We briefly present in this paper the results of 1200eV non-coplanar symmetric (e, 2e) binding energy spectrum of argon and an electron momentum profile of argon 3p.They were measured by a newly constructed spectromete...We briefly present in this paper the results of 1200eV non-coplanar symmetric (e, 2e) binding energy spectrum of argon and an electron momentum profile of argon 3p.They were measured by a newly constructed spectrometer with position-sensitive detectors in USTC. We use non-birming mode to get the Ar3p、 3s and 3s satellites binding energy spectra separately. The experAnental results is well consistent with the available theoretical results.展开更多
The electron momentum distribution of 3σ_u orbital of carbon dioxide has been measured at high momentum resolution. Through comparation between experimental and theoretical results, the calculation by DFT-B3LYP metho...The electron momentum distribution of 3σ_u orbital of carbon dioxide has been measured at high momentum resolution. Through comparation between experimental and theoretical results, the calculation by DFT-B3LYP method using 6- 311 + +G basis set is more agreement with the experirnental data than other calculations.展开更多
文摘We briefly present in this paper the results of 1200eV non-coplanar symmetric (e, 2e) binding energy spectrum of argon and an electron momentum profile of argon 3p.They were measured by a newly constructed spectrometer with position-sensitive detectors in USTC. We use non-birming mode to get the Ar3p、 3s and 3s satellites binding energy spectra separately. The experAnental results is well consistent with the available theoretical results.
文摘The electron momentum distribution of 3σ_u orbital of carbon dioxide has been measured at high momentum resolution. Through comparation between experimental and theoretical results, the calculation by DFT-B3LYP method using 6- 311 + +G basis set is more agreement with the experirnental data than other calculations.
