Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV

We report on the first results of experiments with a new laser-based proton beam line at the GSI accelerator facility in Darmstadt. It delivers high current bunches at proton energies around 9.6 MeV, containing more than 10^{9} particles in less than 10 ns and with tunable energy spread down to 2.7%...

Full description

Bibliographic Details
Main Authors: S. Busold, D. Schumacher, O. Deppert, C. Brabetz, F. Kroll, A. Blažević, V. Bagnoud, M. Roth
Format: Article
Language:English
Published: American Physical Society 2014-03-01
Series:Physical Review Special Topics. Accelerators and Beams
Online Access:http://doi.org/10.1103/PhysRevSTAB.17.031302
id doaj-1dc3c2b150f5428899dd2f29696a6793
record_format Article
spelling doaj-1dc3c2b150f5428899dd2f29696a67932020-11-25T00:03:59ZengAmerican Physical SocietyPhysical Review Special Topics. Accelerators and Beams1098-44022014-03-0117303130210.1103/PhysRevSTAB.17.031302Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeVS. BusoldD. SchumacherO. DeppertC. BrabetzF. KrollA. BlaževićV. BagnoudM. RothWe report on the first results of experiments with a new laser-based proton beam line at the GSI accelerator facility in Darmstadt. It delivers high current bunches at proton energies around 9.6 MeV, containing more than 10^{9} particles in less than 10 ns and with tunable energy spread down to 2.7% (ΔE/E_{0} at FWHM). A target normal sheath acceleration stage serves as a proton source and a pulsed solenoid provides for beam collimation and energy selection. Finally a synchronous radio frequency (rf) field is applied via a rf cavity for energy compression at a synchronous phase of -90  deg. The proton bunch is characterized at the end of the very compact beam line, only 3 m behind the laser matter interaction point, which defines the particle source.http://doi.org/10.1103/PhysRevSTAB.17.031302
collection DOAJ
language English
format Article
sources DOAJ
author S. Busold
D. Schumacher
O. Deppert
C. Brabetz
F. Kroll
A. Blažević
V. Bagnoud
M. Roth
spellingShingle S. Busold
D. Schumacher
O. Deppert
C. Brabetz
F. Kroll
A. Blažević
V. Bagnoud
M. Roth
Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
Physical Review Special Topics. Accelerators and Beams
author_facet S. Busold
D. Schumacher
O. Deppert
C. Brabetz
F. Kroll
A. Blažević
V. Bagnoud
M. Roth
author_sort S. Busold
title Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
title_short Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
title_full Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
title_fullStr Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
title_full_unstemmed Commissioning of a compact laser-based proton beam line for high intensity bunches around 10 MeV
title_sort commissioning of a compact laser-based proton beam line for high intensity bunches around 10 mev
publisher American Physical Society
series Physical Review Special Topics. Accelerators and Beams
issn 1098-4402
publishDate 2014-03-01
description We report on the first results of experiments with a new laser-based proton beam line at the GSI accelerator facility in Darmstadt. It delivers high current bunches at proton energies around 9.6 MeV, containing more than 10^{9} particles in less than 10 ns and with tunable energy spread down to 2.7% (ΔE/E_{0} at FWHM). A target normal sheath acceleration stage serves as a proton source and a pulsed solenoid provides for beam collimation and energy selection. Finally a synchronous radio frequency (rf) field is applied via a rf cavity for energy compression at a synchronous phase of -90  deg. The proton bunch is characterized at the end of the very compact beam line, only 3 m behind the laser matter interaction point, which defines the particle source.
url http://doi.org/10.1103/PhysRevSTAB.17.031302
work_keys_str_mv AT sbusold commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT dschumacher commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT odeppert commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT cbrabetz commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT fkroll commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT ablazevic commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT vbagnoud commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
AT mroth commissioningofacompactlaserbasedprotonbeamlineforhighintensitybunchesaround10mev
_version_ 1725431570138923008