Ultra-low timing-jitter passively mode-locked fiber lasers for long-distance timing synchronization

dc.citation.volumeNumber6389en_US
dc.contributor.authorİlday, F. Ömeren_US
dc.contributor.authorWinter, A.en_US
dc.contributor.authorKim J.-W.en_US
dc.contributor.authorChen, J.en_US
dc.contributor.authorSchmüser, P.en_US
dc.contributor.authorSchlarb, H.en_US
dc.contributor.authorKärtner, F. X.en_US
dc.coverage.spatialBoston, Massachusetts, United Statesen_US
dc.date.accessioned2016-02-08T11:47:50Z
dc.date.available2016-02-08T11:47:50Z
dc.date.issued2006en_US
dc.departmentDepartment of Electrical and Electronics Engineeringen_US
dc.departmentDepartment of Physicsen_US
dc.departmentInstitute of Materials Science and Nanotechnology (UNAM)en_US
dc.descriptionDate of Conference: 1-4 October 2006en_US
dc.descriptionConference name: Proceedings of SPIE, Active and Passive Optical Components for Communications VIen_US
dc.description.abstractOne of the key challenges for the next-generation light sources such as X-FELs is to implement a timing stabilization and distribution system to enable ∼ 10 fs synchronization of the different RF and laser sources distributed in such facilities with distances up to a few kilometers. These requirements appear to be beyond the capability of traditional RF distribution systems based on temperature-stabilized coaxial cables. A promising alternative is to use an optical transmission system: A train of pulses generated from a laser with low timing jitter is distributed over length-stabilized fiber links to remote locations. The repetition frequency of the pulse train and its higher harmonics contain the synchronization information. At the remote locations, RF signals are extracted simply by using a photodiode and a suitable bandpass filter to pick the desired harmonic of the laser repetition rate. Passively mode-locked Er-doped fiber lasers provide excellent long-term stability. The laser must have extremely low timing jitter, particularly at high frequencies (>1 kHz). Ultimately, the timing jitter is limited by quantum fluctuations in the number of photons making up the pulse and the incoherent photons added in the cavity due to spontaneous emission. The amplitude and phase noise of a home-built laser, generating 100-fs, 1-nJ pulses, was characterized. The measured phase noise (timing jitter) is sub-10 fs. from 1 kHz to Nyquist frequency. In addition to synchronization of accelerators, the ultra-low timing jitter pulse source can find applications in next-generation telecommunication systems.en_US
dc.identifier.doi10.1117/12.687364en_US
dc.identifier.issn0277-786Xen_US
dc.identifier.urihttp://hdl.handle.net/11693/27220
dc.language.isoEnglishen_US
dc.publisherSPIEen_US
dc.relation.isversionofhttps://doi.org/10.1117/12.687364en_US
dc.source.titleProceedings of SPIEen_US
dc.subjectFiberen_US
dc.subjectLaseren_US
dc.subjectPhase-noiseen_US
dc.subjectPhotonicsen_US
dc.subjectRFen_US
dc.subjectTiming jitteren_US
dc.subjectUltrafast opticsen_US
dc.subjectHarmonic analysisen_US
dc.subjectLaser mode lockingen_US
dc.subjectLight sourcesen_US
dc.subjectOptical cablesen_US
dc.subjectSynchronizationen_US
dc.subjectTiming jitteren_US
dc.subjectPhase-noiseen_US
dc.subjectPhotonicsen_US
dc.subjectUltrafast opticsen_US
dc.subjectFiber lasersen_US
dc.titleUltra-low timing-jitter passively mode-locked fiber lasers for long-distance timing synchronizationen_US
dc.typeConference Paperen_US

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