Correspondence Between the Energy Equipartition Theorem in Classical Mechanics and its Phase-Space Formulation in Quantum Mechanics
arXiv:2205.12364 · doi:10.3390/e25060939
Abstract
In classical physics there is a well-known theorem in which it is established that the energy per degree of freedom is the same. However, in quantum mechanics due to the non-commutativity of some pairs of observables and the possibility of having non-Markovian dynamics, the energy is not equally distributed. We propose a correspondence between what we know about the classical energy equipartition theorem and its possible counterpart in phase-space formulation in quantum mechanics based on the Wigner representation. Also, we show that in the high-temperature regime, the classical result is recovered.
References in corpus (4)
- Overview of the phase space formulation of quantum mechanics with application to quantum technologies
- Nonclassical phase-space trajectories for the damped harmonic quantum oscillator
- Quantum counterpart of energy equipartition theorem for fermionic systems
- Weyl-Wigner Representation of Canonical Equilibrium States