laser radiation at a second wavelength; and c) outputting said first and second cw laser radiation from said cavity. ### Claim 32 (depends on 31) The method of claim 31, and further comprising the step of absorbing said pump radiation within a short absorption distance into said solid state laser material so that said first and said second laser radiations have a single longitudinal mode. ### Claim 33 (depends on 31) The method of claim 31, wherein said first cw laser radiation is generated at a first polarization and said second cw laser radiation is generated at a second, approximately parallel polarization. ### Claim 34 (depends on 31) The method of claim 31, wherein said first cw laser radiation is generated at a first polarization and said second cw laser radiation is generated at a second, approximately perpendicular polarization. ### Claim 35 (depends on 31) The method of claim 31, wherein said step b includes generating said first cw laser radiation using a first transition of a neodymium ion and generating said second cw laser radiation using a second transition of a neodymium ion. ### Claim 36 (depends on 35) The method of claim 35, wherein said first transition comprises the .sup.4 F.sub.3/2 to .sup.4 I.sub.11/2 transition and the second transition comprises the .sup.4 F.sub.3/2 .sup.4 I.sub.13/2 transition. ### Claim 37 (depends on 35) The method of claim 35, wherein said gain material comprises Nd:YVO.sub.4 and said first transition is centered at approximately 1064 nm and said second transition is centered at approximately 1342 nm.