http://rdf.ncbi.nlm.nih.gov/pubchem/patent/CN-115149383-A

Outgoing Links

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classificationCPCInventive http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-094046
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http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/H01S3-094
filingDate 2022-07-25-04:00^^<http://www.w3.org/2001/XMLSchema#date>
inventor http://rdf.ncbi.nlm.nih.gov/pubchem/patentinventor/MD5_80b5c14af9d64db5e3c059593ed9a531
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publicationDate 2022-10-04-04:00^^<http://www.w3.org/2001/XMLSchema#date>
publicationNumber CN-115149383-A
titleOfInvention A solid-state anti-Stokes Raman laser
abstract The invention discloses a solid anti-Stokes Raman laser, comprising a laser diode pumping source and a resonant cavity. The wavelength of the laser diode pumping source is 808 nm, which can be a laser diode side pumping source or a laser diode end surface pumping The source and the resonator include a back cavity mirror, a coupling mirror and an output mirror, a laser gain medium and a Q-switching device are placed between the back cavity mirror and the coupling mirror in the resonant cavity, and a Raman crystal is placed between the coupling mirror and the output mirror. The technical solution makes full use of the high peak power of the fundamental frequency Q-switched pulse and the high power density of the Raman light in the cavity, and uses the anisotropy of the Raman crystal to realize the collinear four-wave mixing, which improves the anti-Stokes performance. The performance of the Sraman laser solves the disadvantage that the existing laser beams cannot be collinear, and provides a new all-solid-state anti-Stokes Raman laser with small size, low cost and good stability.
priorityDate 2022-07-25-04:00^^<http://www.w3.org/2001/XMLSchema#date>
type http://data.epo.org/linked-data/def/patent/Publication

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Total number of triples: 23.