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REN Hui-juan, ZHANG Xiao-an, #, XIAO Guo-qing. Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface[J]. Nuclear Physics Review, 2009, 26(2): 146-149. doi: 10.11804/NuclPhysRev.26.02.146
Citation: REN Hui-juan, ZHANG Xiao-an, #, XIAO Guo-qing. Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface[J]. Nuclear Physics Review, 2009, 26(2): 146-149. doi: 10.11804/NuclPhysRev.26.02.146

Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface

doi: 10.11804/NuclPhysRev.26.02.146
  • Received Date: 1900-01-01
  • Rev Recd Date: 1900-01-01
  • Publish Date: 2009-06-20
  • The Au atomic Mα characteristic Xray spectrum has been measured for the slow highly charged ions Arq+ (q= 7—14) impacting on Au surface. The result shows that as long as the charge state of projectile is higher(q=11), the characteristic Xrays of heavy atomic can be effectively excited even though the ionic beam is very weak(nA magnitude), and the single ionic Xray yield is in the order of 10-8 and increases with potential energies of projectiles.
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    沈阳化工大学材料科学与工程学院 沈阳 110142

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Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface

doi: 10.11804/NuclPhysRev.26.02.146

Abstract: The Au atomic Mα characteristic Xray spectrum has been measured for the slow highly charged ions Arq+ (q= 7—14) impacting on Au surface. The result shows that as long as the charge state of projectile is higher(q=11), the characteristic Xrays of heavy atomic can be effectively excited even though the ionic beam is very weak(nA magnitude), and the single ionic Xray yield is in the order of 10-8 and increases with potential energies of projectiles.

REN Hui-juan, ZHANG Xiao-an, #, XIAO Guo-qing. Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface[J]. Nuclear Physics Review, 2009, 26(2): 146-149. doi: 10.11804/NuclPhysRev.26.02.146
Citation: REN Hui-juan, ZHANG Xiao-an, #, XIAO Guo-qing. Xray Spectra Excited in Ar q+(q=7—14) Incidence on Au Surface[J]. Nuclear Physics Review, 2009, 26(2): 146-149. doi: 10.11804/NuclPhysRev.26.02.146

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