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Proton Beam Defocusing as a Result of Self-Modulation in Plasma

The AWAKE experiment will use a \SI{400}{GeV/c} proton beam with a longitudinal bunch length of $\sigma_z = 12\,\rm{cm}$ to create and sustain GV/m plasma wakefields over 10 meters . A 12 cm long bunch can only drive strong wakefields in a plasma with $n_{pe} = 7 \times 10^{14}\,\rm{electrons/cm}^3$...

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Autores principales: Turner, Marlene, Petrenko, Alexey, Gschwendtner, Edda, Lotov, Konstantin, Sosedkin, Alexander
Lenguaje:eng
Publicado: 2016
Materias:
Acceso en línea:https://dx.doi.org/10.18429/JACoW-NAPAC2016-WEPOA09
http://cds.cern.ch/record/2226328
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author Turner, Marlene
Petrenko, Alexey
Gschwendtner, Edda
Lotov, Konstantin
Sosedkin, Alexander
author_facet Turner, Marlene
Petrenko, Alexey
Gschwendtner, Edda
Lotov, Konstantin
Sosedkin, Alexander
author_sort Turner, Marlene
collection CERN
description The AWAKE experiment will use a \SI{400}{GeV/c} proton beam with a longitudinal bunch length of $\sigma_z = 12\,\rm{cm}$ to create and sustain GV/m plasma wakefields over 10 meters . A 12 cm long bunch can only drive strong wakefields in a plasma with $n_{pe} = 7 \times 10^{14}\,\rm{electrons/cm}^3$ after the self-modulation instability (SMI) developed and microbunches formed, spaced at the plasma wavelength. The fields present during SMI focus and defocus the protons in the transverse plane \cite{SMI}. We show that by inserting two imaging screens downstream the plasma, we can measure the maximum defocusing angle of the defocused protons for plasma densities above $n_{pe} = 5 \times 10^{14}\,\rm{electrons/cm}^{-3}$. Measuring maximum defocusing angles around 1 mrad indirectly proves that SMI developed successfully and that GV/m plasma wakefields were created. In this paper we present numerical studies on how and when the wakefields defocus protons in plasma, the expected measurement results of the two screen diagnostics and the physics we can deduce from it.
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spelling cern-22263282021-05-03T20:28:08Zdoi:10.18429/JACoW-NAPAC2016-WEPOA09http://cds.cern.ch/record/2226328engTurner, MarlenePetrenko, AlexeyGschwendtner, EddaLotov, KonstantinSosedkin, AlexanderProton Beam Defocusing as a Result of Self-Modulation in Plasmaphysics.acc-phAccelerators and Storage RingsThe AWAKE experiment will use a \SI{400}{GeV/c} proton beam with a longitudinal bunch length of $\sigma_z = 12\,\rm{cm}$ to create and sustain GV/m plasma wakefields over 10 meters . A 12 cm long bunch can only drive strong wakefields in a plasma with $n_{pe} = 7 \times 10^{14}\,\rm{electrons/cm}^3$ after the self-modulation instability (SMI) developed and microbunches formed, spaced at the plasma wavelength. The fields present during SMI focus and defocus the protons in the transverse plane \cite{SMI}. We show that by inserting two imaging screens downstream the plasma, we can measure the maximum defocusing angle of the defocused protons for plasma densities above $n_{pe} = 5 \times 10^{14}\,\rm{electrons/cm}^{-3}$. Measuring maximum defocusing angles around 1 mrad indirectly proves that SMI developed successfully and that GV/m plasma wakefields were created. In this paper we present numerical studies on how and when the wakefields defocus protons in plasma, the expected measurement results of the two screen diagnostics and the physics we can deduce from it.The AWAKE experiment will use a 400 GeV/c proton beam with a longitudinal bunch length of sigmq_{z} = 12 cm to create and sustain GV/m plasma wakefields over 10 meters. A 12 cm long bunch can only drive strong wakefields in a plasma with n_{p}e = 7 x 10¹⁴ electrons/cm³ after the self-modulation instability (SMI) developed and microbunches formed, spaced at the plasma wavelength. The fields present during SMI focus and defocus the protons in the transverse plane. We show that by inserting two imaging screens downstream the plasma, we can measure the maximum defocusing angle of the defocused protons for plasma densities above n_{p}e = 5 x10¹⁴ electrons/cm³. Measuring maximum defocusing angles around 1 mrad indirectly proves that SMI developed successfully and that GV/m plasma wakefields were created. In this paper we present numerical studies on how and when the wakefields defocus protons in plasma, the expected measurement results of the two screen diagnostics and the physics we can deduce from it.arXiv:1610.05527NAPAC-2016-WEPOA09oai:cds.cern.ch:22263282016-10-18
spellingShingle physics.acc-ph
Accelerators and Storage Rings
Turner, Marlene
Petrenko, Alexey
Gschwendtner, Edda
Lotov, Konstantin
Sosedkin, Alexander
Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title_full Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title_fullStr Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title_full_unstemmed Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title_short Proton Beam Defocusing as a Result of Self-Modulation in Plasma
title_sort proton beam defocusing as a result of self-modulation in plasma
topic physics.acc-ph
Accelerators and Storage Rings
url https://dx.doi.org/10.18429/JACoW-NAPAC2016-WEPOA09
http://cds.cern.ch/record/2226328
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AT gschwendtneredda protonbeamdefocusingasaresultofselfmodulationinplasma
AT lotovkonstantin protonbeamdefocusingasaresultofselfmodulationinplasma
AT sosedkinalexander protonbeamdefocusingasaresultofselfmodulationinplasma