Handbook of Ionization Spectra
CONTENT
PREFACE
 
1. PHYSICAL ASPECTS OF IONIZATION SPECTROSCOPY TECHNIQUE
1.1. The nature of ionization spectra
1.2. The role of elastic scattering in ionization spectrum formation for reflection geometry
1.3. Inelastic electron scattering
1.4. IL contour
1.5. Fine structure of ionization spectrum
1.6. Ionization losses
1.7. Opportunities of ionization spectroscopy
 
2. IONIZATION SPECTROSCOPY EQUIPMENT
2.1. Electron spectrometer
2.2. Electron gun
 
3. IL DETECTION
3.1. Detection specifics
3.2. Acceleration voltage fluctuations
3.3. Auger lines suppression
 
4. ADJUSTMENT OF SPECTROMETER'S ELECTRON OPTICS
 
5. SPECTROMETER CALIBRATION
5.1. The goal of calibration
5.2. Calibration of kinetic energy scale
5.3. Electron energy loss scale
5.4. Inspection of spectrometer’s adjustment and calibration
 
6. INTENSITY OF IONIZATION LINES
6.1. IL intensity
6.2. Primary electron energy selection
 
7. SURFACE ANALYSIS BY MEANS OF IS
7.1. Qualitative composition analysis technique
7.2. Standard samples technique
7.3. Elemental sensitivity coefficients technique
7.4. Analysis depth
7.5. Investigation of chemical bonding between the atoms
 
References
Ionisation Spectroscopy: Physical Background and Usage (Contents) On-line Library of IS spectra Info System Software and Library   About Authors

4. ADJUSTMENT OF SPECTROMETER'S ELECTRON OPTICS

The goal of adjustment is to achieve the maximum intensity of the spectral lines with the minimal distortions of their contours. Due to continuous improvements in spectrometers designs it is advised to perform adjustment according to manufacturers specifications. Following is the procedure, recommended by us, which helps to retain the original (manufacturer's) adjustment in the course of frequent primary electron energy changes.

Preserving the adjustment during primary electron energy changes

Changing of Ep in the wide energy range (a necessity in IS) (see note) frequently causes the deflection of the primary electron beam due to incomplete axial symmetry of the fields in the electron gun. In order to retain the adjustment, the allowed deflection from the analyzer’s focus must be substantially smaller than the focus itself and the effective beam diameter. Therefore, IS requires an arrangement to fix the beam direction, which corresponds to the initial adjustment.
Such an arrangement can be done with a Faradey cup (FC), with a diafragm in its screen, comparable in size with the effective beam diameter. The FC is mounted on the sample holder, in a way to allow its positioning in the analyzer's focus. The screen of FC (see note) is electrically connected with the holder and the FC electrode is guided outside of the chamber by a separate vacuum electrical feedthrough.

Before changing the Ep:

  • FC screen is grounded;
  • The FC is positioned by manipulator, so that the primary electron beam is targeted into the screen's diaphragm;
  • The sample holder is manipulated to reach the maximum of electric current on the FC electrode;
  • The holder's position is fixed.
  • After changing the Ep:

  • The electron beam is focused;
  • The electron beam is targeted into the diafragm of the FC screen by means of deflection plates electrodes;
  • By deflecting the beam a maximum current is reached on the FC electrode.

  • After the above described procedure the adjustment is preserved. Practice has proved that with a stable holder's construction and current maximum precision up to 2nd - 3rd decimal digit it is possible to perform multiple changes of Ep without loosing the initial adjustment.

    Look further: 5. SPECTROMETER CALIBRATION

    "Handbook of Ionization Spectra"
    ISBN 966-02-1954-7
    © T. Afanasieva, I. Koval,V. Lysenko, P. Mel'nik, N. Nakhodkin, M. Pyatnitsky
    Ukrainian National Academy of Science, Ukrainian Ministry of Education and Science
    Taras Schevchenko University, Radiophysical department
    tel.: +38(044)526-05-60
    e-mail: afanasieva@univ.kiev.ua