The K-shell ionization probability Pk was measured as a function of Ep across the strong resonance 56Fe(p,p)56Fe at 2.522 MeV and about 50 % variation was observed. For a large ratio of the K-shell binding energy to t...The K-shell ionization probability Pk was measured as a function of Ep across the strong resonance 56Fe(p,p)56Fe at 2.522 MeV and about 50 % variation was observed. For a large ratio of the K-shell binding energy to the total width of the nuclear resonance, Uk/Г≥5, the present experimental result is still in good agreement with theoretical calculation based on Blair and Anholt’s formula.展开更多
The projectile energy dependence of K-shell ionization probability have been measured across the narrow resonance 2.522Mev with large ratio of Uk/Г=5.3 in the reaction^(56)Fe(p,p)^(56)Fe.The frame work of the theory ...The projectile energy dependence of K-shell ionization probability have been measured across the narrow resonance 2.522Mev with large ratio of Uk/Г=5.3 in the reaction^(56)Fe(p,p)^(56)Fe.The frame work of the theory proposed by Blair and Anholt was introduced to analyze the results.展开更多
基金The Project Supported by National Natural Science Foundation of China
文摘The K-shell ionization probability Pk was measured as a function of Ep across the strong resonance 56Fe(p,p)56Fe at 2.522 MeV and about 50 % variation was observed. For a large ratio of the K-shell binding energy to the total width of the nuclear resonance, Uk/Г≥5, the present experimental result is still in good agreement with theoretical calculation based on Blair and Anholt’s formula.
基金Project supported by the Chinese National Science Foundation of Doctoral Research.
文摘The projectile energy dependence of K-shell ionization probability have been measured across the narrow resonance 2.522Mev with large ratio of Uk/Г=5.3 in the reaction^(56)Fe(p,p)^(56)Fe.The frame work of the theory proposed by Blair and Anholt was introduced to analyze the results.
