IPAC2014 - List of Authors (Lotov, K.V.)

Paper	Title	Page
TUPME078	Electron Injection Studies for the AWAKE Experiment at CERN	1537
	A.V. Petrenko, C. Bracco, E. Gschwendtner CERN, Geneva, Switzerland K.V. Lotov NSU, Novosibirsk, Russia K.V. Lotov BINP SB RAS, Novosibirsk, Russia P. Muggli MPI, Muenchen, Germany
	The AWAKE experiment recently approved at CERN will use the self-modulation instability (SMI) of long (12 cm), relativistic (400 GeV/c) proton bunches in dense plasmas to drive wakefields with accelerating gradients at the GV/m level. These accelerating gradients will be probed by externally injected electrons. In order to preserve the plasma uniformity required for the SMI the first experiments will use on-axis injection of a low energy 10-20 MeV electron beam collinearly with the proton beam. In this article we describe the physics of electron injection into the proton driven SMI wakefields. Requirements on the injected electron beam are determined and the final accelerated beam parameters are obtained via numerical simulations.
DOI •	reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-TUPME078
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Paper

Title

Page

Electron Injection Studies for the AWAKE Experiment at CERN

1537

A.V. Petrenko, C. Bracco, E. Gschwendtner
CERN, Geneva, Switzerland
K.V. Lotov
NSU, Novosibirsk, Russia
K.V. Lotov
BINP SB RAS, Novosibirsk, Russia
P. Muggli
MPI, Muenchen, Germany

The AWAKE experiment recently approved at CERN will use the self-modulation instability (SMI) of long (12 cm), relativistic (400 GeV/c) proton bunches in dense plasmas to drive wakefields with accelerating gradients at the GV/m level. These accelerating gradients will be probed by externally injected electrons. In order to preserve the plasma uniformity required for the SMI the first experiments will use on-axis injection of a low energy 10-20 MeV electron beam collinearly with the proton beam. In this article we describe the physics of electron injection into the proton driven SMI wakefields. Requirements on the injected electron beam are determined and the final accelerated beam parameters are obtained via numerical simulations.

DOI •

reference for this paper ※ https://doi.org/10.18429/JACoW-IPAC2014-TUPME078

Export •

reference for this paper using ※ BibTeX, ※ LaTeX, ※ Text/Word, ※ RIS, ※ EndNote (xml)