http://rdf.ncbi.nlm.nih.gov/pubchem/patent/JP-2016514900-A
Outgoing Links
| Predicate | Object |
|---|---|
| classificationCPCInventive | http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-1305 http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-0816 http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H05G2-00 |
| classificationIPCInventive | http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02F1-37 http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02F1-01 http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/H01S3-10 |
| filingDate | 2013-09-12-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| publicationDate | 2016-05-23-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| publicationNumber | JP-2016514900-A |
| titleOfInvention | Optical resonator system |
| abstract | 【Task】 The first problem is that, as described above, it is difficult to control the resonance position of the resonator length necessary for laser amplification of 1000 times or more to be less than 1 mm. Accumulation was difficult. The second problem is that the mirror position information of the optical resonator to be controlled is obtained from the intensity of the accumulated laser, so the laser intensity in the optical resonator becomes very strong during laser amplification, so the thermal deformation of the mirror As a result, the resonance state fluctuates greatly, and as a result, it is difficult to accumulate a high-intensity laser. [Solution] It is selectively used for adjustment control of the optical resonator length of the optical resonator without amplifying the modulated wave or the harmonic generated from the oscillation laser. [Selection] Figure 1 |
| priorityDate | 2013-03-25-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| type | http://data.epo.org/linked-data/def/patent/Publication |
Incoming Links
Total number of triples: 20.