Matches in SemOpenAlex for { <https://semopenalex.org/work/W2900638005> ?p ?o ?g. }
- W2900638005 abstract "We study the formation of bound states in a one-dimensional, single-component Fermi chain with attractive interactions. The phase diagram, computed from DMRG (density matrix renormalization group), shows not only a superfluid of paired fermions (pair phase) and a liquid of fermion triplets (trion phase), but also a phase with two gapless modes. We show that the latter phase is described by a 2-component Tomonaga-Luttinger liquid (TLL) theory, consisting of one charged and one neutral mode. We argue based on our numerical data, that the single, pair, and trion phases are descendants of the 2-component TLL theory. We speculate on the nature of the phase transitions amongst these phases." @default.
- W2900638005 created "2018-11-29" @default.
- W2900638005 creator A5009167599 @default.
- W2900638005 creator A5019056893 @default.
- W2900638005 creator A5040055779 @default.
- W2900638005 creator A5079676164 @default.
- W2900638005 date "2019-11-07" @default.
- W2900638005 modified "2023-09-30" @default.
- W2900638005 title "Emergent mode and bound states in single-component one-dimensional lattice fermionic systems" @default.
- W2900638005 cites W1485771830 @default.
- W2900638005 cites W1671053170 @default.
- W2900638005 cites W1929358554 @default.
- W2900638005 cites W1938944616 @default.
- W2900638005 cites W1950412959 @default.
- W2900638005 cites W1971484191 @default.
- W2900638005 cites W1973700370 @default.
- W2900638005 cites W1973972788 @default.
- W2900638005 cites W1979308046 @default.
- W2900638005 cites W1984903703 @default.
- W2900638005 cites W1997529771 @default.
- W2900638005 cites W2013398427 @default.
- W2900638005 cites W2013548522 @default.
- W2900638005 cites W2021691343 @default.
- W2900638005 cites W2027792124 @default.
- W2900638005 cites W2030278814 @default.
- W2900638005 cites W2037768897 @default.
- W2900638005 cites W2045699664 @default.
- W2900638005 cites W2057563627 @default.
- W2900638005 cites W2059170012 @default.
- W2900638005 cites W2062104302 @default.
- W2900638005 cites W2069840277 @default.
- W2900638005 cites W2070673282 @default.
- W2900638005 cites W2071265569 @default.
- W2900638005 cites W2079212481 @default.
- W2900638005 cites W2085739341 @default.
- W2900638005 cites W2089215777 @default.
- W2900638005 cites W2101936997 @default.
- W2900638005 cites W2114073402 @default.
- W2900638005 cites W2143224758 @default.
- W2900638005 cites W2241142881 @default.
- W2900638005 cites W2280168845 @default.
- W2900638005 cites W2566467992 @default.
- W2900638005 cites W2592094301 @default.
- W2900638005 cites W2611611504 @default.
- W2900638005 cites W2618465568 @default.
- W2900638005 cites W2741062831 @default.
- W2900638005 cites W2752081759 @default.
- W2900638005 cites W2752346050 @default.
- W2900638005 cites W2792505362 @default.
- W2900638005 cites W2793991988 @default.
- W2900638005 cites W2949867928 @default.
- W2900638005 cites W2963588386 @default.
- W2900638005 cites W2964120899 @default.
- W2900638005 cites W3047351161 @default.
- W2900638005 cites W3099428731 @default.
- W2900638005 cites W3100488664 @default.
- W2900638005 cites W3124300277 @default.
- W2900638005 doi "https://doi.org/10.1103/physrevb.100.201101" @default.
- W2900638005 hasPublicationYear "2019" @default.
- W2900638005 type Work @default.
- W2900638005 sameAs 2900638005 @default.
- W2900638005 citedByCount "11" @default.
- W2900638005 countsByYear W29006380052020 @default.
- W2900638005 countsByYear W29006380052021 @default.
- W2900638005 countsByYear W29006380052022 @default.
- W2900638005 countsByYear W29006380052023 @default.
- W2900638005 crossrefType "journal-article" @default.
- W2900638005 hasAuthorship W2900638005A5009167599 @default.
- W2900638005 hasAuthorship W2900638005A5019056893 @default.
- W2900638005 hasAuthorship W2900638005A5040055779 @default.
- W2900638005 hasAuthorship W2900638005A5079676164 @default.
- W2900638005 hasBestOaLocation W29006380051 @default.
- W2900638005 hasConcept C121332964 @default.
- W2900638005 hasConcept C149288129 @default.
- W2900638005 hasConcept C168167062 @default.
- W2900638005 hasConcept C174084160 @default.
- W2900638005 hasConcept C17729963 @default.
- W2900638005 hasConcept C189148282 @default.
- W2900638005 hasConcept C197334999 @default.
- W2900638005 hasConcept C25536358 @default.
- W2900638005 hasConcept C26873012 @default.
- W2900638005 hasConcept C29547527 @default.
- W2900638005 hasConcept C44280652 @default.
- W2900638005 hasConcept C52233224 @default.
- W2900638005 hasConcept C62520636 @default.
- W2900638005 hasConcept C68532491 @default.
- W2900638005 hasConcept C72190298 @default.
- W2900638005 hasConcept C79118098 @default.
- W2900638005 hasConcept C84114770 @default.
- W2900638005 hasConcept C85906118 @default.
- W2900638005 hasConceptScore W2900638005C121332964 @default.
- W2900638005 hasConceptScore W2900638005C149288129 @default.
- W2900638005 hasConceptScore W2900638005C168167062 @default.
- W2900638005 hasConceptScore W2900638005C174084160 @default.
- W2900638005 hasConceptScore W2900638005C17729963 @default.
- W2900638005 hasConceptScore W2900638005C189148282 @default.
- W2900638005 hasConceptScore W2900638005C197334999 @default.
- W2900638005 hasConceptScore W2900638005C25536358 @default.
- W2900638005 hasConceptScore W2900638005C26873012 @default.
- W2900638005 hasConceptScore W2900638005C29547527 @default.