Single-electron-detachment cross sections of Fe− , Ru− , Ni− , Pd− , and Pt− in collisions with inert-gas atoms

2017 ◽  
Vol 95 (6) ◽  
Author(s):  
Guangxin Min ◽  
Guannan Guo ◽  
Dedong Wang ◽  
Xuemei Zhang
2020 ◽  
Vol 98 (3) ◽  
pp. 287-290
Author(s):  
Mingmin Luo ◽  
Yujia Zhai ◽  
Guannan Guo ◽  
Xuemei Zhang

The single-electron and double-electron detachment cross sections of Cl– in collision with inert gas atoms (He–Xe) have been measured by the growth rate method. The incident negative ions’ energies are from 5 to 30 keV. It is found that the single-electron detachment cross sections become greater and greater when the target atoms change from helium to xenon. However, double-electron detachment cross sections show a more complicated relationship with the target atom changing. The results of this work have been compared with the previous data, and a model based on energy division is used to interpret the trends of cross sections.


2004 ◽  
Vol 21 (8) ◽  
pp. 1512-1514 ◽  
Author(s):  
Huang Yong-Yi ◽  
Zhang Xue-Mei ◽  
Wu Shi-Min ◽  
Li Guang-Wu ◽  
Lu Fu-Quan

2013 ◽  
Vol 91 (2) ◽  
pp. 175-179 ◽  
Author(s):  
Zhixian Geng ◽  
Xue Bai ◽  
Baoren Wei ◽  
Xuemei Zhang

The single-electron detachment (SED) cross sections for Co− and Ir− in collision with Ar in the energy region of 10–30 keV are obtained in our laboratory. As our previous paper reported, the SED cross sections have velocity and electron affinity dependency. Using the least-squares method, we analyze the available experimental data of SED cross sections for different negative ions in collision with Ar, and get empirical formulas for different sets of anionic projectiles. For most anionic projectiles, there is a clear correlation between increasing electron affinity and decreasing SED cross sections. Co and Ir, however, are an exception, and we discuss how other physical parameters can be taken into account in the search for general scaling rules for SED cross sections. As the incident velocity increases, the cross section dependence of the anion's electron affinity becomes weaker, and the relation between the SED cross sections and νp is supposed to be [Formula: see text].


2001 ◽  
Vol 18 (10) ◽  
pp. 1344-1345 ◽  
Author(s):  
Li Guang-Wu ◽  
Zhang Xue-Mei ◽  
Wu Shi-Min ◽  
Lu Fu-Quan ◽  
Peng Xian-Jue ◽  
...  

1995 ◽  
Vol 51 (2) ◽  
pp. 1351-1359 ◽  
Author(s):  
T. J. Kvale ◽  
J. S. Allen ◽  
X. D. Fang ◽  
A. Sen ◽  
R. Matulioniene

2002 ◽  
Vol 66 (3) ◽  
Author(s):  
Xuemei Zhang ◽  
Shimin Wu ◽  
Weiguo Jin ◽  
Guangwu Li ◽  
Fuquan Lu ◽  
...  

2001 ◽  
Vol 56 (6) ◽  
pp. 797-800 ◽  
Author(s):  
Xuemei Zhang ◽  
Shimin Wu ◽  
Guangwu Li ◽  
Fuquan Lu ◽  
Jiayong Tang ◽  
...  

Atoms ◽  
2021 ◽  
Vol 9 (2) ◽  
pp. 33
Author(s):  
R.I. Campeanu ◽  
Colm T. Whelan

Triple differential cross sections (TDCS) are presented for the electron and positron impact ionization of inert gas atoms in a range of energy sharing geometries where a number of significant few body effects compete to define the shape of the TDCS. Using both positrons and electrons as projectiles has opened up the possibility of performing complementary studies which could effectively isolate competing interactions that cannot be separately detected in an experiment with a single projectile. Results will be presented in kinematics where the electron impact ionization appears to be well understood and using the same kinematics positron cross sections will be presented. The kinematics are then varied in order to focus on the role of distortion, post collision interaction (pci), and interference effects.


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