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Laser-driven proton-boron reaction for alpha particles production

POSTER

Abstract

The fusion reaction P + 11B generates 3 alpha-particles with a total energy of 8.7 MeV. It opens the possibility of developing a novel generation of high brightness alpha-particle source, with potential interest in astrophysics, fusion energy [1] and medical in particular for the production of radioisotopes for diagnostics or medical treatment [2].

This work aims at studying different schemes of laser-driven p-11B reaction exploiting the high-power and the high repetition rate of VEGAIII laser to improve the alpha production detection and Scandium radioisotope production. Different setups are proposed: (i) Pitcher-catcher configuration: TNSA proton produced from thin aluminium foil target (Pitcher) interact on a solid B type target (catcher) and (ii) Directly irradiation of solid samples of Boron-nitride (BN) target.

We present in this work the experimental setup and the diagnostics used during the campaign, as well as the first preliminary results of the experiment.

[1] H. Hora, et al. Laser and Particle Beams (2015), 33, 607–619

[2] K. Szkliniarz, et al. Applied Radiation and Isotopes 118, 182 (2016)

Presenters

  • Didier Raffestin

    Celia University of Bordeaux

Authors

  • Didier Raffestin

    Celia University of Bordeaux

  • Marine Huault

    Departamento de Física fundamental, Universidad de Salamanca, 37008 Salamanca, Spain

  • Katarzina BATANI

    IPPLM Institute of Plasma Physics and Laser Microfusion, Hery Street 23, 01-497, Warsaw, Poland

  • Howel Larreur

    Departamento de Física fundamental, Universidad de Salamanca, 37008 Salamanca, Spain

  • Philippe Nicolaï

    Université de Bordeaux, CNRS, CEA, CELIA (Centre Lasers Intenses et Applications), Unité Mixte de Recherche 5107, Talence 33400, France

  • Diluka Singappuli

    Université de Bordeaux, CNRS, CEA, CELIA (Centre Lasers Intenses et Applications), Unité Mixte de Recherche 5107, Talence 33400, France

  • Lorenzo Giuffrida

    ELI Beamlines Facility, Institute of Physics of the CAS, v.v.i (FZU), ELI-Beamlines, Prague, Czech Republic

  • Vasiliky Kantarelou

    Institute of Physics of the CAS, v.v.i (FZU), ELI-Beamlines, Prague, Czech Republic

  • stanislav stancek

    Institute of Physics of the CAS, v.v.i (FZU), ELI-Beamlines, Prague, Czech Republic

  • Mattia Cipriani

    ENEA Fusion and Technologies for Nuclear Safety and Security Department-C. R. Frascati, Via Enrico Fermi 45, 00044 Frascati, Italy

  • Fabrizio Consoli

    ENEA Fusion and Technologies for Nuclear Safety and Security Department-C. R. Frascati, Via Enrico Fermi 45, 00044 Frascati, Italy

  • Massimiliano Scisciò

    ENEA, C. R. Casaccia, Via Anguillarese 301, 00123 Rome, Italy., ENEA Fusion and Technologies for Nuclear Safety and Security Department-C. R. Frascati, Via Enrico Fermi 45, 00044 Frascati, Italy

  • Francesco Filippi

    ENEA Fusion and Technologies for Nuclear Safety and Security Department-C. R. Frascati, Via Enrico Fermi 45, 00044 Frascati, Italy

  • Nardjesse Boudjema

    Departamento de Física fundamental, Universidad de Salamanca, 37008 Salamanca, Spain

  • Roberto Lera Matellanes

    Centro de Láseres Pulsados, Edificio M5, Parque Científico, C/ Adaja 8, 37185 Villamayor, Salamanca, Spain

  • José Antonio Pérez

    Centro de Láseres Pulsados, Edificio M5, Parque Científico, C/ Adaja 8, 37185 Villamayor, Salamanca, Spain

  • Aldo Bonasera

    Texas A&M University

  • marcia Rodrigues

    Cyclotron Institute, Texas A&M University, College Station, TX 77843, USA

  • daniela ramirez

    Cyclotron Institute, Texas A&M University, College Station, TX 77843, USA

  • Dimitri Batani

    Université de Bordeaux, CNRS, CEA, CELIA (Centre Lasers Intenses et Applications), Unité Mixte de Recherche 5107, Talence 33400, France