Dynamics and structure of self-generated magnetics fields on solids following high contrast, high intensity laser irradiation
Creators
- Albertazzi, B.1, 2, 3
- Chen, S. N.4, 3
- Fuchs, J.4, 3
- Antici, P.5, 2
- Böker, J.6
- Swantusch, M.6
- Willi, O.6
- Borghesi, M.7
- Breil, J.8
- Feugeas, J. L.8
- Nicolaï, Ph.8
- Tikhonchuk, V. T.8
- D'Humières, E.8
- Dervieux, V.3
- Nakatsutsumi, M.3
- Romagnagni, L.3
- Lancia, L.5
- Shepherd, R.9
- Sentoku, Y.10
- Starodubtsev, M.4
- and others
- 1. Graduate School of Engineering, University of Osaka, Suita, Osaka 565-087 (Japan)
- 2. INRS-EMT, 1650 bd L. Boulet, J3X1S2, Varennes, Québec (Canada)
- 3. LULI, École Polytechnique, CNRS, CEA, UPMC, 91128 Palaiseau (France)
- 4. Institute of Applied Physics, 46 Ulyanov Street, 603950 Nizhny Novgorod (Russian Federation)
- 5. Dept. SBAI, Universita di Roma "La Sapienza," Via A. Scarpa 14, 00161 Rome (Italy)
- 6. Institut für Laser-und Plasmaphysik, Heinrich-Heine-Universität, Düsseldorf (Germany)
- 7. School of Mathematics and Physics, The Queen's University, Belfast (United Kingdom)
- 8. CELIA, University of Bordeaux - CNRS - CEA, 33405 Talence (France)
- 9. LLNL, East Av., Livermore, California 94550 (United States)
- 10. Department of Physics, University of Nevada, Reno, Nevada 89557-0058 (United States)
Description
The dynamics of self-generated magnetic B-fields produced following the interaction of a high contrast, high intensity (I > 1019 W cm−2) laser beam with thin (3 μm thick) solid (Al or Au) targets is investigated experimentally and numerically. Two main sources drive the growth of B-fields on the target surfaces. B-fields are first driven by laser-generated hot electron currents that relax over ∼10–20 ps. Over longer timescales, the hydrodynamic expansion of the bulk of the target into vacuum also generates B-field induced by non-collinear gradients of density and temperature. The laser irradiation of the target front side strongly localizes the energy deposition at the target front, in contrast to the target rear side, which is heated by fast electrons over a much larger area. This induces an asymmetry in the hydrodynamic expansion between the front and rear target surfaces, and consequently the associated B-fields are found strongly asymmetric. The sole long-lasting (>30 ps) B-fields are the ones growing on the target front surface, where they remain of extremely high strength (∼8–10 MG). These B-fields have been recently put by us in practical use for focusing laser-accelerated protons [B. Albertazzi et al., Rev. Sci. Instrum. 86, 043502 (2015)]; here we analyze in detail their dynamics and structure
Additional details
Identifiers
- DOI
- 10.1063/1.4936095;
Publishing Information
- Journal Title
- Physics of Plasmas
- Journal Volume
- 22
- Journal Issue
- 12
- Journal Page Range
- p. 123108-123108.11
- ISSN
- 1070-664X
- CODEN
- PHPAEN
INIS
- Country of Publication
- United States
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 47060020
- Subject category
- S70: PLASMA PHYSICS AND FUSION TECHNOLOGY;
- Descriptors DEI
- ASYMMETRY; DENSITY; ELECTRONS; ENERGY ABSORPTION; FOCUSING; LASER RADIATION; MAGNETIC FIELDS; PHOTON BEAMS; PROTONS; SOLIDS; SURFACES; TEMPERATURE GRADIENTS
- Descriptors DEC
- ABSORPTION; BARYONS; BEAMS; ELECTROMAGNETIC RADIATION; ELEMENTARY PARTICLES; FERMIONS; HADRONS; LEPTONS; NUCLEONS; PHYSICAL PROPERTIES; RADIATIONS; SORPTION
Optional Information
- Notes
- (c) 2015 AIP Publishing LLC