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Improving the Cramér-Rao bound with the detailed fluctuation theorem
1Unidade de Educação a Distância e Tecnologia, Universidade Federal Rural de Pernambuco, 52171-900 Recife, Pernambuco, Brazil.
This study derives a tighter upper bound for mean entropy production rates in nonequilibrium systems using the detailed fluctuation theorem (DFT). This new bound improves upon the Cramér-Rao (CR) bound and accurately approximates entropy production in heat exchange models.
Area of Science:
- Statistical Mechanics
- Non-equilibrium Thermodynamics
- Quantum Information Theory
Background:
- Entropy production is a key indicator of irreversibility in thermodynamic systems.
- The detailed fluctuation theorem (DFT) describes the statistical properties of entropy production.
- The Cramér-Rao (CR) bound provides a general limit on the precision of parameter estimation, including entropy production rates.
Purpose of the Study:
- To derive a novel upper bound for the mean entropy production rate.
- To improve upon the existing Cramér-Rao (CR) bound using the detailed fluctuation theorem (DFT).
- To validate the new bound's accuracy and saturation in specific physical systems.
Main Methods:
- Employing the detailed fluctuation theorem (DFT) to establish a new theoretical bound.
- Analyzing the time-dependent distribution of entropy production (Σ).
- Investigating heat exchange problems mediated by bosonic modes and qubits.
Main Results:
- A new upper bound for the mean entropy production rate was derived, surpassing the CR bound.
- The derived bound serves as an accurate approximation for entropy production in heat exchange via bosonic modes.
- The bound is shown to be saturated in heat exchange mediated by a weakly coupled qubit.
Conclusions:
- The detailed fluctuation theorem (DFT) offers a powerful tool for refining bounds on thermodynamic quantities.
- The newly derived bound provides a more precise estimation of entropy production rates in non-equilibrium systems.
- This work has implications for understanding and quantifying irreversibility in quantum and thermal processes.
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