Invention Application
WO2013106456A1 SINGLE MODE SINGLE FREQUENCY LASER SYSTEM WITH HARMONIC GENERATION
审中-公开
具有谐波发生的单模单频激光系统
- Patent Title: SINGLE MODE SINGLE FREQUENCY LASER SYSTEM WITH HARMONIC GENERATION
- Patent Title (中): 具有谐波发生的单模单频激光系统
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Application No.: PCT/US2013/020866Application Date: 2013-01-09
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Publication No.: WO2013106456A1Publication Date: 2013-07-18
- Inventor: GAPONTSEV, Valentin , AVDOKHIN, Alexey , ANDRUSYAK, Oleksiy , GRAPOV, Yuri
- Applicant: IPG PHOTONICS CORPORATION , GAPONTSEV, Valentin , AVDOKHIN, Alexey , ANDRUSYAK, Oleksiy , GRAPOV, Yuri
- Applicant Address: Kateshov, Yuri 50 Old Webster Road Oxford, MA 01540 US
- Assignee: IPG PHOTONICS CORPORATION,GAPONTSEV, Valentin,AVDOKHIN, Alexey,ANDRUSYAK, Oleksiy,GRAPOV, Yuri
- Current Assignee: IPG PHOTONICS CORPORATION,GAPONTSEV, Valentin,AVDOKHIN, Alexey,ANDRUSYAK, Oleksiy,GRAPOV, Yuri
- Current Assignee Address: Kateshov, Yuri 50 Old Webster Road Oxford, MA 01540 US
- Agency: IPG PHOTONICS CORPORATION
- Priority: US61/584,395 20120109
- Main IPC: H01S3/098
- IPC: H01S3/098 ; H01S3/10
Abstract:
A method for converting the optical frequency of a single-mode, single-frequency laser source includes generating a linearly-polarized single-frequency seed laser signal at a fundamental frequency; amplifying the seed laser signal in an optical amplifier; coupling the amplified signal into an external cavity formed by at least two mirrors, one of the mirrors being installed on a piezo actuator; enhancing the coupled signal inside the external cavity by locking a resonance frequency of the cavity to the frequency of the seed laser by continuously adjusting the optical length of the cavity with the piezo actuator; and converting the frequency of the enhanced signal using a non-linear crystal placed in a beam path inside the cavity. A method for converting the optical frequency of a single-mode, single-frequency laser source, includes generating a linearly polarized single-frequency seed laser signal at a fundamental frequency, the seed laser being a diode laser configured to adjust the frequency in response to controllable pump current variations; amplifying the seed laser signal in an optical amplifier; coupling the amplified signal into an external cavity formed by at least two mirrors; enhancing the coupled signal inside the external cavity by locking the frequency of the diode seed laser to a resonance frequency of the cavity by continuously adjusting the pump current of the diode seed laser; and converting the frequency of the enhanced signal using a non-linear crystal placed in a beam path inside the cavity.
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