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dc.contributor.authorLotnyk, Dmytro
dc.contributor.authorEyal, Anna
dc.contributor.authorZhelev, Nikolay
dc.contributor.authorSebastian, Abhilash
dc.contributor.authorSmith, Eric
dc.contributor.authorTerilli, Michael
dc.contributor.authorWilson, John
dc.contributor.authorMueller, Erich
dc.contributor.authorEinzel, Dietrich
dc.contributor.authorSaunders, John
dc.contributor.authorParpia, Jeevak
dc.date.accessioned2019-06-04T21:38:54Z
dc.date.available2019-06-04T21:38:54Z
dc.date.issued2020-09-24
dc.identifier.urihttps://hdl.handle.net/1813/66208
dc.description.abstractThe investigation of transport properties in normal liquid helium-3 and its topological superfluid phases provides insights into related phenomena in electron fluids, topological materials, and putative topological superconductors. It relies on the measurement of mass, heat, and spin currents, due to system neutrality. Of particular interest is transport in strongly confining channels of height approaching the superfluid coherence length, to enhance the relative contribution of surface excitations, and suppress hydrodynamic counter-flow. Here we report on the thermal conduction of helium-3 in a 1.1 um high channel. The experiment was carried out by locally heating one chamber and by measuring the flow of energy out of that chamber. Figure 2) In the normal state (Figures 3, 4 and Supplemental Figures 6, 7) we observe a diffusive thermal conductivity that is approximately temperature independent, consistent with interference of bulk and boundary scattering. In the superfluid, the thermal conductivity is only weakly temperature dependent (Figure 5), requiring detailed theoretical analysis. An anomalous thermal response is detected in the superfluid (Figures 6, 7 and Supplemental Figures 2, 3, 4) which we propose arises from the emission of a flux of surface excitations from the channel. Supplemental Figure 1 summarizes calculations that show that the anomalous heat transport cannot arise from normal-superfluid counterflow. In this package we provide the data set was used to plot the figures so that digitization is not needed and the data may be used for comparison in future works.
dc.description.sponsorshipThis work was supported at Cornell by the NSF under DMR-1708341, 2002692 (Parpia), PHY-1806357 (Mueller), in London by the EPSRC under EP/J022004/1. John Wilson's participation was supported in part by the Cornell Center for Materials research with funding from the Research Experience for Undergraduates program (DMR-1719875). In addition, the research leading to these results has received funding from the European Union’s Horizon 2020 Research and Innovation Programme, under Grant Agreement no 824109. Fabrication was carried out at the Cornell Nanoscale Science and Technology Facility (CNF) with assistance and advice from technical staff. The CNF is a member of the National Nanotechnology Coordinated Infrastructure (NNCI), which is supported by the National Science Foundation (Grant NNCI-1542081).
dc.language.isoen_USen_US
dc.relation.isreferencedbyLotnyk, D., Eyal, A., Zhelev, N. et al. Thermal transport of helium-3 in a strongly confining channel. Nat Commun 11, 4843 (2020). https://doi.org/10.1038/s41467-020-18662-8
dc.rightsAttribution 4.0 International*
dc.rights.urihttp://creativecommons.org/licenses/by/4.0/*
dc.subjectNormal 3He
dc.subjectSuperfluid 3He
dc.subjectThermal Conductivity of a Fermi Liquid
dc.subjectConfined Fluid
dc.subjectFountain Pressure
dc.subjectSurface Mediated Thermal Conduction
dc.titleData from: Thermal transport of helium-3 in a strongly confining channelen_US
dc.typedataseten_US
dc.relation.isreferencedbyurihttps://doi.org/10.1038/s41467-020-18662-8
dc.identifier.doihttps://doi.org/10.7298/4fhq-e356


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