1 Ocak 2019 Dergi makalesi Açık Erişim

Sangwan, D.; Culfa, O.; Ridgers, C. P.; Aogaki, S.; Stutman, D.; Diaconescu, B.

JSON-LD (schema.org)

{
  "@context": "https://schema.org/", 
  "@id": 74927, 
  "@type": "ScholarlyArticle", 
  "creator": [
    {
      "@type": "Person", 
      "affiliation": "Horia Hulubei Natl Inst Phys & Nucl Engn, Extreme Light Infrastruct Nucl Phys ELI NP, Magurele, Romania", 
      "name": "Sangwan, D."
    }, 
    {
      "@type": "Person", 
      "name": "Culfa, O."
    }, 
    {
      "@type": "Person", 
      "affiliation": "Univ York, York Plasma Inst, Dept Phys, York YO10 5DD, N Yorkshire, England", 
      "name": "Ridgers, C. P."
    }, 
    {
      "@type": "Person", 
      "affiliation": "Horia Hulubei Natl Inst Phys & Nucl Engn, Extreme Light Infrastruct Nucl Phys ELI NP, Magurele, Romania", 
      "name": "Aogaki, S."
    }, 
    {
      "@type": "Person", 
      "name": "Stutman, D."
    }, 
    {
      "@type": "Person", 
      "affiliation": "Horia Hulubei Natl Inst Phys & Nucl Engn, Extreme Light Infrastruct Nucl Phys ELI NP, Magurele, Romania", 
      "name": "Diaconescu, B."
    }
  ], 
  "datePublished": "2019-01-01", 
  "description": "We present results of 2D particle-in-cell (PIC) simulations of carbon ion acceleration by 10 petawatt (PW) laser pulses, studying both circular polarized (CP) and linear polarized (LP) pulses. We carry out a thickness scanning of a solid carbon target to investigate the ideal thickness for carbon ion acceleration mechanisms using a 10 PW laser with an irradiance of 5 x 10(22) W cm(-2). The energy spectra of carbon ions and electrons and their temperature are studied. Additionally, for the carbon ions, their angular divergence is studied. It is shown that the ideal thickness for the carbon acceleration is 120 nm and the cutoff energy for carbon ions is 5 and 3 GeV for CP and LP pulses, respectively. The corresponding carbon ions temperature is 1 and 0.75 GeV. On the other hand, the energy cutoff for the electrons is 500 MeV with LP and 400 MeV with CP laser pulses. We report that the breakout afterburner mechanism is most likely causing the acceleration of carbon ions to such high energies for the optimal target thickness.", 
  "headline": "Simulations of carbon ion acceleration by 10 PW laser pulses on ELI-NP", 
  "identifier": 74927, 
  "image": "https://aperta.ulakbim.gov.tr/static/img/logo/aperta_logo_with_icon.svg", 
  "license": "http://www.opendefinition.org/licenses/cc-by", 
  "name": "Simulations of carbon ion acceleration by 10 PW laser pulses on ELI-NP", 
  "url": "https://aperta.ulakbim.gov.tr/record/74927"
}