Amplification of Quantum Meson Modes in the Late Time of the Chiral Phase Transition(Nuclear Physics)
スポンサーリンク
概要
- 論文の詳細を見る
It is shown that there exists a possibility for the amplification of amplitudes of quantum pion modes with low momenta in the late time of the chiral phase transition by using the Gaussian wave functional approximation in the O(4) linear sigma model. It is also shown that amplification occurs in the mechanism of the resonance through forced oscillation as well as parametric resonance induced by the small oscillation of the chiral condensate. These mechanisms are investigated in both the cases of a spatially homogeneous system and a spatially expanded system described by the Bjorken coordinate.
- 理論物理学刊行会の論文
- 2005-02-25
著者
-
TSUE Yasuhiko
Physics Division, Faculty of Science, Kochi University
-
Nishiyama Seiya
Physics Division Faculty Of Science Kochi University
-
Tsue Yasuhiko
Physics Division Faculty Of Science Kochi University
-
Watanabe Kazu
Department Of Applied Science Kochi University:(present Address)kochi Gakuen Kochi Junior High Schoo
-
TSUE Yasuhiko
Department of Physics, Kyoto University
-
WATANABE Kazu
Department of Applied Science, Kochi University:(Present address)Kochi Gakuen Kochi Junior High School
関連論文
- First-Order Quark-Hadron Phase-Transition in a NJL-Type Model for Nuclear and Quark Matter : The Case of Symmetric Nuclear Matter(Nuclear Physics)
- A Refined Numerical Result on the First Excitation Energy in the Two-Level Pairing Model(Nuclear Physics)
- Classical and Quantal Descriptions of Small Amplitude Fluctuations around Equilibriums in the Two-Level Pairing Model(Nuclear Physics)
- The Lipkin Model in Many-Fermion System as an Example of the su(1, 1) ⊗ su(1, 1)-Algebraic Model(Nuclear Physics)
- A Note on the Two-Level Pairing Model Obeying the su (2) ⊗ su (2)-Algebra : Re-formation in Terms of the su (1, 1) ⊗ su (1, 1)-Algebra(Nuclear Physics)
- A New Boson Realization of the Two-Level Pairing Model in a Many-Fermion System and Its Classical Counterpart : The Role of the su (2) ⊗ su (1, 1)-Coherent State in the Schwinger Boson Representation for the su (2) ⊗ su (2)-Algebra(Nuclear P
- Note on Many-Quark Model with su(4) Algebraic Structure(Nuclear Physics)
- On the Exact Eigenstates and the Ground States Based on the Boson Realization for Many-Quark Model with su(4) Algebraic Structure(Nuclear Physics)
- Many-Quark Model with su(4) Algebraic Structure : An Example of Analytically Soluble Many-Fermion System(Nuclear Physics)
- Semi-Classical Approach to the Two-Level Pairing Model : Various Aspects of Phase Change(Nuclear Physics)
- Boson Realization of the su (3)-Algebra. IV : Holstein-Primakoff Representation for the Elliott Model (Nuclear Physics)
- Boson Realization of the su (3)-Algebra. III : Schwinger Representation for the Elliott Model (Nuclear Physics)
- Boson Realization of the su(3)-Algebra. II : Holstein-Primakoff Representation for the Lipkin Model(Nuclear Physics)
- Boson Realization of the su(3)-Algebra. I : Schwinger Representation for the Lipkin Model(Nuclear Physics)
- The Lipkin Model in the su(M+1)-Algebra for Many-Fermion System and Its Counterpart in the Schwinger Boson Representation(Nuclear Physics)
- A Possible Boson Realization of the so(4)-and the so(3, 1)-Algebra : In Relation to the Runge-Lenz-Pauli Vector(Nuclear Physics)
- A Note on the Eigenvalue Problem in the su(1, 1)-Algebra(Nuclear Physics)
- On the Eigenvalue Problem of the su(1,1)-Algebra and the Coupling Scheme of Two su(1,1)-Spins(Nuclear Physics)
- Coupling Schemes for an n su(2) Spin System(Nuclear Physics)
- 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
- Fermionic Squeezed State for the O(4) Model as a Schematic Model in a Many-Fermion System(Nuclear Physics)
- A Possible Extension of a Trial State in the TDHF Theory with a Canonical Form to the Lipkin Model : Canonicity Conditions and Dynamical Treatment of Classical and Quantal Variables in an Extended State of the su(2)-Coherent State(Nuclear Physics)
- Time-Evolution of a Collective Meson Field by Use of a Squeezed State
- Amplification of Quantum Meson Modes in the Late Time of the Chiral Phase Transition(Nuclear Physics)
- Variational Approach to the Chiral Phase Transition in the Linear Sigma Model
- Time-Dependent Variational Approach to the Non-Abelian Pure Gauge Theory : Its Application to Evaluation of the Shear Viscosity of Quantum Gluonic Matter(Nuclear Physics)
- Effective Potential Study of the Chiral Phase Transition in a QCD-Like Theory(Nuclear Physics)
- 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
- 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
- Utility of su(1,1)-Algebra in a Schematic Nuclear su(2)-Model
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. III : Transition from the Quark-Triplet to the Quark-Pair Phase(Nuclear Physics)
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. II : Determination of Ground-State Energies(Nuclear Physics)
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. I : Color-Symmetric Form(Nuclear Physics)
- 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
- Note on the Minimum Weight States in the su(2)-Algebraic Many-Fermion Model : Extension of the Role of the Auxiliary su(2)-Algebra(Nuclear Physics)
- Background of the su(2)-Algebraic Many-Fermion Models in the Boson Realization : Construction of Minimum Weight States by Means of an Auxiliary su(2)-Algebra and Its Related Problems(Nuclear Physics)
- Color-Singlet Three-Quark States in the su(4)-Algebraic Many-Quark Model : An Example of the su(4) ⨂ su(4)-Model(Nuclear Physics)
- Re-Formation of Many-Quark Model with the su(4)-Algebraic Structure in the Schwinger Boson Realization : Reconsideration in the Original Fermion Space(Nuclear Physics)
- Scalar and Pseudoscalar Glueball Masses within a Gaussian Wavefunctional Approximation(Nuclear Physics)
- Color-Singlet Three-Quark States in the su(4)-Algebraic Many-Quark Model : An Example of the su(4)⊗su(4)-Model
- Re-Formation of Many-Quark Model with the su(4)-Algebraic Structure in the Schwinger Boson Realization : Reconsideration in the Original Fermion Space
- Effective Potential Approach to Quark Ferromagnetization in High Density Quark Matter(Nuclear Physics)
- The BCS-Bogoliubov and the su(2)-Algebraic Approach to the Pairing Model in Many-Fermion System : The Quasiparticle in the Conservation of the Fermion Number(Nuclear Physics)
- A Role of the Quasiparticle in the Conservation of the Fermion Number : An Example Illustrative of the Deformation of the Cooper Pair(Nuclear Physics)
- Note on the Minimum Weight States in the su(2)-Algebraic Many-Fermion Model : Extension of the Role of the Auxiliary su(2)-Algebra
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. I : Color-Symmetric Form
- Background of the su(2)-Algebraic Many-Fermion Models in the Boson Realization : Construction of Minimum Weight States by Means of an Auxiliary su(2)-Algebra and Its Related Problems
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. III : Transition from the Quark-Triplet to the Quark-Pair Phase
- On the Color-Singlet States in Many-Quark Model with the su(4)-Algebraic Structure. II : Determination of Ground-State Energies
- First-Order Quark-Hadron Phase-Transition in a NJL-Type Model for Nuclear and Quark Matter : The Case of Symmetric Nuclear Matter
- On the Exact Eigenstates and the Ground States Based on the Boson Realization for Many-Quark Model with su(4) Algebraic Structure
- Note on Many-Quark Model with su(4) Algebraic Structure
- Many-Quark Model with su(4) Algebraic Structure : An Example of Analytically Soluble Many-Fermion System
- A Refined Numerical Result on the First Excitation Energy in the Two-Level Pairing Model
- Classical and Quantal Descriptions of Small Amplitude Fluctuations around Equilibriums in the Two-Level Pairing Model
- Semi-Classical Approach to the Two-Level Pairing Model : Various Aspects of Phase Change
- The Lipkin Model in Many-Fermion System as an Example of the su(1,1)〓su(1,1)-Algebraic Model
- A Note on the Two-Level Pairing Model Obeying the su(2)〓su(2)-Algebra--Re-Formation in Terms of the su(1,1)〓su(1,1)-Algebra
- A New Boson Realization of the Two-Level Pairing Model in a Many-Fermion System and Its Cassical Counterpart--The Role of the su(2)〓su(1,1)-Coherent State in the Schwinger Boson Representation for the su(2)〓su(2)-Algebra
- Boson Realization of the su(3)-Algebra. IV : Holstein-Primakoff Representation for the Elliott Model
- Boson Realization of the su(3)-Algebra. III : Schwinger Representation for the Elliott Model
- The Lipkin Model in the su(M+1)-Algebra for Many-Fermion System and Its Counterpart in the Schwinger Boson Representation(Nuclear Physics)
- Coupling Schemes for an n su(2) Spin System(Nuclear Physics)
- A Note on the Eigenvalue Problem in the su(1, 1)-Algebra(Nuclear Physics)
- A Possible Boson Realization of the so(4)-and the so(3, 1)-Algebra : In Relation to the Runge-Lenz-Pauli Vector(Nuclear Physics)
- A Possible Extension of a Trial State in the TDHF Theory with a Canonical Form to the Lipkin Model : Canonicity Conditions and Dynamical Treatment of Classical and Quantal Variables in an Extended State of the su(2)-Coherent State(Nuclear Physics)
- Fermionic Squeezed State for the O(4) Model as a Schematic Model in a Many-Fermion System(Nuclear Physics)
- Time-Dependent Variational Approach to the Non-Abelian Pure Gauge Theory : Its Application to Evaluation of the Shear Viscosity of Quantum Gluonic Matter
- Amplification of Quantum Meson Modes in the Late Time of the Chiral Phase Transition(Nuclear Physics)
- On the Eigenvalue Problem of the su(1,1)-Algebra and the Coupling Scheme of Two su(1,1)-Spins(Nuclear Physics)
- The BCS-Bogoliubov and the su (2)-Algebraic Approach to the Pairing Model in Many-Fermion System : The Quasiparticle in the Conservation of the Fermion Number
- A Role of the Quasiparticle in the Conservation of the Fermion Number : An Example Illustrative of the Deformation of the Cooper Pair