000428507 001__ 428507 000428507 005__ 20250716153928.0 000428507 0247_ $$2doi$$a10.3390/app9132626 000428507 0247_ $$2datacite_doi$$a10.3204/PUBDB-2019-04617 000428507 0247_ $$2WOS$$aWOS:000477031900045 000428507 0247_ $$2altmetric$$aaltmetric:126280620 000428507 0247_ $$2openalex$$aopenalex:W2956020309 000428507 037__ $$aPUBDB-2019-04617 000428507 041__ $$aEnglish 000428507 082__ $$a600 000428507 1001_ $$0P:(DE-H253)PIP1017227$$aHidding, Bernhard$$b0$$eCorresponding author 000428507 245__ $$aFundamentals and Applications of Hybrid LWFA-PWFA 000428507 260__ $$aBasel$$bMDPI$$c2019 000428507 3367_ $$2DRIVER$$aarticle 000428507 3367_ $$2DataCite$$aOutput Types/Journal article 000428507 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1575281705_16594 000428507 3367_ $$2BibTeX$$aARTICLE 000428507 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000428507 3367_ $$00$$2EndNote$$aJournal Article 000428507 520__ $$aFundamental similarities and differences between laser-driven plasma wakefield acceleration (LWFA) and particle-driven plasma wakefield acceleration (PWFA) are discussed. The complementary features enable the conception and development of novel hybrid plasma accelerators, which allow previously not accessible compact solutions for high quality electron bunch generation and arising applications. Very high energy gains can be realized by electron beam drivers even in single stages because PWFA is practically dephasing-free and not diffraction-limited. These electron driver beams for PWFA in turn can be produced in compact LWFA stages. In various hybrid approaches, these PWFA systems can be spiked with ionizing laser pulses to realize tunable and high-quality electron sources via optical density downramp injection (also known as plasma torch) or plasma photocathodes (also known as Trojan Horse) and via wakefield-induced injection (also known as WII). These hybrids can act as beam energy, brightness and quality transformers, and partially have built-in stabilizing features. They thus offer compact pathways towards beams with unprecedented emittance and brightness, which may have transformative impact for light sources and photon science applications. Furthermore, they allow the study of PWFA-specific challenges in compact setups in addition to large linac-based facilities, such as fundamental beam–plasma interaction physics, to develop novel diagnostics, and to develop contributions such as ultralow emittance test beams or other building blocks and schemes which support future plasma-based collider concepts. 000428507 536__ $$0G:(DE-HGF)POF3-631$$a631 - Accelerator R & D (POF3-631)$$cPOF3-631$$fPOF III$$x0 000428507 536__ $$0G:(DE-H253)PWA-20150304$$aPWA - Research group for plasma-based accelerators (PWA-20150304)$$cPWA-20150304$$x1 000428507 536__ $$0G:(EU-Grant)653782$$aEuPRAXIA - Proposal for a Horizon 2020 Design Study on the “European Plasma Research Accelerator with eXcellence In Applications“ (EuPRAXIA) (653782)$$c653782$$fH2020-INFRADEV-1-2014-1$$x2 000428507 536__ $$0G:(EU-Grant)715807$$aM-PAC - Miniature beam-driven Plasma ACcelerators (715807)$$c715807$$fERC-2016-STG$$x3 000428507 588__ $$aDataset connected to CrossRef 000428507 693__ $$0EXP:(DE-H253)FLASHForward-20150101$$1EXP:(DE-H253)FLASH-20150101$$5EXP:(DE-H253)FLASHForward-20150101$$aFLASH$$eFLASHForward$$x0 000428507 7001_ $$0P:(DE-H253)PIP1028054$$aBeaton, Andrew$$b1 000428507 7001_ $$0P:(DE-H253)PIP1086724$$aBoulton, Lewis$$b2 000428507 7001_ $$00000-0002-5015-0387$$aCorde, Sebastién$$b3 000428507 7001_ $$0P:(DE-HGF)0$$aDoepp, Andreas$$b4 000428507 7001_ $$0P:(DE-H253)PIP1013853$$aHabib, Fahim Ahmad$$b5 000428507 7001_ $$0P:(DE-H253)PIP1019372$$aHeinemann, Thomas$$b6$$udesy 000428507 7001_ $$0P:(DE-H253)PIP1081480$$aIrman, Arie$$b7 000428507 7001_ $$0P:(DE-H253)PIP1023635$$aKarsch, Stefan$$b8 000428507 7001_ $$0P:(DE-HGF)0$$aKirwan, Gavin$$b9 000428507 7001_ $$0P:(DE-H253)PIP1021516$$aKnetsch, Alexander$$b10$$udesy 000428507 7001_ $$0P:(DE-H253)PIP1022893$$aManahan, Grace Gloria$$b11 000428507 7001_ $$0P:(DE-H253)PIP1006726$$aMartinez de la Ossa, Alberto$$b12$$udesy 000428507 7001_ $$0P:(DE-H253)PIP1087168$$aNutter, Alastair$$b13 000428507 7001_ $$0P:(DE-H253)PIP1022055$$aScherkl, Paul$$b14 000428507 7001_ $$0P:(DE-H253)PIP1089311$$aSchramm, Ulrich$$b15 000428507 7001_ $$0P:(DE-H253)PIP1032206$$aUllmann, Daniel$$b16 000428507 773__ $$0PERI:(DE-600)2704225-X$$a10.3390/app9132626$$gVol. 9, no. 13, p. 2626 -$$n13$$p2626 -$$tApplied Sciences$$v9$$x2076-3417$$y2019 000428507 8564_ $$uhttps://www.mdpi.com/2076-3417/9/13/2626 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.pdf$$yOpenAccess 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.gif?subformat=icon$$xicon$$yOpenAccess 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.jpg?subformat=icon-640$$xicon-640$$yOpenAccess 000428507 8564_ $$uhttps://bib-pubdb1.desy.de/record/428507/files/applsci-09-02626-v2.pdf?subformat=pdfa$$xpdfa$$yOpenAccess 000428507 909CO $$ooai:bib-pubdb1.desy.de:428507$$pdnbdelivery$$pec_fundedresources$$pVDB$$pdriver$$popen_access$$popenaire 000428507 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1017227$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1028054$$aExternal Institute$$b1$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1086724$$aExternal Institute$$b2$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1013853$$aExternal Institute$$b5$$kExtern 000428507 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1019372$$aDeutsches Elektronen-Synchrotron$$b6$$kDESY 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1019372$$aExternal Institute$$b6$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1023635$$aExternal Institute$$b8$$kExtern 000428507 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1021516$$aDeutsches Elektronen-Synchrotron$$b10$$kDESY 000428507 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1006726$$aDeutsches Elektronen-Synchrotron$$b12$$kDESY 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1006726$$aExternal Institute$$b12$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1087168$$aExternal Institute$$b13$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1022055$$aExternal Institute$$b14$$kExtern 000428507 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1089311$$aExternal Institute$$b15$$kExtern 000428507 9131_ $$0G:(DE-HGF)POF3-631$$1G:(DE-HGF)POF3-630$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lMaterie und Technologie$$vAccelerator R & D$$x0 000428507 9141_ $$y2019 000428507 915__ $$0StatID:(DE-HGF)0200$$2StatID$$aDBCoverage$$bSCOPUS 000428507 915__ $$0LIC:(DE-HGF)CCBYNV$$2V:(DE-HGF)$$aCreative Commons Attribution CC BY (No Version)$$bDOAJ 000428507 915__ $$0StatID:(DE-HGF)1160$$2StatID$$aDBCoverage$$bCurrent Contents - 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