Quantum bounds on heat transport through nanojunctions
arXiv:1502.03095 · doi:10.1103/PhysRevLett.114.220401
Abstract
We derive rigorous quantum mechanical bounds for the heat current through a nanojunction connecting two thermal baths at different temperatures. Based on exact sum rules, these bounds compliment the well-known quantum of thermal conductance , which provides a bound for low-temperature heat transport in all systems, but is saturated only for noninteracting transport. In contrast, our bounds are saturated at high temperatures---but still in the quantum regime---, even when interactions are very strong. We evaluate these bounds for harmonic and strongly anharmonic junction models and compare with numerical approaches.
8 pages, 4 figures
References in corpus (16)
- Viscosity in Strongly Interacting Quantum Field Theories from Black Hole Physics
- Energy Dissipation and Transport in Nanoscale Devices
- Driven quantum transport on the nanoscale
- Theory of universal incoherent metallic transport
- Direct Measurement of Room Temperature Non-diffusive Thermal Transport Over Micron Distances in a Silicon Membrane
- Universal Quantum Viscosity in a Unitary Fermi Gas
- Quantum limit of heat flow across a single electronic channel
- Single-mode heat conduction by photons
- Nonequilibrium Green's function approach to mesoscopic thermal transport
- Optimal thermoelectric figure of merit of a molecular junction
- Heat transport in harmonic lattices
- Mesoscopic photon heat transistor
- Heat transfer in the spin-boson model: A comparative study in the incoherent tunneling regime
- Meir-Wingreen formula for heat transport in a spin-boson nanojunction model
- Lower bounds for the conductivities of correlated quantum systems
- Energy Dissipation and Fluctuation-Response in Driven Quantum Langevin Dynamics