High-energy femtosecond photonic crystal fiber laser
dc.citation.epage | 3158 | en_US |
dc.citation.issueNumber | 19 | en_US |
dc.citation.spage | 3156 | en_US |
dc.citation.volumeNumber | 35 | en_US |
dc.contributor.author | Lecaplain, C. | en_US |
dc.contributor.author | Ortaç, B. | en_US |
dc.contributor.author | MacHinet G. | en_US |
dc.contributor.author | Boullet J. | en_US |
dc.contributor.author | Baumgart, M. | en_US |
dc.contributor.author | Schreiber, T. | en_US |
dc.contributor.author | Cormier, E. | en_US |
dc.contributor.author | Hideur, A. | en_US |
dc.date.accessioned | 2016-02-08T09:56:38Z | |
dc.date.available | 2016-02-08T09:56:38Z | |
dc.date.issued | 2010 | en_US |
dc.department | Institute of Materials Science and Nanotechnology (UNAM) | en_US |
dc.description.abstract | We report the generation of high-energy high-peak power pulses in an all-normal dispersion fiber laser featuring large-mode-area photonic crystal fibers. The self-starting chirped-pulse fiber oscillator delivers 11 W of average power at 15:5 MHz repetition rate, resulting in 710 nJ of pulse energy. The output pulses are dechirped outside the cavity from 7 ps to nearly transform-limited duration of 300 fs, leading to pulse peak powers as high as 1:9 MW. Numerical simulations reveal that pulse shaping is dominated by the amplitude modulation and spectral filtering provided by a resonant semiconductor saturable absorber. © 2010 Optical Society of America. | en_US |
dc.description.provenance | Made available in DSpace on 2016-02-08T09:56:38Z (GMT). No. of bitstreams: 1 bilkent-research-paper.pdf: 70227 bytes, checksum: 26e812c6f5156f83f0e77b261a471b5a (MD5) Previous issue date: 2010 | en |
dc.identifier.doi | 10.1364/OL.35.003156 | en_US |
dc.identifier.issn | 1469592 | |
dc.identifier.uri | http://hdl.handle.net/11693/22184 | |
dc.language.iso | English | en_US |
dc.relation.isversionof | http://dx.doi.org/10.1364/OL.35.003156 | en_US |
dc.source.title | Optics Letters | en_US |
dc.subject | Average power | en_US |
dc.subject | Chirped-pulse | en_US |
dc.subject | Femtoseconds | en_US |
dc.subject | Fiber oscillators | en_US |
dc.subject | High energy | en_US |
dc.subject | High peak power | en_US |
dc.subject | Large-mode-area photonic crystal fibers | en_US |
dc.subject | Normal dispersion | en_US |
dc.subject | Numerical simulation | en_US |
dc.subject | Output pulse | en_US |
dc.subject | Peak power | en_US |
dc.subject | Pulse energies | en_US |
dc.subject | Pulse-shaping | en_US |
dc.subject | Repetition rate | en_US |
dc.subject | Self-starting | en_US |
dc.subject | Semiconductor saturable absorbers | en_US |
dc.subject | Spectral filtering | en_US |
dc.subject | Crystal whiskers | en_US |
dc.subject | Fiber lasers | en_US |
dc.subject | Fibers | en_US |
dc.subject | High energy physics | en_US |
dc.subject | Photonic crystals | en_US |
dc.subject | Pulse repetition rate | en_US |
dc.subject | Semiconductor lasers | en_US |
dc.subject | Single mode fibers | en_US |
dc.subject | Photonic crystal fibers | en_US |
dc.title | High-energy femtosecond photonic crystal fiber laser | en_US |
dc.type | Article | en_US |
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