Fluctuation theorems: Work is not an observable
arXiv:cond-mat/0703189 · doi:10.1103/PhysRevE.75.050102
Abstract
The characteristic function of the work performed by an external time-dependent force on a Hamiltonian quantum system is identified with the time-ordered correlation function of the exponentiated system's Hamiltonian. A similar expression is obtained for the averaged exponential work which is related to the free energy difference of equilibrium systems by the Jarzynski work theorem.
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- Modelling mechanical equilibration processes of closed quantum systems: a case-study
- The Rabi problem with elliptic polarization
- A decoherence interpretation of quantum work for adiabatic processes
- A perspective on Lindblad's Non-Equilibrium Entropy
- Projection hypothesis in the setting for the quantum Jarzynski equality
- On the Quantum Jarzynski Identity
- Adiabatic Dynamics and Shortcuts to Adiabaticity: Fundamentals and Applications
- Full statistics of erasure processes: Isothermal adiabatic theory and a statistical Landauer principle
- Quantum advantage from negativity of a work quasiprobability distribution
- Quantum thermodynamics under continuous monitoring: a general framework
- Quantum Work Relations under Trial Hamiltonians
- Edge States Effects in Quantum Work Statistics
- Miniatures on Open Quantum Systems
- Work and heat exchanged during sudden quenches of strongly coupled quantum systems
- Information-acquiring von Neumann architecture of a computer: A theoretical design
- Calculation of semiclassical free energy differences along non-equilibrium classical trajectories
- Work Statistics and Quantum Trajectories: No-Click Limit and non-Hermitian Hamiltonians
- Enhancement of efficiency in the Dicke model quantum heat engine
- Informational work storage in quantum thermodynamics