Nonequilibrium thermal machines under cyclic driving generally outperform steady-state counterparts. However, there is still lack of coherent understanding of versatile transport and fluctuation features under time modulations. Here, we formulate a theoretical framework of thermodynamic geometry in terms of full counting statistics of nonequilibrium driven transports. We find that, besides the conventional dynamic and adiabatic geometric curvature contributions, the generating function is divided into an additional nonadiabatic contribution, manifested as the metric term of full counting statistics. This nonadiabatic metric generalizes recent results of thermodynamic geometry in near-equilibrium entropy production to far-from-equilibrium fl...
An inherent feature of small systems in contact with thermal reservoirs, be it a pollen grain in wat...
Small nonequilibrium systems in contact with a heat bath can be analyzed with the framework of stoch...
Dealing with a generic time-local non-Markovian master equation, we define current and power to be p...
In contrast to the classical concept of a Carnot engine that alternates contact between heat baths o...
In the quest for high-performance quantum thermal machines, looking for an optimal thermodynamic eff...
We propose a geometric theory of non-equilibrium thermodynamics, namely geometric thermodynamics, us...
Fluctuations strongly affect the dynamics and functionality of nanoscale thermal machines. Recent de...
Understanding heat transfer between a quantum system and its environment is of undisputed importance...
Molecular complexes with movable components form the basis of nanoscale machines. Their inherent sto...
We consider a generic four-stroke quantum Otto engine consisting of two unitary and two thermalizati...
The trade-off between large power output, high efficiency and small fluctuations in the operation of...
Thermodynamic uncertainty relations (TURs) represent one of the few broad-based and fundamental rela...
Entropy production is the key to the second law of thermodynamics, and it is well defined by conside...
Counterdiabatic driving (CD) exploits auxiliary control fields to tailor the nonequilibrium dynamics...
Stochastic thermodynamics has revolutionized our understanding of heat engines operating in finite t...
An inherent feature of small systems in contact with thermal reservoirs, be it a pollen grain in wat...
Small nonequilibrium systems in contact with a heat bath can be analyzed with the framework of stoch...
Dealing with a generic time-local non-Markovian master equation, we define current and power to be p...
In contrast to the classical concept of a Carnot engine that alternates contact between heat baths o...
In the quest for high-performance quantum thermal machines, looking for an optimal thermodynamic eff...
We propose a geometric theory of non-equilibrium thermodynamics, namely geometric thermodynamics, us...
Fluctuations strongly affect the dynamics and functionality of nanoscale thermal machines. Recent de...
Understanding heat transfer between a quantum system and its environment is of undisputed importance...
Molecular complexes with movable components form the basis of nanoscale machines. Their inherent sto...
We consider a generic four-stroke quantum Otto engine consisting of two unitary and two thermalizati...
The trade-off between large power output, high efficiency and small fluctuations in the operation of...
Thermodynamic uncertainty relations (TURs) represent one of the few broad-based and fundamental rela...
Entropy production is the key to the second law of thermodynamics, and it is well defined by conside...
Counterdiabatic driving (CD) exploits auxiliary control fields to tailor the nonequilibrium dynamics...
Stochastic thermodynamics has revolutionized our understanding of heat engines operating in finite t...
An inherent feature of small systems in contact with thermal reservoirs, be it a pollen grain in wat...
Small nonequilibrium systems in contact with a heat bath can be analyzed with the framework of stoch...
Dealing with a generic time-local non-Markovian master equation, we define current and power to be p...