Thick-target method in the measurement of inner-shell ionization cross-sections by low-energy electron impact

被引:18
作者
An, Z.
Wu, Y.
Liu, M. T.
Duan, Y. M.
Tang, C. H.
机构
[1] Sichuan Univ, Key Lab Radiat Phys & Technol, Minist Educ, Inst Nucl Sci & Technol, Chengdu 610064, Peoples R China
[2] China Acad Engn Phys, Laser Fus Res Ctr, Mianyang 621900, Peoples R China
基金
高等学校博士学科点专项科研基金; 中国国家自然科学基金;
关键词
electron impact; atomic inner-shell ionization cross-sections; Monte Carlo simulation;
D O I
10.1016/j.nimb.2005.12.051
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
In this paper, we have studied the thick-target method for the measurements of atomic inner-shell ionization cross-section or X-ray production cross-section by keV electron impact. We find that in the processes of electron impact on the thick targets, the ratios of the characteristic X-ray yields of photoelectric ionization by bremsstrahlung to the total characteristic X-ray yields are Z-dependent and shell-dependent. and the ratios also show the weak energy-dependence. In addition, in the lower incident energy region (i.e. U < 5-6) the contribution from the rediffusion effect and the secondary electrons call be negligible. In general, the thick-target method call be appropriately applied to the measurements of atomic inner-shell ionization cross-sections or X-ray production cross-sections by electron impact for low and medium Z elements in the lower incident electron energy (i.e. U < 5-6). The experimental accuracies by the thick-target method can reach to the level equivalent or superior to the accuracies of experimental data based on the thin-target method. This thick-target method has been applied to the measurement of K-shell ionization cross-sections of Ni element by electron impact in this paper. (c) 2005 Elsevier B.V. All rights reserved.
引用
收藏
页码:281 / 287
页数:7
相关论文
共 45 条
[1]   Monte Carlo simulation of bremsstrahlung emission by electrons [J].
Acosta, E ;
Llovet, X ;
Salvat, F .
APPLIED PHYSICS LETTERS, 2002, 80 (17) :3228-3230
[2]   Correction of substrate effect in the measurement of 8-25-keV electron-impact K-shell ionization cross sections of Cu and Co elements [J].
An, Z ;
Li, TH ;
Wang, LM ;
Xia, XY ;
Luo, ZM .
PHYSICAL REVIEW A, 1996, 54 (04) :3067-3069
[3]   Some recent progress on the measurement of K-shell ionization cross-sections of atoms by electron impact: Application to Ti and Cr elements [J].
An, Z ;
Liu, MT ;
Fu, YC ;
Luo, ZM ;
Tang, CH ;
Li, CM ;
Zhang, BH ;
Tang, YJ .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS, 2003, 207 (03) :268-274
[4]   On the efficiency calibration of Si(Li) detector in the low-energy region using thick-target bremsstrahlung [J].
An, Z ;
Liu, MT .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS, 2002, 194 (04) :513-518
[5]   Study of cross-sections for the K-shell ionization of atoms by electron and positron impact [J].
An, Z ;
Luo, ZM ;
Tang, C .
NUCLEAR INSTRUMENTS & METHODS IN PHYSICS RESEARCH SECTION B-BEAM INTERACTIONS WITH MATERIALS AND ATOMS, 2001, 179 (03) :334-342
[6]   Measurement of the mass attenuation coefficient for elemental materials in the range 6 ≤, Z ≤ 82 using X-rays from 13 up to 50 kev [J].
Angelone, M ;
Bubba, T ;
Esposito, A .
APPLIED RADIATION AND ISOTOPES, 2001, 55 (04) :505-511
[7]   Measurement of the K X-ray absorption jump ratio of erbium by attenuation of a Compton peak [J].
Ayala, AP ;
Mainardi, RT .
RADIATION PHYSICS AND CHEMISTRY, 1996, 47 (02) :177-181
[8]  
Berger MJ, 1999, ESTAR PSTAR ASTAR CO
[9]   Measurements of L-shell x-ray production cross sections of W, Pt, and Au by 10-30-keV electrons -: art. no. 012719 [J].
Campos, CS ;
Vasconcellos, MAZ ;
Llovet, X ;
Salvat, F .
PHYSICAL REVIEW A, 2002, 66 (01) :127191-127199
[10]  
CASNATI E, 1983, J PHYS B-AT MOL OPT, V16, P505, DOI 10.1088/0022-3700/16/3/525