<p>The emission angular distributions, the transverse momentum distributions, and the temperature parameters of projectile fragments produced in fragmentation of <InlineEquation ID="IEq3"> <InlineMediaObject> <ImageObject Color="BlackWhite" FileRef="40042_2025_1411_Article_IEq3.gif" Format="GIF" Height="10" Rendition="HTML" Resolution="72" Type="Linedraw" Width="13" /> </InlineMediaObject> <EquationSource Format="TEX">\(^{40}\)</EquationSource> <EquationSource Format="MATHML"><math> <mmultiscripts> <mrow /> <mrow /> <mn>40</mn> </mmultiscripts> </math></EquationSource> </InlineEquation>Ar on Al and Cu targets at 500 A MeV are investigated using the solid nuclear track detector CR-39. It is found that the mean value and the width of the angular distribution are increased with the decrease of the charge of projectile fragments. The cumulative squared transverse momentum distribution of projectile fragments can be well fitted by a single Rayleigh distribution, which indicates that the projectile fragments are emitted from a single temperature emission source. The temperatures of projectile fragments emission source are in the range of 2–10 MeV, increase with the decrease of the charge of the projectile fragments.</p>

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Temperature of projectile fragment emission source in fragmentation of \(^\mathbf{40}\)Ar at 500 A MeV

  • Rong Li,
  • Ying-Hua Dang,
  • Jing-Xiao Kang,
  • Jun-Sheng Li,
  • Dong-Hai Zhang

摘要

The emission angular distributions, the transverse momentum distributions, and the temperature parameters of projectile fragments produced in fragmentation of \(^{40}\) 40 Ar on Al and Cu targets at 500 A MeV are investigated using the solid nuclear track detector CR-39. It is found that the mean value and the width of the angular distribution are increased with the decrease of the charge of projectile fragments. The cumulative squared transverse momentum distribution of projectile fragments can be well fitted by a single Rayleigh distribution, which indicates that the projectile fragments are emitted from a single temperature emission source. The temperatures of projectile fragments emission source are in the range of 2–10 MeV, increase with the decrease of the charge of the projectile fragments.