FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2022649861> ?p ?o ?g. }

• W2022649861 abstract "Several new classes of compounds can be modeled in first approximation by electrons on the triangular lattice that interact through on-site repulsion $U$ as well as nearest-neighbor repulsion $V$. This extended Hubbard model on a triangular lattice has been studied mostly in the strong coupling limit for only a few types of instabilities. Using the extended two-particle self-consistent approach (ETPSC), that is valid at weak to intermediate coupling, we present an unbiased study of the density and interaction dependent crossover diagram for spin- and charge-density wave instabilities of the normal state at arbitrary wave vector. When $U$ dominates over $V$ and electron filling is large, instabilities are chiefly in the spin sector and are controlled mostly by Fermi surface properties. Increasing $V$ eventually leads to charge instabilities. In the latter case, it is mostly the wave vector dependence of the vertex that determines the wave vector of the instability rather than Fermi surface properties. At small filling, nontrivial instabilities appear only beyond the weak coupling limit. There again, charge-density wave instabilities are favored over a wide range of dopings by large $V$ at wave vectors corresponding to $sqrt{(3)}ifmmodetimeselsetexttimesfi{}sqrt{(3)}$ superlattice in real space. Commensurate fillings do not play a special role for this instability. Increasing $U$ leads to competition with ferromagnetism. At negative values of $U$ or $V$, neglecting superconducting fluctuations, one finds that charge instabilities are favored. In general, the crossover diagram presents a rich variety of instabilities. We also show that thermal charge-density wave fluctuations in the renormalized-classical regime can open a pseudogap in the single-particle spectral weight, just as spin or superconducting fluctuations." @default.
• W2022649861 created "2016-06-24" @default.
• W2022649861 creator A5026699910 @default.
• W2022649861 creator A5043786584 @default.
• W2022649861 creator A5047325183 @default.
• W2022649861 date "2008-06-05" @default.
• W2022649861 modified "2023-10-17" @default.
• W2022649861 title "Competition between charge and spin order in the<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:mi>t</mml:mi><mml:mtext>−</mml:mtext><mml:mi>U</mml:mi><mml:mtext>−</mml:mtext><mml:mi>V</mml:mi></mml:mrow></mml:math>extended Hubbard model on the triangular lattice" @default.
• W2022649861 cites W1483693037 @default.
• W2022649861 cites W1499192185 @default.
• W2022649861 cites W1648096492 @default.
• W2022649861 cites W1666799076 @default.
• W2022649861 cites W1830239731 @default.
• W2022649861 cites W1853787478 @default.
• W2022649861 cites W1979490640 @default.
• W2022649861 cites W1990095135 @default.
• W2022649861 cites W1990760741 @default.
• W2022649861 cites W1998837897 @default.
• W2022649861 cites W2009569291 @default.
• W2022649861 cites W2020649173 @default.
• W2022649861 cites W2023003113 @default.
• W2022649861 cites W2035339342 @default.
• W2022649861 cites W2037061674 @default.
• W2022649861 cites W2041923345 @default.
• W2022649861 cites W2048556304 @default.
• W2022649861 cites W2049181746 @default.
• W2022649861 cites W2052504236 @default.
• W2022649861 cites W2054424147 @default.
• W2022649861 cites W2055691504 @default.
• W2022649861 cites W2059658587 @default.
• W2022649861 cites W2066901226 @default.
• W2022649861 cites W2070835228 @default.
• W2022649861 cites W2086145921 @default.
• W2022649861 cites W2086540608 @default.
• W2022649861 cites W2095221361 @default.
• W2022649861 cites W2136027377 @default.
• W2022649861 cites W2154633152 @default.
• W2022649861 cites W2227891475 @default.
• W2022649861 cites W2318800141 @default.
• W2022649861 cites W2531745781 @default.
• W2022649861 doi "https://doi.org/10.1103/physrevb.77.214408" @default.
• W2022649861 hasPublicationYear "2008" @default.
• W2022649861 type Work @default.
• W2022649861 sameAs 2022649861 @default.
• W2022649861 citedByCount "24" @default.
• W2022649861 countsByYear W20226498612015 @default.
• W2022649861 countsByYear W20226498612016 @default.
• W2022649861 countsByYear W20226498612017 @default.
• W2022649861 countsByYear W20226498612018 @default.
• W2022649861 countsByYear W20226498612019 @default.
• W2022649861 countsByYear W20226498612021 @default.
• W2022649861 countsByYear W20226498612023 @default.
• W2022649861 crossrefType "journal-article" @default.
• W2022649861 hasAuthorship W2022649861A5026699910 @default.
• W2022649861 hasAuthorship W2022649861A5043786584 @default.
• W2022649861 hasAuthorship W2022649861A5047325183 @default.
• W2022649861 hasBestOaLocation W20226498612 @default.
• W2022649861 hasConcept C109496249 @default.
• W2022649861 hasConcept C121332964 @default.
• W2022649861 hasConcept C127413603 @default.
• W2022649861 hasConcept C131584629 @default.
• W2022649861 hasConcept C188082385 @default.
• W2022649861 hasConcept C201991461 @default.
• W2022649861 hasConcept C207821765 @default.
• W2022649861 hasConcept C24890656 @default.
• W2022649861 hasConcept C26873012 @default.
• W2022649861 hasConcept C2780525273 @default.
• W2022649861 hasConcept C2781204021 @default.
• W2022649861 hasConcept C54101563 @default.
• W2022649861 hasConcept C62520636 @default.
• W2022649861 hasConcept C78519656 @default.
• W2022649861 hasConceptScore W2022649861C109496249 @default.
• W2022649861 hasConceptScore W2022649861C121332964 @default.
• W2022649861 hasConceptScore W2022649861C127413603 @default.
• W2022649861 hasConceptScore W2022649861C131584629 @default.
• W2022649861 hasConceptScore W2022649861C188082385 @default.
• W2022649861 hasConceptScore W2022649861C201991461 @default.
• W2022649861 hasConceptScore W2022649861C207821765 @default.
• W2022649861 hasConceptScore W2022649861C24890656 @default.
• W2022649861 hasConceptScore W2022649861C26873012 @default.
• W2022649861 hasConceptScore W2022649861C2780525273 @default.
• W2022649861 hasConceptScore W2022649861C2781204021 @default.
• W2022649861 hasConceptScore W2022649861C54101563 @default.
• W2022649861 hasConceptScore W2022649861C62520636 @default.
• W2022649861 hasConceptScore W2022649861C78519656 @default.
• W2022649861 hasIssue "21" @default.
• W2022649861 hasLocation W20226498611 @default.
• W2022649861 hasLocation W20226498612 @default.
• W2022649861 hasOpenAccess W2022649861 @default.
• W2022649861 hasPrimaryLocation W20226498611 @default.
• W2022649861 hasRelatedWork W1631558033 @default.
• W2022649861 hasRelatedWork W1965397319 @default.
• W2022649861 hasRelatedWork W1981664029 @default.
• W2022649861 hasRelatedWork W2056892828 @default.
• W2022649861 hasRelatedWork W2096343998 @default.
• W2022649861 hasRelatedWork W2171425679 @default.
• W2022649861 hasRelatedWork W2892520477 @default.
• W2022649861 hasRelatedWork W2963992548 @default.
• W2022649861 hasRelatedWork W3114312134 @default.
• W2022649861 hasRelatedWork W4360874952 @default.

• next