In cooperation with researchers from Osaka City University and The University of Tokyo, researchers at Osaka University, through the highest level of precise measurement of current fluctuations in quantum liquids in artificial atoms created by fine processing technology, succeeded in elucidating theoretically-predicted behavior of quantum liquid in a non-equilibrium state.

Quantum liquids are macroscopic ensembles of interacting particles dense enough for quantum statistics to manifest itself. For fermions, it is known that, around equilibrium, all the quantum liquids can be universally described within a single theory, so called Landau Fermi liquid theory. The idea is that they can be treated as an ensemble of free “quasi-particles”. This conceptual framework has been applied to many physical systems, such as liquid helium 3, normal metals, heavy fermions, neutron stars, and cold gases, where their properties in the linear-response regime have been successfully described by the theory. However, non-equilibrium properties beyond this regime have still to be established and remain a key issue of many-body physics.

Here, we show a precise experimental demonstration of Landau Fermi-liquid theory extended to the non-equilibrium regime in a 0-D system. Combining transport and sensitive current noise measurements, we have identified the SU(2) and SU(4) symmetries of quantum liquid in a carbon nanotube tuned in the Kondo regime. We find that, while the electronic transport is well described by the free quasi-particle picture around equilibrium just as the Fermi liquid theory tells us, a two-particle scattering process due to residual interaction shows up in the non-equilibrium regime. Our result, in perfect agreement with theory, provides a strong quantitative experimental background for further developments of the many-body physics. Moreover, we discovered a new scaling law for the effective charge, signaling as-yet-unknown universality in the non-equilibrium regime.

This achievement will open up a new way to explore quantum many-body physics through fluctuations, which stands on firm ground even out of equilibrium beyond the conventional Landau Fermi liquid theory. The newly discovered universality would trigger a vast theoretical effort.

Figure (left) In a single particle system, the behavior of the particle is well understood by solving the Schrodinger equation. Here the particle possesses wave nature characterized by the de Broglie wave length. (right) In a many particle system, on the other hand, the particles interact each other in a quantum mechanical way and behave as if they are “liquid”. This is called quantum liquid whose properties are very different from that of the single particle case.

(Link) http://resou.osaka-u.ac.jp/en/research/2015/20151124_1