New Journal of Physics (Jan 2016)
Buffered high charge spectrally-peaked proton beams in the relativistic-transparency regime
- N P Dover,
- C A J Palmer,
- M J V Streeter,
- H Ahmed,
- B Albertazzi,
- M Borghesi,
- D C Carroll,
- J Fuchs,
- R Heathcote,
- P Hilz,
- K F Kakolee,
- S Kar,
- R Kodama,
- A Kon,
- D A MacLellan,
- P McKenna,
- S R Nagel,
- D Neely,
- M M Notley,
- M Nakatsutsumi,
- R Prasad,
- G Scott,
- M Tampo,
- M Zepf,
- J Schreiber,
- Z Najmudin
Affiliations
- N P Dover
- The John Adams Institute for Accelerator Science , Blackett Laboratory, Imperial College, London SW7 2BZ, UK
- C A J Palmer
- The John Adams Institute for Accelerator Science , Blackett Laboratory, Imperial College, London SW7 2BZ, UK
- M J V Streeter
- The John Adams Institute for Accelerator Science , Blackett Laboratory, Imperial College, London SW7 2BZ, UK
- H Ahmed
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK
- B Albertazzi
- LULI, École Polytechnique , CNRS, CEA, Palaiseau, France
- M Borghesi
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK
- D C Carroll
- SUPA Department of Physics, University of Strathclyde , Glasgow G4 0NG, UK; Central Laser Facility, STFC Rutherford Appleton Laboratory , Oxfordshire OX11 0QX, UK
- J Fuchs
- LULI, École Polytechnique , CNRS, CEA, Palaiseau, France
- R Heathcote
- Central Laser Facility, STFC Rutherford Appleton Laboratory , Oxfordshire OX11 0QX, UK
- P Hilz
- Fakultät für Physik, Ludwig-Maximilians-Universität München , Am Coulombwall 1, D-85748 Garching, Germany; Max-Planck-Institut für Quantenoptik , Hans-Kopfermann-Str. 1, D-85748 Garching, Germany
- K F Kakolee
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK; Jagannath University , Dhaka, Bangladesh
- S Kar
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK
- R Kodama
- Graduate School of Engineering, Osaka University , Osaka D-565-0871, Japan
- A Kon
- Graduate School of Engineering, Osaka University , Osaka D-565-0871, Japan
- D A MacLellan
- SUPA Department of Physics, University of Strathclyde , Glasgow G4 0NG, UK
- P McKenna
- SUPA Department of Physics, University of Strathclyde , Glasgow G4 0NG, UK
- S R Nagel
- The John Adams Institute for Accelerator Science , Blackett Laboratory, Imperial College, London SW7 2BZ, UK
- D Neely
- SUPA Department of Physics, University of Strathclyde , Glasgow G4 0NG, UK; Central Laser Facility, STFC Rutherford Appleton Laboratory , Oxfordshire OX11 0QX, UK
- M M Notley
- Central Laser Facility, STFC Rutherford Appleton Laboratory , Oxfordshire OX11 0QX, UK
- M Nakatsutsumi
- LULI, École Polytechnique , CNRS, CEA, Palaiseau, France; European XFEL , GmbH, Albert-Einstein-Ring 19, 22671 Hamburg, Germany
- R Prasad
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK; Institute for Laser and Plasma Physics, Heinrich Heine University , Düsseldorf, D-40225, Germany
- G Scott
- SUPA Department of Physics, University of Strathclyde , Glasgow G4 0NG, UK; Central Laser Facility, STFC Rutherford Appleton Laboratory , Oxfordshire OX11 0QX, UK
- M Tampo
- Graduate School of Engineering, Osaka University , Osaka D-565-0871, Japan
- M Zepf
- Centre for Plasma Physics, Queen’s University Belfast BT7 1NN , UK
- J Schreiber
- Fakultät für Physik, Ludwig-Maximilians-Universität München , Am Coulombwall 1, D-85748 Garching, Germany; Max-Planck-Institut für Quantenoptik , Hans-Kopfermann-Str. 1, D-85748 Garching, Germany
- Z Najmudin
- The John Adams Institute for Accelerator Science , Blackett Laboratory, Imperial College, London SW7 2BZ, UK
- DOI
- https://doi.org/10.1088/1367-2630/18/1/013038
- Journal volume & issue
-
Vol. 18,
no. 1
p. 013038
Abstract
Spectrally-peaked proton beams of high charge ( ${E}_{{\rm{p}}}\approx 8\;{\rm{MeV}}$ , ${\rm{\Delta }}E\approx 4\;{\rm{MeV}}$ , $N\approx 50$ nC ) have been observed from the interaction of an intense laser ( $\gt {10}^{19}$ W cm ^−2 ) with ultrathin CH foils, as measured by spectrally-resolved full beam profiles. These beams are reproducibly generated for foil thicknesses 5–100 nm, and exhibit narrowing divergence with decreasing target thickness down to $\approx 8^\circ $ for 5 nm. Simulations demonstrate that the narrow energy spread feature is a result of buffered acceleration of protons. The radiation pressure at the front of the target results in asymmetric sheath fields which permeate throughout the target, causing preferential forward acceleration. Due to their higher charge-to-mass ratio, the protons outrun a carbon plasma driven in the relativistic transparency regime.
Keywords