Chapter V A Coupled Channel Variational Method for Microscopic Study of Reactions between Complex Nuclei
スポンサーリンク
概要
- 論文の詳細を見る
A precise generalization of the Kohn-Hulthen-Kato variational method for scattering matrix is made for the purpose of microscopic study of reactions between complex nuclei with many channels coupled. The framework is given by the resonating group method (RGM) both for two-cluster systems and for three-cluster systems. The scattering boundary condition is imposed on the trial functions of the dynamical coordinate space, while the required matrix elements between the RGM trial basis functions for the internal region are described in terms of the generator coordinate (GC) kernels and the corresponding GC trial basis functions. Detailed numerical tests are exhibited with showing very good accuracy and sufficiently short computational time in the result of the present method, which is encouraging enough to apply the method to coupled channel studies of various-kind reactions based both on the microscopic models and on certain phenomenological models.
- 理論物理学刊行会の論文
- 1978-05-31
著者
関連論文
- Big-Bang Nucleosynthesis Reactions Catalyzed by a Long-Lived Negatively Charged Leptonic Particle(Nuclear Physics)
- S=-2 Hypernuclear Structure(Chapter II.,Hypernuclei and Baryon-Baryon Interaction)
- S=-1 Hypernuclear Structure(Chapter II.,Hypernuclei and Baryon-Baryon Interaction)
- Three- and Four-Body Cluster Models of Hypernuclei Using the G-Matrix ΛN Interaction : ^9_ΛBe, ^_ΛC, ^6_He and ^_Be : Nuclear Physics
- ^6He+^6He Molecular States in Highly-Excited ^12Be
- ^6He+^6He Molecular States in Highly-Excited ^Be
- Capter V Microscopic Study of the Interaction between Complex Nuclei
- Chapter IV Coupled-Channels Approach to Deuteron and ^3He Breakup Reactions
- Chapter III Effects of Deuteron Virtual Breakup on Deuteron Elastic and Inelastic Scattering
- Chapter I Projectile Breakup Processes in Nuclear Reactions
- Coupled-Discretized-Continuum-Channels Method for Deuteron Breakup Reactions Based on Three-Body Model : Justification of the Method for Truncation and Discretization of the p-n Continuum
- Role of the Quark-Quark Correlation in Baryon Structure and Non-Leptonic Weak Transitions of Hyperons(Nuclear Physics)
- Four- and Five-Body Scattering Calculations of Exotic Hadron Systems(Pentaquarks and related topics, Exotic hadrons, New Frontiers in QCD-Exotic Hadrons and Hadronic Matter-)
- Capter II Comprehensive Study of Alpha-Nuclei
- Is Muon-Catalyzed d-^3He Fusion Possible?(Microscopic Cluster Models of Light Nuclei and Related Topics)
- On a Calculational Method of Folding Model Potential with Density-Dependent Effective Interactions : Progress Letters
- Alpha-Like Spatial Four-Body Correlations in Light Nuclei : Vertically-Truncated-Subspace Shell Model for the Core Plus Four-Particle System
- Chapter VI Microscopic Coupled-Channels Study of Scattering and Breakup of Light Heavy-Ions
- Elastic Scattering and Breakup of ^6Li : A New Type of Dynamical Polarization Potential
- Projectile Breakup Effect on ^6Li Elastic Scattering from ^Si and ^Ca Studied by Microscopic Coupled-Channels Method
- A Study of α-Widths of ^Ne Based on ^O and α-Cluster Model
- Chapter V A Coupled Channel Variational Method for Microscopic Study of Reactions between Complex Nuclei
- The Generator Coordinate Method for Composite-Particle Scattering Based on the Kohn-Hulthen Variational Principle : Application to α-α, ^O-^O scattering
- Electron-Scattering Form Factors and α-Clustering Structure of ^Ne
- Quantum Three-Body Calculation of the Nonresonant Triple-α Reaction Rate at Low Temperatures
- A Coupled Channel Variational Method for Multi-Step Direct Nuclear Reactions. II : Test on a (d,p) Reaction
- A Coupled Channel Variational Method for Multi-Step Direct Nuclear Reactions. I : Formalism and Numerical Test
- Chapter V Coupled-Channels Variational Method for Nuclear Breakup and Rearrangement Processes
- Study of the Alpha-Clustering Structure of ^Ne Based on the Resonating Group Method for ^O+α : Analysis of Alpha-Decay Widths and the Exchange Kernel
- S=-2 Hypernuclear Structure
- S=-1 Hypernuclear Structure