KURIYAMA Atsushi | Faculty of Engineering, Kansai University

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概要

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著作論文

An Orthogonal Set Constituted by Eight Kinds of Boson Operators
A Note on a Boson Realization in Many-Boson System
On the Coupling of Two su(1, 1)Spins in the Holstein-Primakoff Type Boson Representation
On Parametric Resonance in Quantum Many-Body System : Collective Motion and Quantum Fluctuation around It in Coupled Lipkin Model(Nuclear Physics)
Deformed Boson Scheme Stressing Even-Odd Boson Number Difference. III : Parameter-Dependent Deformation
Deformed Boson Scheme Stressing Even-Odd Boson Number Difference. II : Unified Forms of Boson-Pair Coherent States in Even- and Odd-Boson Systems(Nuclear Physics)
Note on the Orthogonal Set in Six Kinds of Boson Operators : In Relation to the su (1,1)-and Its Relevant Algebras
On the Random Phase Approximation Based on the Thermo Field Dynamics Formalism : Nuclear Physics
A Note on Classical Orbits, Collective Submanifold and Quantal Collective Subspace : Progress Letters
Specification of Collective Submanifold by Adiabatic Time-Dependent Hartree-Fock Method : Coupled Lipkin Model
Generalized Center of Mass and Relative Motions in Classical Many-Body System : An Example of Solutions of Equations of Collective Submanifold : Nuclear Physics
Unique Specification of Collective Submanifold : Nuclear Physics
Quasi-Spin Squeezed State for Lipkin Model : Nuclear Physics
Time-Dependent Hartree-Fock Method and Its Extension
Equation of Collective Submanifold for Mixed States : Condensed Matter and Statistical Physics
A Boson System Interacting with an External Harmonic Oscillator : The su(1,1)-Spin Like Behavior in the su(2)-Spin System : Nuclear Physics
Three Forms of Coherent States in the su(2)-Spin System and Related Classical Counterparts : Nuclear Physics
Coherent State Combined with Mixed State for an Imperfect Boson System II : Static Solution and Elementary Excitation(Nuclear Physics)
Coherent State Combined with Mixed State for an Imperfect Boson System I : Thermalization of Pure Squeezed Coherent State(Nuclear Physics)
Imperfect Bose System and Its Mixed State Representation. II : Numerical Analysis with a Short-Range Replusive Force(Nuclear Physics)
Imperfect Bose System and Its Mixed State Representation. II : Numerical Analysis with a Short-Range Replusive Force
Deformed Boson Scheme Stressing Even-Odd Boson Number Difference. I : Various Forms of Boson-Pair Coherent State(Nuclear Physics)
Deformed Boson Scheme Stressing Even-Odd Boson Number Difference. I : Various Forms of Boson-Pair Coherent State
Note on the Orthogonal Set in Six Kinds of Boson Operators : In Relation to the su(1,1)- and Its Relevant Algebras
A Possible Form of the Orthogonal Set in Six Kinds of Boson Operators : In Relation to the su(2)- and Its Relevant Algebras
On the Boson Number Operator in the Deformed Boson Scheme
The su(1,1)-Algebraic Boson Model in the Deformed Boson Scheme : The Second Holstein-Primakoff Representation as q-Deformed Boson Operator(Nuclear Physics)
The su (1, 1)-Algebraic Boson Model in the Deformed Boson Scheme : The Second Holstein-Primakoff Representation as q-Deformed Boson Operator
Note on the Deformed Boson Scheme in Four Kinds of Boson Operators
Even-Odd Effect on the Thermal Equilibrium State of the Pairing Model. II : Mean Field Approximation and Renormalized Distribution
Even-Odd Effect on the Thermal Equilibrium State of the Pairing Model. I : Comparison between Canonical and Grand Canonical Ensembles
Deformed Boson Scheme including Conventional q-Deformation in Time-Dependent Variational Method. IV : The su(2)_q-and the su(1, 1)_q-Algebras in Four Kinds of Boson Operators
Two Contrastive Boson-Pair Coherent States in Deformed Boson Scheme
On the Multiboson Coherent State in Deformed Boson Scheme
Note on the Deformed Boson Scheme in Time-Dependent Variational Method
Deformed Boson Scheme including Conventional q-Deformation in Time-Dependent Variational Method. III : Deformation of the su(2,1)-Algebra in Terms of Three Kinds of Boson Operators
Deformed Boson Scheme including Conventional q-Deformation in Time-Dependent Variational Method.II : Deformation of the su(2)- and the su(1, 1)-Algebras in the Schwinger Boson Representation
Deformed Boson Scheme including Conventional q-Deformation in Time-Dependent Variational Method.I : The Case of Many-Body Systems Consisting of One Kind of Boson Operator
Pairing Model and Mixed State Representation. II : Grand Partition Function and Its Mean Field Approximation

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