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000437316 0247_ $$2doi$$a10.1103/PhysRevAccelBeams.23.031301
000437316 0247_ $$2INSPIRETeX$$aNghiem:2020ggc
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000437316 0247_ $$2ISSN$$a1098-4402
000437316 0247_ $$2ISSN$$a2469-9888
000437316 0247_ $$2datacite_doi$$a10.3204/PUBDB-2020-01432
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000437316 037__ $$aPUBDB-2020-01432
000437316 041__ $$aEnglish
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000437316 1001_ $$0P:(DE-HGF)0$$aNghiem, P. A. P.$$b0$$eCorresponding author
000437316 245__ $$aToward a Plasma-based Accelerator at High Beam Energy with High Beam Charge and High Beam Quality
000437316 260__ $$aCollege Park, MD$$bAmerican Physical Society$$c2020
000437316 264_1 $$2Crossref$$3online$$bAmerican Physical Society (APS)$$c2020-03-03
000437316 264_1 $$2Crossref$$3print$$bAmerican Physical Society (APS)$$c2020-03-01
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000437316 520__ $$aFrom plasma-wakefield acceleration as a physics experiment toward a plasma-based accelerator as a user facility, the beam physics issues remaining to be solved are still numerous. Providing beams with high energy, charge, and quality simultaneously, not only within the plasma but also at the user doorstep itself, is the main concern. Despite its tremendous efficiency in particle acceleration, the wakefield displays a complex 3D profile which, associated to the beam-loading field induced by the accelerated beam itself, makes the acceleration of high charge to high energy often incompatible with high beam quality. Beam extraction from the plasma without quality degradation for a transfer either to the next plasma stage or to the user application is another difficulty to consider. This article presents the substantial studies carried out and the different innovative methods employed for tackling all these different issues. Efforts focused on achieving the challenging beam parameters targeted by the EuPRAXIA accelerator facility project. The lessons learned at the end of these in-depth simulations and optimizations are highlighted. The sensitivity to different error sources is also estimated to point out the critical components of such an accelerator. Finally, the needs in terms of laser and plasma parameters are provided.
000437316 536__ $$0G:(DE-HGF)POF3-631$$a631 - Accelerator R & D (POF3-631)$$cPOF3-631$$fPOF III$$x0
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000437316 650_7 $$2INSPIRE$$acharge: high
000437316 650_7 $$2INSPIRE$$aaccelerator: wake field
000437316 650_7 $$2INSPIRE$$aparticle: acceleration
000437316 650_7 $$2INSPIRE$$aquality
000437316 650_7 $$2INSPIRE$$abeam loading
000437316 650_7 $$2INSPIRE$$asensitivity
000437316 650_7 $$2INSPIRE$$aplasma: wake field
000437316 650_7 $$2INSPIRE$$anumerical calculations
000437316 650_7 $$2INSPIRE$$abeam: injection
000437316 650_7 $$2INSPIRE$$abeam profile
000437316 650_7 $$2INSPIRE$$abeam transport
000437316 650_7 $$2INSPIRE$$alaser
000437316 650_7 $$2INSPIRE$$abibliography
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000437316 7001_ $$0P:(DE-H253)PIP1027268$$aLee, P.$$b11
000437316 7001_ $$0P:(DE-H253)PIP1081485$$aLi, Xiangkun$$b12
000437316 7001_ $$0P:(DE-H253)PIP1030943$$aMarocchino, A.$$b13
000437316 7001_ $$0P:(DE-H253)PIP1006726$$aMartinez de la Ossa, A.$$b14
000437316 7001_ $$0P:(DE-H253)PIP1030947$$aMassimo, F.$$b15
000437316 7001_ $$0P:(DE-H253)PIP1031807$$aMaynard, G.$$b16
000437316 7001_ $$0P:(DE-H253)PIP1093374$$aMosnier, A.$$b17
000437316 7001_ $$0P:(DE-H253)PIP1081500$$aRomeo, S.$$b18
000437316 7001_ $$0P:(DE-HGF)0$$aRossi, A. R.$$b19
000437316 7001_ $$0P:(DE-H253)PIP1085115$$aSilva, T.$$b20
000437316 7001_ $$0P:(DE-H253)PIP1028567$$aSvystun, E.$$b21
000437316 7001_ $$0P:(DE-H253)PIP1081502$$aTomassini, P.$$b22
000437316 7001_ $$0P:(DE-HGF)0$$aVaccarezza, C.$$b23
000437316 7001_ $$0P:(DE-H253)PIP1031809$$aVieira, J.$$b24
000437316 7001_ $$0P:(DE-H253)PIP1023492$$aZhu, Jun$$b25
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