| Predicate |
Object |
| assignee |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_0e73e26f0d96cd7eb35aaf8c644c5247
http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_f5983413052c79c2fa9d56ff8a3f4a61
http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_e43aab565d3aa63d979fad55f8e36ad1
http://rdf.ncbi.nlm.nih.gov/pubchem/patentassignee/MD5_9c325b062811d52c41937a8f31460c52 |
| classificationCPCAdditional |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/G02F1-392
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-2383
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-0057
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-005
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-2308
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/G02F1-3507 |
| classificationCPCInventive |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/G02F1-39
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H01S3-10038
http://rdf.ncbi.nlm.nih.gov/pubchem/patentcpc/H03F7-00 |
| classificationIPCAdditional |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02B27-30
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/H03F7-00
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02B5-18 |
| classificationIPCInventive |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/H01S3-09
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02B27-10
http://rdf.ncbi.nlm.nih.gov/pubchem/patentipc/G02F1-39 |
| filingDate |
2012-08-16-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| inventor |
http://rdf.ncbi.nlm.nih.gov/pubchem/patentinventor/MD5_4ff9baf659d2f426fb74fe6ea0946b8c
http://rdf.ncbi.nlm.nih.gov/pubchem/patentinventor/MD5_b2d22a223568806a2d64ea5e7ecd8b2b
http://rdf.ncbi.nlm.nih.gov/pubchem/patentinventor/MD5_677c045be6975d56e70255a562380271 |
| publicationDate |
2013-02-21-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| publicationNumber |
WO-2013023301-A1 |
| titleOfInvention |
Method and system for high power parametric amplification of ultra-broadband few-cycle laser pulses |
| abstract |
A system and method for high power parametric amplification based on performing amplification in a frequency domain after time domain pulses are optically Fourier transformed, to overcome bandwidth limitations. In a nutshell, a first optical Fourier transformation of a seed spectrum is performed and parametric amplification is carried out in this spatially dispersed frequency plane. As a consequence, individual parts of the spectrum can be amplified using an optical amplification medium comprising a series of optical amplification units, such as different narrowband crystals, placed one next to each other. Each crystal is tuned independently to optimize its corresponding spectral slice. A second optical Fourier transformation recovers the time domain laser pulses. This method enables scalability of amplified bandwidth and pulse energy at the same time. |
| isCitedBy |
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/US-9910339-B2
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/EP-2821848-A1
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/US-9203208-B2
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/WO-2014205573-A1
http://rdf.ncbi.nlm.nih.gov/pubchem/patent/EP-3014352-A4 |
| priorityDate |
2011-08-17-04:00^^<http://www.w3.org/2001/XMLSchema#date> |
| type |
http://data.epo.org/linked-data/def/patent/Publication |