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

2. IONIZATION SPECTROSCOPY EQUIPMENT

2.2. Electron gun

The primary beam parameters (effective diameter, beam current ip and electron energy Ep) are substantially influencing the possibilities of the whole spectrometer. In particular, the minimal lateral dimensions of investigated areas of the sample are limited by the effective beam diameter. The majority of spectrometers operate with beam no larger than several micrometers.


The beam current ip limits the minimal beam diameter and determines the time t, required to record the IL with the given signal-to-noise ratio: . The electron guns of commercial AES spectrometers deliver ip = 0.1...1.0 microampers with accelerating voltage of Vp = 0.2...10.0 kV. This current is enough for recording of intensive ILs within the time of . It is desirable to increase the ip for decreasing of recording time and detection of less intensive ILs.


The primary electron energy Ep is of special importance in IS (paragraph 6.2). Usually in IS the Ep =200...1200 eV, which is substantially lower than standard values of Ep in commercial spectrometers. Lowering of Ep in commercial spectrometers decreases the beam current ip and increases its diameter above nominal value.


Look further: 3. IL DETECTION

"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