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000576801 037__ $$aPUBDB-2023-00913
000576801 041__ $$aEnglish
000576801 1001_ $$0P:(DE-H253)PIP1023917$$aGeorgiev, Georgi$$b0
000576801 1112_ $$a40th International Free Electron Laser Conference$$cTrieste$$d2022-08-22 - 2022-08-26$$gFEL2022$$wItaly
000576801 245__ $$aSimulations of Seeding Options for THz FEL at PITZ
000576801 260__ $$c2022
000576801 3367_ $$033$$2EndNote$$aConference Paper
000576801 3367_ $$2DataCite$$aOther
000576801 3367_ $$2BibTeX$$aINPROCEEDINGS
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000576801 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1677489821_25804
000576801 500__ $$aApproved by PITZ CB JACoW Proceedings
000576801 520__ $$aA THz FEL is under commissioning at PITZ as a proof-of-principle experiment for a high power and high repetitionrate THz source and as an option for THz-driven experi-ments at the European XFEL. Some of these experimentsrequire excellent coherence and CEP stable THz pulses. InSASE regime, the coherent properties of the FEL radiationare limited. A seeding scheme can be used instead of SASEto improve the coherent properties and shot-to-shot stability.Several options for seeding are considered in simulation forthe THz FEL at PITZ: external laser pulse, pre-bunched elec-tron beam, energy modulated electron beam and additionalshort spike on top of a smooth beam profile. The improve-ments over SASE in energy, spectral and temporal stabilityof the THz pulse are presented.
000576801 536__ $$0G:(DE-HGF)POF4-621$$a621 - Accelerator Research and Development (POF4-621)$$cPOF4-621$$fPOF IV$$x0
000576801 693__ $$0EXP:(DE-H253)PITZ-20150101$$5EXP:(DE-H253)PITZ-20150101$$ePhoto Injector Test Facility$$x0
000576801 7001_ $$0P:(DE-H253)PIP1019294$$aBoonpornprasert, Prach$$b1
000576801 7001_ $$0P:(DE-H253)PIP1004128$$aKrasilnikov, Mikhail$$b2
000576801 7001_ $$0P:(DE-H253)PIP1081485$$aLi, Xiangkun$$b3
000576801 7001_ $$0P:(DE-H253)PIP1032393$$aHillert, Wolfgang$$b4
000576801 7870_ $$0PUBDB-2022-04414$$aGeorgiev, Georgi et.al.$$d2022$$iIsMemberOf$$tSimulations of Seeding Options for THz FEL at PITZ
000576801 909CO $$ooai:bib-pubdb1.desy.de:576801$$pVDB
000576801 9141_ $$y2022
000576801 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1023917$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
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000576801 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1019294$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
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000576801 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1081485$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000576801 9101_ $$0I:(DE-H253)_CFEL-20120731$$6P:(DE-H253)PIP1032393$$aCentre for Free-Electron Laser Science$$b4$$kCFEL
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000576801 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
000576801 9201_ $$0I:(DE-H253)Z_PITZ-20210408$$kZ_PITZ$$lTechnologie$$x0
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