6.0-10.0-MeV/u He{sup 2+}-ion-induced electron emission from water vapor
6.0-10.0-MeV/u He{sup 2+}-ion-induced electron emission from water vapor
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6.0-10.0-MeV/u He{sup 2 }-离子引起的水蒸气电子发射
DOI：
10.1103/physreva.72.062710
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发表时间：
2005
影响因子：
2.9
通讯作者：
F. Soga
中科院分区：
文献类型：
--
作者：
D. Ohsawa;Y. Sato;Y. Okada;V. Shevelko;F. Soga
We discuss absolute doubly differential cross sections (DDCS's) for the energy and angular distributions (20\ifmmode^\circ\else\textdegree\fi{}\char21{}160\ifmmode^\circ\else\textdegree\fi{}) of secondary electrons produced in the collisions of 6.0- and $10.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions with water vapor. Details of our experiments were reported in our previous paper [D. Ohsawa et al., Nucl. Instrum. Methods Phys. Res. B 227, 431 (2005)], which mainly considered the total uncertainty $(\ifmmode\pm\else\textpm\fi{}13%)$, as well as absolute DDCS data $(7\char21{}10\phantom{\rule{0.2em}{0ex}}000\phantom{\rule{0.3em}{0ex}}\mathrm{eV})$ by $6.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions. All DDCS data, including the newly obtained data $(20\char21{}12\phantom{\rule{0.2em}{0ex}}000\phantom{\rule{0.3em}{0ex}}\mathrm{eV})$ by $10.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions, are compared with classical theories after being corrected for relativistic effects. Based on the Rudd model and the Rutherford cross section, the experimental results are discussed by taking account of the momentum spread of the bound electrons. This paper mainly describes the analysis of low-energy electrons and binary encounter peaks at high energies, as well as details of relativistic corrections.
We discuss absolute doubly differential cross sections (DDCS's) for the energy and angular distributions (20\ifmmode^\circ\else\textdegree\fi{}\char21{}160\ifmmode^\circ\else\textdegree\fi{}) of secondary electrons produced in the collisions of 6.0- and $10.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions with water vapor. Details of our experiments were reported in our previous paper [D. Ohsawa et al., Nucl. Instrum. Methods Phys. Res. B 227, 431 (2005)], which mainly considered the total uncertainty $(\ifmmode\pm\else\textpm\fi{}13%)$, as well as absolute DDCS data $(7\char21{}10\phantom{\rule{0.2em}{0ex}}000\phantom{\rule{0.3em}{0ex}}\mathrm{eV})$ by $6.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions. All DDCS data, including the newly obtained data $(20\char21{}12\phantom{\rule{0.2em}{0ex}}000\phantom{\rule{0.3em}{0ex}}\mathrm{eV})$ by $10.0\text{\ensuremath{-}}\mathrm{MeV}∕\mathrm{u}$ ${\mathrm{He}}^{2+}$ ions, are compared with classical theories after being corrected for relativistic effects. Based on the Rudd model and the Rutherford cross section, the experimental results are discussed by taking account of the momentum spread of the bound electrons. This paper mainly describes the analysis of low-energy electrons and binary encounter peaks at high energies, as well as details of relativistic corrections.