Matches in SemOpenAlex for { <https://semopenalex.org/work/W2003048996> ?p ?o ?g. }
- W2003048996 abstract "While classical or quantum interacting liquids become turbulent under sufficiently strong driving, it is not obvious what flow pattern an ideal quantum gas develops under similar conditions. Unlike classical noninteracting particles which exhibit rather trivial flow, ideal fermions have to satisfy the exclusion principle, which acts as a form of collective repulsion. We thus study the flow of an ideal Fermi gas as it is driven out of a narrow orifice of width comparable to the Fermi wavelength, employing both a microcanonical approach to transport, and solving a Lindblad equation for Markovian driving leads. Both methods are in good agreement and predict an outflowing current density with a complex microscopic pattern of vorticity in the steady state. Applying a bias of the order of the chemical potential results in a short-range correlated antiferromagnetic vorticity pattern, corresponding to local moments of the order of a tenth of a magneton, $ehbar/2m$, if the fermions are charged. The latter may be detectable by magnetosensitive spectroscopy in strongly driven cold gases (atoms) or clean electronic nanostructures (electrons)." @default.
- W2003048996 created "2016-06-24" @default.
- W2003048996 creator A5010526289 @default.
- W2003048996 creator A5045296314 @default.
- W2003048996 creator A5072782132 @default.
- W2003048996 creator A5076782439 @default.
- W2003048996 date "2013-10-09" @default.
- W2003048996 modified "2023-09-25" @default.
- W2003048996 title "Quantum-statistics-induced flow patterns in driven ideal Fermi gases" @default.
- W2003048996 cites W1484667027 @default.
- W2003048996 cites W1523636626 @default.
- W2003048996 cites W1575867504 @default.
- W2003048996 cites W1666710590 @default.
- W2003048996 cites W1875695870 @default.
- W2003048996 cites W1969199716 @default.
- W2003048996 cites W1973063342 @default.
- W2003048996 cites W1979308046 @default.
- W2003048996 cites W1984962612 @default.
- W2003048996 cites W1990595724 @default.
- W2003048996 cites W2005436767 @default.
- W2003048996 cites W2016293496 @default.
- W2003048996 cites W2020953818 @default.
- W2003048996 cites W2024329825 @default.
- W2003048996 cites W2026237280 @default.
- W2003048996 cites W2026442798 @default.
- W2003048996 cites W2033959570 @default.
- W2003048996 cites W2036382602 @default.
- W2003048996 cites W2037879124 @default.
- W2003048996 cites W2041578725 @default.
- W2003048996 cites W2046775071 @default.
- W2003048996 cites W2050232844 @default.
- W2003048996 cites W2056238079 @default.
- W2003048996 cites W2065022163 @default.
- W2003048996 cites W2065425034 @default.
- W2003048996 cites W2081317485 @default.
- W2003048996 cites W2110970930 @default.
- W2003048996 cites W2118740470 @default.
- W2003048996 cites W2136661619 @default.
- W2003048996 cites W2160043413 @default.
- W2003048996 cites W2163964512 @default.
- W2003048996 cites W224387178 @default.
- W2003048996 cites W2962806804 @default.
- W2003048996 cites W3098595953 @default.
- W2003048996 cites W3104493244 @default.
- W2003048996 cites W3105397373 @default.
- W2003048996 cites W3142882841 @default.
- W2003048996 cites W4231097340 @default.
- W2003048996 cites W4252293059 @default.
- W2003048996 cites W2011338988 @default.
- W2003048996 doi "https://doi.org/10.1103/physreva.88.043611" @default.
- W2003048996 hasPublicationYear "2013" @default.
- W2003048996 type Work @default.
- W2003048996 sameAs 2003048996 @default.
- W2003048996 citedByCount "7" @default.
- W2003048996 countsByYear W20030489962014 @default.
- W2003048996 countsByYear W20030489962017 @default.
- W2003048996 countsByYear W20030489962018 @default.
- W2003048996 countsByYear W20030489962023 @default.
- W2003048996 crossrefType "journal-article" @default.
- W2003048996 hasAuthorship W2003048996A5010526289 @default.
- W2003048996 hasAuthorship W2003048996A5045296314 @default.
- W2003048996 hasAuthorship W2003048996A5072782132 @default.
- W2003048996 hasAuthorship W2003048996A5076782439 @default.
- W2003048996 hasBestOaLocation W20030489964 @default.
- W2003048996 hasConcept C111472728 @default.
- W2003048996 hasConcept C121332964 @default.
- W2003048996 hasConcept C122527463 @default.
- W2003048996 hasConcept C138885662 @default.
- W2003048996 hasConcept C140820882 @default.
- W2003048996 hasConcept C147120987 @default.
- W2003048996 hasConcept C186769553 @default.
- W2003048996 hasConcept C200114574 @default.
- W2003048996 hasConcept C26873012 @default.
- W2003048996 hasConcept C2776639384 @default.
- W2003048996 hasConcept C30342001 @default.
- W2003048996 hasConcept C3079626 @default.
- W2003048996 hasConcept C38349280 @default.
- W2003048996 hasConcept C52233224 @default.
- W2003048996 hasConcept C57879066 @default.
- W2003048996 hasConcept C62520636 @default.
- W2003048996 hasConcept C84114770 @default.
- W2003048996 hasConcept C85867844 @default.
- W2003048996 hasConcept C97355855 @default.
- W2003048996 hasConceptScore W2003048996C111472728 @default.
- W2003048996 hasConceptScore W2003048996C121332964 @default.
- W2003048996 hasConceptScore W2003048996C122527463 @default.
- W2003048996 hasConceptScore W2003048996C138885662 @default.
- W2003048996 hasConceptScore W2003048996C140820882 @default.
- W2003048996 hasConceptScore W2003048996C147120987 @default.
- W2003048996 hasConceptScore W2003048996C186769553 @default.
- W2003048996 hasConceptScore W2003048996C200114574 @default.
- W2003048996 hasConceptScore W2003048996C26873012 @default.
- W2003048996 hasConceptScore W2003048996C2776639384 @default.
- W2003048996 hasConceptScore W2003048996C30342001 @default.
- W2003048996 hasConceptScore W2003048996C3079626 @default.
- W2003048996 hasConceptScore W2003048996C38349280 @default.
- W2003048996 hasConceptScore W2003048996C52233224 @default.
- W2003048996 hasConceptScore W2003048996C57879066 @default.
- W2003048996 hasConceptScore W2003048996C62520636 @default.
- W2003048996 hasConceptScore W2003048996C84114770 @default.