Počet záznamů: 1  

Laser Power Density Dependence on Charge State Distribution of Ta Ion Laser Plasma

  1. 1.
    SYSNO ASEP0524538
    Druh ASEPJ - Článek v odborném periodiku
    Zařazení RIVJ - Článek v odborném periodiku
    Poddruh JČlánek ve WOS
    NázevLaser Power Density Dependence on Charge State Distribution of Ta Ion Laser Plasma
    Tvůrce(i) Okamura, M. (JP)
    Tamis, A. (US)
    Whelan, T. (US)
    Kanesue, T. (US)
    Ikeda, S. (US)
    Cannavó, Antonino (UJF-V) ORCID, SAI
    Celkový počet autorů6
    Číslo článku013325
    Zdroj.dok.Review of Scientific Instruments. - : AIP Publishing - ISSN 0034-6748
    Roč. 91, č. 1 (2020)
    Poč.str.4 s.
    Forma vydáníTištěná - P
    Jazyk dok.eng - angličtina
    Země vyd.US - Spojené státy americké
    Klíč. slovalaser ablation ; laser produced plasma ; accelerator applications
    Vědní obor RIVBG - Jaderná, atomová a mol. fyzika, urychlovače
    Obor OECDNuclear physics
    Způsob publikováníOpen access
    Institucionální podporaUJF-V - RVO:61389005
    UT WOS000602546800001
    EID SCOPUS85078527319
    DOI10.1063/1.5129530
    AnotaceLaser power density per pulse, which is commonly expressed with the unit of 'W/cm2,' is an important parameter to characterize ablation plasma. To match a design charge state of heavy ion beam induced by a laser ion source, a laser power density must be carefully chosen. Above around 108 W/cm2 of laser power density, laser ablation plasma is emitted from the surface of solid material. Then, up to 109 W/cm2, the most abundant charge state is 1+. Because the ionization energy increases with higher charge states, increasing the laser intensity leads to the charge state distribution shifting higher. Increasing the density to increase charge states also results in lower time of flight due to higher velocities. The maximum laser power density is obtained by the smallest available laser spot size on the target material which is determined by the quality of the laser beam. For many accelerator applications, higher charge state beams are preferred. In particular cases, singly charge ion beams are demanded. Therefore, production of intermediate charge state beams has not been investigated well. In this study, we selected Ta4+ as an example demanded beam and tried to clarify how the transition of charge state distribution depends on laser power density. Conclusively, the possible specification of a laser ion source for Ta4+ delivery was elucidated.
    PracovištěÚstav jaderné fyziky
    KontaktMarkéta Sommerová, sommerova@ujf.cas.cz, Tel.: 266 173 228
    Rok sběru2021
    Elektronická adresahttps://doi.org/10.1063/1.5129530
Počet záznamů: 1  

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