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Thermo Quantum Dynamics in the Thermodynamic Limit $(\rm{N} \rightarrow \infty)$ (Trends in Infinite Dimensional Analysis and Quantum Probability)

Masuo Suzuki

Published Aug 1, 2002• 0 citations
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Thermo Quantum Dynamics in the Thermodynamic Limit (N→∞)(\rm{N} \rightarrow \infty)(N→∞) (Trends in Infinite Dimensional Analysis and Quantum Probability)
Thermo Quantum Dynamics in the Thermodynamic Limit (N→∞)(\rm{N} \rightarrow \infty)(N→∞) (Trends in Infinite Dimensional Analysis and Quantum Probability)
Most of the mathematical approaches for quantum Langevin equation are based on the noncommutativity of the random force operators.Non-commutative random force operators are introduced in order to guarantee that the equal-time commutation relation for the stochastic anlihilation and creation operators preserves in time.If it is true, it means that the origin of dissipation is of quantum mechanical.However, physically, it is hard to believe it.By making use of the unified canonical operator formalism for the system of the quantum stochastic differential equations within Non-Equilibri um Thermo Field Dynamics, it is shown that it is not true in general.