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Transport of bound quasiparticle states in a two-dimensional boundary superfluid

The B phase of superfluid (3)He can be cooled into the pure superfluid regime, where the thermal quasiparticle density is negligible. The bulk superfluid is surrounded by a quantum well at the boundaries of the container, confining a sea of quasiparticles with energies below that of those in the bul...

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Detalles Bibliográficos
Autores principales: Autti, Samuli, Haley, Richard P., Jennings, Asher, Pickett, George R., Poole, Malcolm, Schanen, Roch, Soldatov, Arkady A., Tsepelin, Viktor, Vonka, Jakub, Zavjalov, Vladislav V., Zmeev, Dmitry E.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10622538/
https://www.ncbi.nlm.nih.gov/pubmed/37919295
http://dx.doi.org/10.1038/s41467-023-42520-y
Descripción
Sumario:The B phase of superfluid (3)He can be cooled into the pure superfluid regime, where the thermal quasiparticle density is negligible. The bulk superfluid is surrounded by a quantum well at the boundaries of the container, confining a sea of quasiparticles with energies below that of those in the bulk. We can create a non-equilibrium distribution of these states within the quantum well and observe the dynamics of their motion indirectly. Here we show that the induced quasiparticle currents flow diffusively in the two-dimensional system. Combining this with a direct measurement of energy conservation, we conclude that the bulk superfluid (3)He is effectively surrounded by an independent two-dimensional superfluid, which is isolated from the bulk superfluid but which readily interacts with mechanical probes. Our work shows that this two-dimensional quantum condensate and the dynamics of the surface bound states are experimentally accessible, opening the possibility of engineering two-dimensional quantum condensates of arbitrary topology.