quantum-thermodynamics

Layer 1 — Physics24 concepts in this subtree

Thermodynamic laws and transformations for single or few quantum systems. Foundational: Jarzynski 1997 equality ⟨e^(-βW)⟩ = e^(-βΔF) — free-energy differences recoverable from non-equilibrium work distributions; Crooks 1999 fluctuation…

Jarzynski 1997: ⟨exp(-βW)⟩ = exp(-βΔF) — non-equilibrium avg recovers equilibrium ΔF
Crooks 1999: P_F(W)/P_R(-W) = exp(β(W - ΔF)) — forward/reverse work-PDF ratio
Quantum Otto cycle: 2 adiabatic + 2 isochoric — frequency-change expansion/compression
Gaussian-work limit: ⟨W⟩ = ΔF + β σ_W²/2 (cumulant identity)
Crooks ratio: [P_F(W)/P_R(-W)]·exp(-β(W-ΔF)) = 1 — identity along entire W axis
Otto efficiency: η = 1 − ω_c/ω_h for harmonic-oscillator quantum substrate
Landauer erasure: Delta-Q >= k_B*T*log(2) per erased bit via Shannon-McMillan-Breiman AEP
Jarzynski-via-Jensen second-law corollary: <W> >= dF (Jensen on convex exp(-x))
Thermodynamic uncertainty relation (TUR): Var(J)/<J>^2 >= 2*k_B/<Sigma> via large-deviations
Landauer bound Q_min = k_B*T*log(2); at T = 300 K, Q_min ~ 2.87e-21 J/bit
Jarzynski-Jensen: exp(-beta*<W>) <= <exp(-beta*W)> = exp(-beta*dF); hence <W> >= dF
TUR saturation at minimal dissipation: Var(J) = 2*k_B*<J>^2/<Sigma>; ratio = 2*k_B/<Sigma>
Jarzynski (quantum)
Crooks (1999)
Landauer principle (1961)
Quantum Otto cycle
Third law (quantum)
ETH + thermalization
Scovil-Schulz-DuBois (1959)
Kosloff (1984)
Jarzynski (1997)
Crooks fluctuation (1999)
Landauer bound (1961)
Maxwell demon (Szilárd 1929)
Explore the quantum-thermodynamics subtree on the interactive graph →