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  • 1
    Online Resource
    Online Resource
    Milton :CRC Press LLC,
    Keywords: Atomic structure-Measurement-Data processing. ; Electronic books.
    Description / Table of Contents: Computational Atomic Structure: An MCHF Approach deals with the field of computational atomic structure, specifically with the multiconfiguration Hartree-Fock (MCHF) approach and the manner in which this approach is used in modern physics.
    Type of Medium: Online Resource
    Pages: 1 online resource (292 pages)
    Edition: 1st ed.
    ISBN: 9781351458924
    DDC: 539.14
    Language: English
    Note: Cover -- Half Title -- Title Page -- Copyright Page -- Table of Contents -- Preface -- Acknowledgments -- 1: Introduction -- 1.1 Introduction -- 1.2 Properties of the Wave Function -- 1.3 One-Electron Systems -- 1.4 Many-Electron Systems -- 1.5 The Variational Method -- 1.6 Summary -- 1.7 Exercises -- 2: Configuration State Functions and Matrix Elements of the Hamiltonian -- 2.1 Configuration State Functions -- 2.2 Matrix Elements of the Hamiltonian -- 2.3 Exercises -- 3: Hartree-Fock Calculations -- 3.1 The Hartree-Fock Approximation -- 3.2 The Hartree-Fock Equation for 1s 2p 3P -- 3.3 The Self-Consistent Field Procedure -- 3.4 Hartree-Fock Solutions for the Ground State of Lithium -- 3.5 The Hartree-Fock Solutions for 1s2s 3S and 1S States in He -- 3.6 The General Hartree-Fock Equations -- 3.7 Brillouin's Theorem -- 3.8 Term Dependence -- 3.9 Iso-Electronic Sequences and Orbital Collapse -- 3.10 Quantum Defects and Rydberg Series -- 3.11 Computational Aspects -- 3.12 Exercises -- 4: Multiconfiguration Hartree-Fock Wave Functions -- 4.1 Correlation in Many-Electron Atoms -- 4.2 Z-Dependent Perturbation Theory -- 4.3 Pair-Correlation Expansions -- 4.4 Complete and Restricted Active Spaces -- 4.5 The MCHF Approximation -- 4.6 a Non-Orthogonal Extension -- 4.7 MCHF Calculation for 3s2 3p 2P in AI -- 4.8 Properties of MCHF Wave Functions -- 4.9 Computational Aspects -- 4.10 Exercises -- 5: Two-Electron Systems -- 5.1 Non-Uniqueness of the Wave Function -- 5.2 The Reduced Form -- 5.3 Rydberg Series -- 5.4 Rydberg Series with Perturber -- 5.5 The GBT Method -- 5.6 Exercises -- 6: Correlation in Many-Electron Systems -- 6.1 Zero-Order Wave Functions -- 6.2 First-Order Wave Functions -- 6.3 Z-Dependence of Atomic Properties -- 6.4 Exercises -- 7: Relativistic Effects -- 7.1 Introduction -- 7.2 The Breit-Pauli Hamiltonian. , 7.3 Breit-Pauli Wave Functions -- 7.4 Fine-Structure Levels -- 7.5 Computational Aspects -- 7.6 Fine Structure in Helium -- 7.7 The Blume-Watson Approach -- 7.8 Systems with Two Valence Electrons -- 7.9 A Limited Model for Core-Valence Correlation -- 7.10 Exploring Complex Spectra -- 7.11 Z-Dependence of Relativistic Effects -- 7.12 Exercises -- 8: Isotope and Hyperfine Effects -- 8.1 The Effects of the Nucleus -- 8.2 Mass Shift -- 8.3 Field Shift -- 8.4 Level Isotope Shift -- 8.5 Transition Isotope Shift -- 8.6 Field Shift Correction for 3d8(3F)4p 4D5/2 in Ni II -- 8.7 Hyperfine Structure -- 8.8 Hyperfine Interaction -- 8.9 Angular Properties of the Hyperfine States -- 8.10 First-Order Hyperfine Energies -- 8.11 First-Order Wave Functions -- 8.12 Computational Aspects -- 8.13 Configuration Expansions for Hyperfine Structure -- 8.14 Polarization Effects -- 8.15 Exercises -- 9: Allowed and Forbidden Transitions -- 9.1 Introduction -- 9.2 Matrix Elements for Transition Operators -- 9.3 Selection Rules for Radiative Transitions -- 9.4 Computational Aspects -- 9.5 Allowed Transitions -- 9.6 LS Calculations for Allowed Transitions -- 9.7 Cancellations in the Transition Integral -- 9.8 Core-Valence Effects on Line Strength -- 9.9 Spin-Forbidden Transitions -- 9.10 Branching Ratios in Complex Spectra -- 9.11 Forbidden Lines -- 9.12 Hyperfine-Induced Transition -- 9.13 Z-Dependence of Transition Properties -- 9.14 Exercises -- 10: MCHF Continuum Wave Functions -- 10.1 Continuum Processes -- 10.2 Continuum Functions -- 10.3 Photoionization or Photodetachment -- 10.4 Autoionization -- 10.5 Computational Aspects -- 10.6 Exercises -- Appendices -- A: Angular Momentum Theory -- A.1 Angular Momentum Operators -- A.2 Coupling of Two Angular Momenta -- A.3 Coupling of Three and Four Angular Momenta -- A.4 Spherical Tensor Operators -- A.5 The Wigner-Eckart Theorem. , A.6 Matrix Elements of Tensor Operators Between Coupled Functions -- B: The Dirac and Breit-Pauli Theory -- B.1 Introduction -- B.2 Dirac Theory of One-Electron Systems -- B.3 The Relativistic Wave Equation for Many-Electron Systems -- C: Fundamental Constants -- C.1 Atomic Units -- C.2 Additional Units -- D: Program Input Parameters -- References -- Index.
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 83 (1998), S. 4206-4212 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: The Shockley–Read–Hall (SRH) carrier lifetime in electron-irradiated low-doped p-type silicon was measured at different injection levels and various temperatures. The lifetime under high-level injection was determined using the open-circuit carrier decay technique. The reverse recovery technique was used to determine the lifetime under low-level injection. The defect composition was studied using deep-level transient spectroscopy, and according to that the SRH lifetime is calculated. The good agreement between the calculated and the measured lifetimes strongly indicates that the lifetime is controlled by two different deep levels. At low injection levels, the lifetime is mainly controlled by the singly negative charge state of the divacancy center, HC−HT=0.421 eV, and at high injection levels by the vacancy–oxygen complex, HC−HT=0.164 eV. These are the same levels controlling the lifetime in electron-irradiated n-type silicon. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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