Practical formulas for inner-shell ionization cross sections by electron impact: Applications in quantitative Auger electron spectroscopy

被引:5
作者
Jablonski, A. [1 ]
Salvat, F. [2 ,3 ]
Powell, C. J. [4 ]
机构
[1] Polish Acad Sci, Inst Phys Chem, PL-01224 Warsaw, Poland
[2] Univ Barcelona, Fac Fis, ECM, E-08028 Barcelona, Spain
[3] Univ Barcelona, Fac Fis, ICC, E-08028 Barcelona, Spain
[4] NIST, Surface & Microanal Sci Div, Gaithersburg, MD 20899 USA
关键词
aluminium; Auger electron spectra; copper; electron backscattering; gold; inner-shell ionisation; silicon; silver; MEAN FREE PATHS; EXCITATION DEPTH DISTRIBUTION; K-SHELL; BACKSCATTERING FACTOR; ELASTIC-SCATTERING; ATOMS; VIII; AES; SI;
D O I
10.1063/1.3195046
中图分类号
O59 [应用物理学];
学科分类号
摘要
We evaluated analytical formulas for the inner-shell ionization cross section from three sources in calculations of the backscattering factor (BF) for quantitative Auger electron spectroscopy: the Gryzinski expression from classical atomic physics, the Casnati [J. Phys. B 15, 155 (1982)] formula from fits to measured K-shell cross sections, and two expressions from Bote [At. Data Nucl. Data Tables (unpublished)] from fits to improved calculations of ionization cross sections by Bote and Salvat [Phys. Rev. A 77, 042701 (2008)]. BFs were calculated for five illustrative Auger transitions (Al KL23L23, Si KL23L23, Cu L3M45M45, Ag M4N45N45, and Au M5N67N67 in the respective elemental solids) for primary energies from the threshold for ionization to 30 keV. Differences between BFs calculated from the expressions of Bote and those from the expressions of Casnati were less than 2%, while the differences between BFs from the expressions of Bote and those from the Gryzinski expression were less than 5.4%. BFs from the expressions of Bote were also compared with BFs from a widely used formula of Shimizu with differences between 7% and 15% at 30 keV. The Shimizu [Jpn. J. Appl. Phys., Part 1 22, 1631 (1983)] formula was derived for primary energies from 3 to 10 keV but is widely employed in quantitative Auger applications for higher energies. The differences between BFs from the expressions of Bote and the Shimizu formula arise from the improved models and data now available.
引用
收藏
页数:13
相关论文
共 54 条
  • [1] *ASTM INT, 2008, ANN BOOK ASTM STAND, P675
  • [2] Bethe H, 1930, ANN PHYS-BERLIN, V5, P325
  • [3] BOTE D, AT DATA NUCL D UNPUB
  • [4] Calculations of inner-shell ionization by electron impact with the distorted-wave and plane-wave Born approximations
    Bote, David
    Salvat, Francesc
    [J]. PHYSICAL REVIEW A, 2008, 77 (04):
  • [5] CASNATI E, 1982, J PHYS B-AT MOL OPT, V15, P155, DOI 10.1088/0022-3700/15/1/022
  • [6] Inner-shell electron-impact ionization of neutral atoms
    Colgan, J.
    Fontes, C. J.
    Zhang, H. L.
    [J]. PHYSICAL REVIEW A, 2006, 73 (06):
  • [7] Improved calculation of the backscattering factor for quantitative analysis by Auger electron spectroscopy
    Ding, Z. J.
    Tan, W. S.
    Li, Y. G.
    [J]. JOURNAL OF APPLIED PHYSICS, 2006, 99 (08)
  • [8] Fujita D, 1996, SURF INTERFACE ANAL, V24, P211, DOI 10.1002/(SICI)1096-9918(199603)24:3<211::AID-SIA99>3.0.CO
  • [9] 2-M
  • [10] Extraction of depth distributions of electron-excited Auger electrons in Fe, Ni and Si using inelastic peak shape analysis
    Fujita, D
    Schleberger, M
    Tougaard, S
    [J]. SURFACE SCIENCE, 1996, 357 (1-3) : 180 - 185