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A publicação pode ser exportada nos seguintes formatos: referência da APA (American Psychological Association), referência do IEEE (Institute of Electrical and Electronics Engineers), BibTeX e RIS.

Exportar Referência (APA)
Lotov, K., Sosedkin, A., Petrenko, A., Amorim, L. D., Vieira, J., Fonseca, R. A....Muggli, P. (2014). Electron trapping and acceleration by the plasma wakefield of a self-modulating proton beam. Physics of Plasmas. 21 (12)
Exportar Referência (IEEE)
K. V. Lotov et al.,  "Electron trapping and acceleration by the plasma wakefield of a self-modulating proton beam", in Physics of Plasmas, vol. 21, no. 12, 2014
Exportar BibTeX
@article{lotov2014_1731662424730,
	author = "Lotov, K. and Sosedkin, A. and Petrenko, A. and Amorim, L. D. and Vieira, J. and Fonseca, R. A. and Silva, L. O. and Gschwendtner, E. and Muggli, P.",
	title = "Electron trapping and acceleration by the plasma wakefield of a self-modulating proton beam",
	journal = "Physics of Plasmas",
	year = "2014",
	volume = "21",
	number = "12",
	doi = "10.1063/1.4904365",
	url = "http://scitation.aip.org/content/aip/journal/pop/21/12/10.1063/1.4904365"
}
Exportar RIS
TY  - JOUR
TI  - Electron trapping and acceleration by the plasma wakefield of a self-modulating proton beam
T2  - Physics of Plasmas
VL  - 21
IS  - 12
AU  - Lotov, K.
AU  - Sosedkin, A.
AU  - Petrenko, A.
AU  - Amorim, L. D.
AU  - Vieira, J.
AU  - Fonseca, R. A.
AU  - Silva, L. O.
AU  - Gschwendtner, E.
AU  - Muggli, P.
PY  - 2014
SN  - 1070-664X
DO  - 10.1063/1.4904365
UR  - http://scitation.aip.org/content/aip/journal/pop/21/12/10.1063/1.4904365
AB  - It is shown that co-linear injection of electrons or positrons into the wakefield of the self-modulating particle beam is possible and ensures high energy gain. The witness beam must co-propagate with the tail part of the driver, since the plasma wave phase velocity there can exceed the light velocity, which is necessary for efficient acceleration. If the witness beam is many wakefield periods long, then the trapped charge is limited by beam loading effects. The initial trapping is better for positrons, but at the acceleration stage a considerable fraction of positrons is lost from the wave. For efficient trapping of electrons, the plasma boundary must be sharp, with the density transition region shorter than several centimeters. Positrons are not susceptible to the initial plasma density gradient.
ER  -