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Breakdown of the Wiedemann-Franz law in a unitary Fermi gas.


ABSTRACT: We report on coupled heat and particle transport measurements through a quantum point contact (QPC) connecting two reservoirs of resonantly interacting, finite temperature Fermi gases. After heating one of them, we observe a particle current flowing from cold to hot. We monitor the temperature evolution of the reservoirs and find that the system evolves after an initial response into a nonequilibrium steady state with finite temperature and chemical potential differences across the QPC. In this state any relaxation in the form of heat and particle currents vanishes. From our measurements we extract the transport coefficients of the QPC and deduce a Lorenz number violating the Wiedemann-Franz law by one order of magnitude, a characteristic persisting even for a wide contact. In contrast, the Seebeck coefficient takes a value close to that expected for a noninteracting Fermi gas and shows a smooth decrease as the atom density close to the QPC is increased beyond the superfluid transition. Our work represents a fermionic analog of the fountain effect observed with superfluid helium and poses challenges for microscopic modeling of the finite temperature dynamics of the unitary Fermi gas.

SUBMITTER: Husmann D 

PROVIDER: S-EPMC6112745 | biostudies-literature | 2018 Aug

REPOSITORIES: biostudies-literature

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Breakdown of the Wiedemann-Franz law in a unitary Fermi gas.

Husmann Dominik D   Lebrat Martin M   Häusler Samuel S   Brantut Jean-Philippe JP   Corman Laura L   Esslinger Tilman T  

Proceedings of the National Academy of Sciences of the United States of America 20180809 34


We report on coupled heat and particle transport measurements through a quantum point contact (QPC) connecting two reservoirs of resonantly interacting, finite temperature Fermi gases. After heating one of them, we observe a particle current flowing from cold to hot. We monitor the temperature evolution of the reservoirs and find that the system evolves after an initial response into a nonequilibrium steady state with finite temperature and chemical potential differences across the QPC. In this  ...[more]

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