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《光电子光谱学:原理和应用(第3版)内容为：Since the completion of the manuscript for the first edition of PhotoelectronSpectroscopy, the field has undergone a steady growth.Firstly, the theory has been refined and condensed into a manageableform. Secondly two important experimental developments have occurred. Theresolution that can be obtained is now of the order of 3 meV, which corre-sponds approximately to an energy of 30 kBK. This means that photoelectronspectroscopy can now obtain data with an accuracy similar to that achievedin standard thermodynamic experiments （such as specific heat experiments）,thus facilitating a direct comparison of data from the two different types ofexperiment. The second important experimental advance is that one can nowreadily measure electron energy distributions over a solid angle of almost This yields valuable information whenever these electron energy distributionshave anisotropies.

1. Introduction and Basic Principles

　1.1 Historical Development

　1.2 The Electron Mean Free Path

　1.3 Photoelectron Spectroscopy and Inverse Photoelectron Spectroscopy

　1.4 Experimental Aspects

　1.5 Very High Resolution

　1.6 The Theory of Photoemission

　　1.6.1 Core-Level Photoemission

　　1.6.2 Valence-State Photoemission

　　1.6.3 Three-Step and One-Step Considerations

　1.7 Deviations from the Simple Theory of Photoemission

　References

2. Core Levels and Final States

　2.1 Core-Level Binding Energies in Atoms and Molecules

　　2.1.1 The Equivalent-Core Approximation

　　2.1.2 Chemical Shifts

　2.2 Core-Level Binding Energies in Solids

　　2.2.1 The Born-Haber Cycle in Insulators

　　2.2.2 Theory of Binding Energies

　　2.2.3 Determination of Binding Energies and Chemical Shifts from Thermodynamic Data

　2.3 Core Polarization

　2.4 Final-State Multiplets in Rare-Earth Valence Bands

　2.5 Vibrational Side Bands

　2.6 Core Levels of Adsorbed Molecules

　2.7 Quantitative Chemical Analysis from Core-Level Intensities

　References

3. Charge-Excitation Final States: Satellites

3.1 Copper Dihalides; 3d Transition Metal Compounds

　　3.1.1 Characterization of a Satellite

　　3.1.2 Analysis of Charge-Transfer Satellites

　　3.1.3 Non-local Screening

　 3.2 The 6-eV Satellite in Nickel

　　3.2.1 Resonance Photoemission

　　3.2.2 Satellites in Other Metals

　3.3 The Gunnarsson-Sch6nhammer Theory

　3.4 Photoemission Signals and Narrow Bands in Metals

　References

4. Continuous Satellites and Plasmon Satellites: XPS Photoemission in Nearly Free Electron Systems

　4.1 Theory

　　4.1.1 General

　　4.1.2 Core-Line Shape

　　4.1.3 Intrinsic Plasmons

　　4.1.4 Fxtrinsic FAectron Scattering: Plasmons and Background

　　411.5 The Total Photoelectron Spectrum

　4.2 Experimental Results

　　4.2.1 The Core Line Without Plasmons

　　4.2.2 Core-Level Spectra Including Plasmoas

　　4.2.3 Valence-Band Spectra of the Simple Metals

　　4.2.4 Simple Metals: A General Comment

　4.3 The Background Correction

　References

5. Valence Orbitals in Simple Molecules and Insulating Solids

　5.1 UPS Spectra of Monatomic Gases

　5.2 Photoelectron Spectra of Diatomic Molecules

　5.3 Binding Energy of the H2 Molecule

　5.4 Hydrides Isoelectronic with Noble Gases

　　Neon (Ne)

　　Hydrogen Fluoride (HF)

　　Water (H2O)

　　Ammonia (NH3)

　　Methane (CH4)

　5.5 Spectra of the Alkali HMides

　5.6 Transition Metal Dihalides

　5.7 Hydrocarbons

　　5.7.1 Guidelines for the Interpretation of Spectra from Free Molecules

　　5.7.2 Linear Polymers

5.8 Insulating Solids with Valence d Electrons

　　5.8.1 The NiO Problem

　　5.8.2 Mort Insulation

……

6. Photoemission of Valence Electrons from Metallic Solids in the One-Electron Approximation

7. Band Structure and Angular-Resolved Photoelectron Spectra

8. Surface States, Surface Effects

9. Inverse Photoelectron Spectroscopy

10. Spin-Polarized Photoelectron Spectroscopy

11. Photoelectron Diffraction

Appendix

Index

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书籍介绍

《光电子光谱学:原理和应用(第3版)内容为：Since the completion of the manuscript for the first edition of PhotoelectronSpectroscopy, the field has undergone a steady growth.Firstly, the theory has been refined and condensed into a manageableform. Secondly two important experimental developments have occurred. Theresolution that can be obtained is now of the order of 3 meV, which corre-sponds approximately to an energy of 30 kBK. This means that photoelectronspectroscopy can now obtain data with an accuracy similar to that achievedin standard thermodynamic experiments （such as specific heat experiments）,thus facilitating a direct comparison of data from the two different types ofexperiment. The second important experimental advance is that one can nowreadily measure electron energy distributions over a solid angle of almost This yields valuable information whenever these electron energy distributionshave anisotropies.