FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2323801747> ?p ?o ?g. }

• W2323801747 abstract "We compute second-order transport coefficients of the dilute Fermi gas at unitarity. The calculation is based on kinetic theory and the Boltzmann equation at second order in the Knudsen expansion. The second-order transport coefficients describe the shear stress relaxation time, nonlinear terms in the strain-stress relation, and nonlinear couplings between vorticity and strain. An exact calculation in the dilute limit gives ${ensuremath{tau}}_{R}=ensuremath{eta}/P$, where ${ensuremath{tau}}_{R}$ is the shear stress relaxation time, $ensuremath{eta}$ is the shear viscosity, and $P$ is pressure. This relation is identical to the result obtained using the Bhatnagar-Gross-Krook approximation to the collision term, but other transport coefficients are sensitive to the exact collision integral." @default.
• W2323801747 created "2016-06-24" @default.
• W2323801747 creator A5028715548 @default.
• W2323801747 date "2014-10-29" @default.
• W2323801747 modified "2023-10-05" @default.
• W2323801747 title "Second-order fluid dynamics for the unitary Fermi gas from kinetic theory" @default.
• W2323801747 cites W1550355308 @default.
• W2323801747 cites W1582471707 @default.
• W2323801747 cites W1967710829 @default.
• W2323801747 cites W1969490992 @default.
• W2323801747 cites W1986358404 @default.
• W2323801747 cites W1988605141 @default.
• W2323801747 cites W2007501680 @default.
• W2323801747 cites W2027232051 @default.
• W2323801747 cites W2028357351 @default.
• W2323801747 cites W2031260040 @default.
• W2323801747 cites W2036311716 @default.
• W2323801747 cites W2037722155 @default.
• W2323801747 cites W2042099747 @default.
• W2323801747 cites W2045961355 @default.
• W2323801747 cites W2046518125 @default.
• W2323801747 cites W2055408431 @default.
• W2323801747 cites W2055767718 @default.
• W2323801747 cites W2056706689 @default.
• W2323801747 cites W2058042134 @default.
• W2323801747 cites W2064311929 @default.
• W2323801747 cites W2066060292 @default.
• W2323801747 cites W2066211183 @default.
• W2323801747 cites W2067871162 @default.
• W2323801747 cites W2078564068 @default.
• W2323801747 cites W2081882693 @default.
• W2323801747 cites W2081977520 @default.
• W2323801747 cites W2083587546 @default.
• W2323801747 cites W2097909025 @default.
• W2323801747 cites W2117267248 @default.
• W2323801747 cites W2128628775 @default.
• W2323801747 cites W2135036759 @default.
• W2323801747 cites W2144293283 @default.
• W2323801747 cites W2157236990 @default.
• W2323801747 cites W2161197687 @default.
• W2323801747 cites W2164013960 @default.
• W2323801747 cites W2962984446 @default.
• W2323801747 cites W3102802194 @default.
• W2323801747 cites W3104071324 @default.
• W2323801747 cites W3105323762 @default.
• W2323801747 cites W3105397373 @default.
• W2323801747 cites W3105741425 @default.
• W2323801747 cites W3121429264 @default.
• W2323801747 doi "https://doi.org/10.1103/physreva.90.043633" @default.
• W2323801747 hasPublicationYear "2014" @default.
• W2323801747 type Work @default.
• W2323801747 sameAs 2323801747 @default.
• W2323801747 citedByCount "7" @default.
• W2323801747 countsByYear W23238017472014 @default.
• W2323801747 countsByYear W23238017472015 @default.
• W2323801747 countsByYear W23238017472016 @default.
• W2323801747 countsByYear W23238017472017 @default.
• W2323801747 countsByYear W23238017472020 @default.
• W2323801747 countsByYear W23238017472023 @default.
• W2323801747 crossrefType "journal-article" @default.
• W2323801747 hasAuthorship W2323801747A5028715548 @default.
• W2323801747 hasBestOaLocation W23238017471 @default.
• W2323801747 hasConcept C10138342 @default.
• W2323801747 hasConcept C121332964 @default.
• W2323801747 hasConcept C121704057 @default.
• W2323801747 hasConcept C121838276 @default.
• W2323801747 hasConcept C130295795 @default.
• W2323801747 hasConcept C135889238 @default.
• W2323801747 hasConcept C140820882 @default.
• W2323801747 hasConcept C147120987 @default.
• W2323801747 hasConcept C158622935 @default.
• W2323801747 hasConcept C162324750 @default.
• W2323801747 hasConcept C165995430 @default.
• W2323801747 hasConcept C182306322 @default.
• W2323801747 hasConcept C19979193 @default.
• W2323801747 hasConcept C200114574 @default.
• W2323801747 hasConcept C35304006 @default.
• W2323801747 hasConcept C37914503 @default.
• W2323801747 hasConcept C38652104 @default.
• W2323801747 hasConcept C41008148 @default.
• W2323801747 hasConcept C62520636 @default.
• W2323801747 hasConcept C85867844 @default.
• W2323801747 hasConcept C97355855 @default.
• W2323801747 hasConceptScore W2323801747C10138342 @default.
• W2323801747 hasConceptScore W2323801747C121332964 @default.
• W2323801747 hasConceptScore W2323801747C121704057 @default.
• W2323801747 hasConceptScore W2323801747C121838276 @default.
• W2323801747 hasConceptScore W2323801747C130295795 @default.
• W2323801747 hasConceptScore W2323801747C135889238 @default.
• W2323801747 hasConceptScore W2323801747C140820882 @default.
• W2323801747 hasConceptScore W2323801747C147120987 @default.
• W2323801747 hasConceptScore W2323801747C158622935 @default.
• W2323801747 hasConceptScore W2323801747C162324750 @default.
• W2323801747 hasConceptScore W2323801747C165995430 @default.
• W2323801747 hasConceptScore W2323801747C182306322 @default.
• W2323801747 hasConceptScore W2323801747C19979193 @default.
• W2323801747 hasConceptScore W2323801747C200114574 @default.
• W2323801747 hasConceptScore W2323801747C35304006 @default.
• W2323801747 hasConceptScore W2323801747C37914503 @default.
• W2323801747 hasConceptScore W2323801747C38652104 @default.

• next