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Emittance evolution of a tightly focused electron bunch with high energy spread

The production of a self injected high energy electron beam from laser-plasma interaction is one of the goals at the LI2FE infrastructure at LNF. The formation and acceleration of a beam produced with the experimental setting available in Frascati has been simulated by C. Benedetti et al. by means o...

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Autor principal: Rossi, A R
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: 2011
Materias:
Acceso en línea:http://cds.cern.ch/record/1345759
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author Rossi, A R
author_facet Rossi, A R
author_sort Rossi, A R
collection CERN
description The production of a self injected high energy electron beam from laser-plasma interaction is one of the goals at the LI2FE infrastructure at LNF. The formation and acceleration of a beam produced with the experimental setting available in Frascati has been simulated by C. Benedetti et al. by means of the code AlaDyn [1]; the results, shown in Figure 1, foresee that the bunch should have a total charge of about 3.5 nC, a transverse size of few microns and a very broad spectrum, ranging from a few MeV up to about 1 GeV, in agreement with other numerical and experimental results produced world wide. In particular, a neatly separated charge portion at high energy is present (Figure 2), whose main parameters are reported in Table 1, which constitutes the most interesting product of the plasma based accelerator.
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spelling cern-13457592019-09-30T06:29:59Z http://cds.cern.ch/record/1345759 eng Rossi, A R Emittance evolution of a tightly focused electron bunch with high energy spread Accelerators and Storage Rings 11: Assessment of Novel Accelerator Concepts The production of a self injected high energy electron beam from laser-plasma interaction is one of the goals at the LI2FE infrastructure at LNF. The formation and acceleration of a beam produced with the experimental setting available in Frascati has been simulated by C. Benedetti et al. by means of the code AlaDyn [1]; the results, shown in Figure 1, foresee that the bunch should have a total charge of about 3.5 nC, a transverse size of few microns and a very broad spectrum, ranging from a few MeV up to about 1 GeV, in agreement with other numerical and experimental results produced world wide. In particular, a neatly separated charge portion at high energy is present (Figure 2), whose main parameters are reported in Table 1, which constitutes the most interesting product of the plasma based accelerator. info:eu-repo/grantAgreement/EC/FP7/227579 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/1345759 2011
spellingShingle Accelerators and Storage Rings
11: Assessment of Novel Accelerator Concepts
Rossi, A R
Emittance evolution of a tightly focused electron bunch with high energy spread
title Emittance evolution of a tightly focused electron bunch with high energy spread
title_full Emittance evolution of a tightly focused electron bunch with high energy spread
title_fullStr Emittance evolution of a tightly focused electron bunch with high energy spread
title_full_unstemmed Emittance evolution of a tightly focused electron bunch with high energy spread
title_short Emittance evolution of a tightly focused electron bunch with high energy spread
title_sort emittance evolution of a tightly focused electron bunch with high energy spread
topic Accelerators and Storage Rings
11: Assessment of Novel Accelerator Concepts
url http://cds.cern.ch/record/1345759
http://cds.cern.ch/record/1345759
work_keys_str_mv AT rossiar emittanceevolutionofatightlyfocusedelectronbunchwithhighenergyspread