Quantum thermodynamics is the study of thermodynamic processes and laws in quantum mechanical systems.Quantum thermodynamics extends classical thermodynamics to systems where quantum effects dominate: discrete energy levels, coherence (synchronization of wave functions), and entanglement. Individual quantum systems (electron, photon, molecule) can exhibit fluctuations of work and heat comparable to average values, and temporarily violate the second law of thermodynamics (law of entropy increase). However, for large ensembles or long time intervals, statistical regularities are restored. Central concepts include quantum fluctuation theorems linking forward and reverse processes, and generalization of entropy through the density matrix (description of quantum state).
Thermodynamics as a phenomenological science emerged in the 19th century thanks to the works of Sadi Carnot, Rudolf Clausius, and Lord Kelvin. Statistical justification was provided by Ludwig Boltzmann, linking entropy to the number of microstates (formula S = k log W). The quantum era required a revision of these ideas, starting with the work of von Neumann, who introduced the entropy S(ρ) = −Tr(ρ ln ρ) and showed its role in measurement. In the 1950s, the development of the theory of open quantum systems and lasers stimulated interest in the thermodynamics of small systems. The field acquired its modern form in the 1990s–2000s after the proof of fluctuation theorems (Jarzynski, Crooks) and their quantum generalizations. Today, quantum thermodynamics is actively developing in the context of quantum computing and nanotechnology.
Quantum thermodynamics is based on the description of a system through the density matrix ρ, which generalizes the classical probability distribution. The equilibrium state is given by the Gibbs distribution: ρ_eq = e^{-βH} / Z, where Z = Tr(e^{-βH}) is the partition function, β = 1/(k_B T). Entropy is given by the von Neumann entropy S_vN = −k_B Tr(ρ ln ρ). Work and heat are defined as changes in the internal energy U = Tr(ρH) with the separation of contributions from changes in the Hamiltonian H (work) and from changes in the density matrix (heat). In non-equilibrium processes, the quantum fluctuation theorem applies: the probability of obtaining work W in the forward process and −W in the reverse are related by P_f(W)/P_r(−W) = e^{β(W−ΔF)}. This expresses the universality of fluctuations and allows testing the laws of thermodynamics at the level of single quantum transitions. Additionally, quantum correlations (entanglement) can enhance the efficiency of heat engines by using non-classical states of the working body.
Used in the design of quantum engines and nanorefrigerators, as well as for understanding energy exchange in quantum computers.
In quantum thermodynamics, one can create a "quantum Maxwell's demon" — a device using quantum information to extract work from a system, seemingly violating the second law. But, as theorems have shown, the cost of acquiring and erasing information compensates for the gain, preserving overall entropy.












