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000600339 041__ $$aEnglish
000600339 1001_ $$0P:(DE-H253)PIP1094182$$aBeinortaite, Judita$$b0$$eCorresponding author$$udesy
000600339 1112_ $$aDPG-Frühjahrstagung 2023$$cDresden$$d2023-03-20 - 2023-03-24$$wGermany
000600339 245__ $$aPlasma Density Evolution Background to the Ion-motion Recovery in a Beam-driven Plasma-wakefield Accelerator
000600339 260__ $$c2023
000600339 3367_ $$033$$2EndNote$$aConference Paper
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000600339 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1708611541_3691542
000600339 520__ $$aBeam-driven plasma-wakefield acceleration is a promising avenue for the future design of compact linear accelerators with applications in high-energy physics and photon science. Meeting the luminosity and brilliance demands of current users requires the delivery of thousands of bunches per second: many orders of magnitude beyond the current state-of-the-art of plasma-wakefield accelerators, which typically operate at the Hz-level. As recently explored at FLASHForward, a fundamental limitation for the highest repetition rate is the long-term motion of ions that follows the dissipation of the driven wakefield (R. D'Arcy, et al. Nature 603, 58,62 (2022)). The duration of this ion motion could vary with the mass of the plasma ions, thus significantly decreasing in lighter gas species. To observe this, the understanding of the background processes, such as microsecond-level plasma density evolution of different gases in a capillary, is needed. Here we present the first steps of exploring this plasma evolution.
000600339 536__ $$0G:(DE-HGF)POF4-621$$a621 - Accelerator Research and Development (POF4-621)$$cPOF4-621$$fPOF IV$$x0
000600339 536__ $$0G:(DE-HGF)POF4-6G2$$a6G2 - FLASH (DESY) (POF4-6G2)$$cPOF4-6G2$$fPOF IV$$x1
000600339 693__ $$0EXP:(DE-H253)FLASHForward-20150101$$1EXP:(DE-H253)FLASH-20150101$$5EXP:(DE-H253)FLASHForward-20150101$$aFLASH$$eFLASHForward$$x0
000600339 8564_ $$uhttps://www.dpg-verhandlungen.de/year/2023/conference/smuk/part/akbp/session/15/contribution/5?lang=en
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000600339 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1094182$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000600339 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
000600339 9131_ $$0G:(DE-HGF)POF4-6G2$$1G:(DE-HGF)POF4-6G0$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lGroßgeräte: Materie$$vFLASH (DESY)$$x1
000600339 9141_ $$y2023
000600339 9201_ $$0I:(DE-H253)HH_FH_FTX_AS-20210421$$kHH_FH_FTX_AS$$lFTX Fachgruppe AST$$x0
000600339 9201_ $$0I:(DE-H253)MPA-20200816$$kMPA$$lPlasma Accelerators$$x1
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