Number of the records: 1  

Electron emission from laser irradiating target normal sheath acceleration (TNSA)

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    SYSNO ASEP0471158
    Document TypeJ - Journal Article
    R&D Document TypeJournal Article
    Subsidiary JČlánek ve WOS
    TitleElectron emission from laser irradiating target normal sheath acceleration (TNSA)
    Author(s) Torrisi, L. (IT)
    Cutroneo, Mariapompea (UJF-V) ORCID, RID, SAI
    Number of authors2
    Source TitleRadiation Effects and Defects in Solids. - : Taylor & Francis - ISSN 1042-0150
    Roč. 171, 9-10 (2016), s. 754-765
    Number of pages12 s.
    Publication formPrint - P
    Action12th Workshop on European Collaboration for Higher Education and Research in Nuclear Engineering and Radiological Protection
    Event date30.05.2016 - 01.06.2016
    VEvent locationBologna, Catania, Milan
    CountryIT - Italy
    Event typeEUR
    Languageeng - English
    CountryGB - United Kingdom
    Keywordselectron emission from plasma ; TNSA ; TOF ; SiC ; plastic scintillator ; Thomson parabola spectrometer
    Subject RIVBH - Optics, Masers, Lasers
    R&D ProjectsGBP108/12/G108 GA ČR - Czech Science Foundation (CSF)
    LM2015056 GA MŠMT - Ministry of Education, Youth and Sports (MEYS)
    Institutional supportUJF-V - RVO:61389005
    UT WOS000392416100008
    EID SCOPUS85007340848
    DOI10.1080/10420150.2016.1261862
    AnnotationA study of the electron emission from laser-generated plasma in target normal sheath acceleration regime is presented for different targets. The used laser has an intensity of about 10(16)W/cm(2) and a pulse duration of 300ps. Electrons were detected using SiC detectors and plastic scintillators employed in time-of-flight configuration and a Thomson parabola spectrometer (TPS). Measurements indicated the presence of hot electrons with a kinetic energy of the order of some MeVs. SiC and scintillators detect electrons up to about 400keV while TPS electrons up to about 5MeV energy. Electrons yield emitted in the forward direction is proportional to the effective atomic number of the target and is inversely proportional to the target thickness.
    WorkplaceNuclear Physics Institute
    ContactMarkéta Sommerová, sommerova@ujf.cas.cz, Tel.: 266 173 228
    Year of Publishing2017
Number of the records: 1  

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