000599438 001__ 599438
000599438 005__ 20240122110626.0
000599438 037__ $$aPUBDB-2023-07410
000599438 041__ $$aEnglish
000599438 1001_ $$0P:(DE-H253)PIP1026858$$aHua, Yi$$b0$$udesy
000599438 1112_ $$a2023 Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference$$cMunich$$d2023-06-26 - 2023-06-30$$g(CLEO/Europe-EQEC)$$wGermany
000599438 245__ $$aInfluence of XPM in All-PM Fiber Oscillators Mode-Locked Using NPE in Linear Self-Stabilized Fiber Interferometers
000599438 260__ $$c2023
000599438 3367_ $$0PUB:(DE-HGF)1$$2PUB:(DE-HGF)$$aAbstract$$babstract$$mabstract$$s1705328039_3778158
000599438 3367_ $$033$$2EndNote$$aConference Paper
000599438 3367_ $$2BibTeX$$aINPROCEEDINGS
000599438 3367_ $$2DRIVER$$aconferenceObject
000599438 3367_ $$2DataCite$$aOutput Types/Conference Abstract
000599438 3367_ $$2ORCID$$aOTHER
000599438 520__ $$aMode-locked fiber oscillators enable many applications such as frequency metrology and timing distribution. In recent years, all-PM fiber oscillators based on nonlinear amplifying loop mirror (NALM) attracted large attention due to their environmental stability combined with excellent noise performance. As less known alternative to NALM lasers, all-PM cavity configurations can be realized with a linear self-stabilized fiber interferometer (LFI) [1] which enable e.g., the implementation of pulse dividers for efficient energy scaling [2]. In this work, we numerically investigate the influence of cross-phase modulation (XPM) between the co-propagating orthogonal polarization modes on the stability of LFI mode-locked fiber lasers. A compact numerical model based on coupled nonlinear Schrödinger equations and rate equations is applied to compare the mode-locked steady-states with and without XPM.
000599438 536__ $$0G:(DE-HGF)POF4-621$$a621 - Accelerator Research and Development (POF4-621)$$cPOF4-621$$fPOF IV$$x0
000599438 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000599438 7001_ $$0P:(DE-H253)PIP1088033$$aEdelmann, Marvin$$b1$$udesy
000599438 7001_ $$0P:(DE-H253)PIP1013198$$aKärtner, Franz$$b2$$udesy
000599438 7001_ $$0P:(DE-H253)PIP1018794$$aHartl, Ingmar$$b3$$udesy
000599438 909CO $$ooai:bib-pubdb1.desy.de:599438$$pVDB
000599438 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1026858$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000599438 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1026858$$aCentre for Free-Electron Laser Science$$b0$$kCFEL
000599438 9101_ $$0I:(DE-588)1043621512$$6P:(DE-H253)PIP1026858$$aEuropean XFEL$$b0$$kXFEL.EU
000599438 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1026858$$aExternal Institute$$b0$$kExtern
000599438 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1088033$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000599438 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1088033$$aCentre for Free-Electron Laser Science$$b1$$kCFEL
000599438 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1013198$$aDeutsches Elektronen-Synchrotron$$b2$$kDESY
000599438 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1013198$$aCentre for Free-Electron Laser Science$$b2$$kCFEL
000599438 9101_ $$0I:(DE-588)1043621512$$6P:(DE-H253)PIP1013198$$aEuropean XFEL$$b2$$kXFEL.EU
000599438 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1018794$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000599438 9131_ $$0G:(DE-HGF)POF4-621$$1G:(DE-HGF)POF4-620$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator Research and Development$$x0
000599438 9141_ $$y2023
000599438 9201_ $$0I:(DE-H253)FS-CFEL-2-20120731$$kFS-CFEL-2$$lUltrafast Lasers & X-rays Division$$x0
000599438 9201_ $$0I:(DE-H253)XFEL_DO_ID_LAS-20210408$$kXFEL_DO_ID_LAS$$lOptical Lasers$$x1
000599438 9201_ $$0I:(DE-H253)FS-LA-20130416$$kFS-LA$$lLaser Forschung und Entwicklung$$x2
000599438 980__ $$aabstract
000599438 980__ $$aVDB
000599438 980__ $$aI:(DE-H253)FS-CFEL-2-20120731
000599438 980__ $$aI:(DE-H253)XFEL_DO_ID_LAS-20210408
000599438 980__ $$aI:(DE-H253)FS-LA-20130416
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