A Unified Theory of the Nucleus (Clustering Phenomena in Nuclei) (German Edition)
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Science, A Unified Theory of the Nucleus, 1. Introduction.- 1.1. General Remarks.- 1.2. Difficulties of Some Reaction Theories.- 2. Reformulation of the Schrdinger Equation.- 3. Discussion of the Basis Wave Functions for Nuclear Systems.- 3.1. General Remarks.- 3.2. Qualitative Discussion of Cluster Correlations.- 3.3. Construction of Oscillator Cluster Wave Functions.- 3.4. Discussion of 8Be as an Illustrative Example.- 3.5. Effects of Antisymmetrization.- 3.5a. Fermions without Mutual Interaction in a Square-Well Potential.- 3.5b. The Lowest 4+ ?-Cluster State of 8Be.- 3.5c. Mathematical Equivalence of the Lowest 6Li States Described in the t + 3He and the d + ? Oscillator Cluster Representations.- 3.5d. Summary.- 3.6. Applications of Oscillator Cluster Representations to a Qualitative Description of Low-Lying Levels in Light Nuclei.- 3.6a. 7Liand7Be.- 3.6b. 6He, 6Li, and 6Be.- 3.6c. ?-Cluster States of 16O.- 3.6d. Brief Remarks.- 3.7. Construction of Generalized Cluster Wave Functions.- 3.7a. Introduction of Jacobi Coordinates.- 3.7b. Introduction of Parameter Coordinates.- 3.7c. Introduction of Jastrow Factors.- 3.7d. Summary.- 4. Formulation of a Unified Microscopic Nuclear Structure and Reaction Theory.- 4.1. General Remarks.- 4.2. Specific Examples.- 4.2a. n + ? Scattering.- 4.2b. d + ? Scattering.- 4.2c. Discussion.- 4.3. Extension to General Systems.- 5. Bound-State Calculations.- 5.1. General Remarks.- 5.2. Calculation of Matrix Elements.- 5.2a. Evaluation of Matrix Elements by the Cluster-Coordinate Technique Example of 8Be.- 5.2b. Evaluation of Matrix Elements by the Generator-Coordinate Technique Example of 8Be.- 5.3. Ground and Low Excited States of 6Li.- 5.3a. Introduction.- 5.3b. Calculation With a Nucleon-Nucleon Potential Containing a Hard Core Accurate Treatment of the Jastrow Factor.- 5.3c. Calculation with a Nucleon-Nucleon Potential Containing a Soft Core Approximate Treatment of the Jastrow Factor.- 5.3d. Calculation with a Nucleon-Nucleon Potential Containing no Repulsive Core.- 5.3e. Summary.- 5.4. Low-Energy T = 0 States of 12C.- 5.5. Low-Lying Levels of 7Be.- 5.6. Concluding Remarks.- 6. Further Comments About the Pauli Principle.- 6.1. General Remarks.- 6.2. Cluster Overlapping and Pauli Principle.- 6.3. Energetical Favouring of a Cluster Inside a Large Nucleus.- 7. Scattering and Reaction Calculations.- 7.1. General Remarks.- 7.2. Derivation of Coupled Equations.- 7.2a. Single-Channel Problem.- 7.2b. Coupled-Channel Problem.- 7.2c. Reaction Calculations Using Hulthn-Kohn-Type Variational Functions.- 7.3. Quantitative Results.- 7.3a. 3He + ? Elastic Scattering.- 7.3b. l = 0 Phase-Shift in ? + ? scattering.- 7.3c. Specific Distortion Effects in d + ? Scattering.- 7.3d. Effect of Reaction Channels on 3He + 3He Scattering Cross Sections.- 7.3e. ? + 16O Scattering Utilization of the Generator-Coordinate Technique.- 7.3f. p + ? Scattering Around 3/2+ Resonance Level in 5Li.- 7.3g. ? + ? Scattering with Specific Distortion Effect and a Nucleon-Nucleon Pot, eBook.

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