001     416738
005     20250729165247.0
020 _ _ |a 978-3-95450-184-7
024 7 _ |a 10.18429/JACoW-IPAC2018-TUPML047
|2 doi
024 7 _ |a 10.3204/PUBDB-2018-05122
|2 datacite_doi
024 7 _ |a inspire:1690516
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024 7 _ |a openalex:W2891645642
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037 _ _ |a PUBDB-2018-05122
041 _ _ |a English
100 1 _ |a Loisch, Gregor
|0 P:(DE-H253)PIP1026627
|b 0
|e Corresponding author
|u desy
111 2 _ |a 9th International Particle Accelerator Conference
|g IPAC'18
|c Vancouver
|d 2018-04-29 - 2018-05-04
|w Canada
245 _ _ |a Optimisation of High Transformer Ratio Plasma Wakefield Acceleration at PITZ
260 _ _ |a Geneva, Switzerland
|c 2018
|b JACoW Publishing
300 _ _ |a 1648-1650
336 7 _ |a CONFERENCE_PAPER
|2 ORCID
336 7 _ |a Conference Paper
|0 33
|2 EndNote
336 7 _ |a INPROCEEDINGS
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336 7 _ |a conferenceObject
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336 7 _ |a Output Types/Conference Paper
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336 7 _ |a Contribution to a conference proceedings
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336 7 _ |a Contribution to a book
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520 _ _ |a The transformer ratio, the ratio between maximum accelerating field and maximum decelerating field in the driving bunch of a plasma wakefield accelerator (PWFA), is one of the key aspects of this acceleration scheme. It not only defines the maximum possible energy gain of the PWFA but it is also connected to the maximum percentage of energy that can be extracted from the driver, which is a limiting factor for the efficiency of the accelerator. Since in linear wakefield theory a transformer ratio of 2 cannot be exceeded with symmetrical drive bunches, any ratio above 2 is considered high. After the first demonstration of high transformer ratio acceleration in a plasma wakefield at PITZ, the photoinjector test facility at DESY, Zeuthen site, limiting aspects of the transformer ratio are under investigation. This includes e.g. the occurrence of bunch instabilities, like the transverse two stream instability, or deviations of the experimentally achieved bunch shapes from the ideal.
536 _ _ |a 631 - Accelerator R & D (POF3-631)
|0 G:(DE-HGF)POF3-631
|c POF3-631
|f POF III
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588 _ _ |a Dataset connected to DataCite
693 _ _ |0 EXP:(DE-H253)PITZ-20150101
|5 EXP:(DE-H253)PITZ-20150101
|e Photo Injector Test Facility
|x 0
700 1 _ |a Boonpornprasert, Prach
|0 P:(DE-H253)PIP1019294
|b 1
|u desy
700 1 _ |a Brinkmann, Reinhard
|0 P:(DE-H253)PIP1002844
|b 2
|u desy
700 1 _ |a Good, James David
|0 P:(DE-H253)PIP1014737
|b 3
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700 1 _ |a Groß, Matthias
|0 P:(DE-H253)PIP1013620
|b 4
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700 1 _ |a Grüner, Florian
|0 P:(DE-H253)PIP1013695
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700 1 _ |a Huck, Holger
|0 P:(DE-H253)PIP1023201
|b 6
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700 1 _ |a Krasilnikov, Mikhail
|0 P:(DE-H253)PIP1004128
|b 7
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700 1 _ |a Lishilin, Osip
|0 P:(DE-H253)PIP1023202
|b 8
|u desy
700 1 _ |a Martinez de la Ossa, Alberto
|0 P:(DE-H253)PIP1006726
|b 9
|u desy
700 1 _ |a Oppelt, Anne
|0 P:(DE-H253)PIP1011785
|b 10
|u desy
700 1 _ |a Osterhoff, Jens
|0 P:(DE-H253)PIP1012785
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700 1 _ |a Renier, Yves
|0 P:(DE-H253)PIP1023200
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|u desy
700 1 _ |a Stephan, Frank
|0 P:(DE-H253)PIP1004143
|b 13
|u desy
773 _ _ |a 10.18429/JACoW-IPAC2018-TUPML047
856 4 _ |y OpenAccess
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910 1 _ |a Deutsches Elektronen-Synchrotron
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910 1 _ |a Deutsches Elektronen-Synchrotron
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910 1 _ |a Deutsches Elektronen-Synchrotron
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910 1 _ |a Centre for Free-Electron Laser Science
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910 1 _ |a Deutsches Elektronen-Synchrotron
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910 1 _ |a Deutsches Elektronen-Synchrotron
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913 1 _ |a DE-HGF
|b Forschungsbereich Materie
|l Materie und Technologie
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914 1 _ |y 2018
915 _ _ |a Creative Commons Attribution CC BY 3.0
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920 1 _ |0 I:(DE-H253)FLA-20120731
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980 _ _ |a I:(DE-H253)ZEU-PITZ-20120731
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980 _ _ |a I:(DE-H253)CFEL-NOVA-20160909
980 _ _ |a I:(DE-H253)FLA-20120731
981 _ _ |a I:(DE-H253)Z_PITZ-20210408


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