000888620 001__ 888620
000888620 005__ 20221109161718.0
000888620 0247_ $$2doi$$a10.21468/SciPostPhys.9.6.084
000888620 0247_ $$2Handle$$a2128/26425
000888620 0247_ $$2WOS$$aWOS:000606593100006
000888620 037__ $$aFZJ-2020-05072
000888620 082__ $$a530
000888620 1001_ $$0P:(DE-Juel1)133032$$aRohe, Daniel$$b0$$eCorresponding author$$ufzj
000888620 245__ $$aQuasi-particle functional Renormalisation Group calculations in the two-dimensional half-filled Hubbard model at finite temperatures
000888620 260__ $$aAmsterdam$$bSciPost Foundation$$c2020
000888620 3367_ $$2DRIVER$$aarticle
000888620 3367_ $$2DataCite$$aOutput Types/Journal article
000888620 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1610714571_9558
000888620 3367_ $$2BibTeX$$aARTICLE
000888620 3367_ $$2ORCID$$aJOURNAL_ARTICLE
000888620 3367_ $$00$$2EndNote$$aJournal Article
000888620 520__ $$aWe present a highly parallelisable scheme for treating functional Renormalisation Group equations which incorporates a quasi-particle-based feedback on the flow and provides direct access to real-frequency self-energy data. This allows to map out the boundaries of Fermi-liquid regimes and to study the effect of quasi-particle degradation near Fermi liquid instabilities. As a first application, selected results for the two-dimensional half-filled perfectly nested Hubbard model are shown.
000888620 536__ $$0G:(DE-HGF)POF3-511$$a511 - Computational Science and Mathematical Methods (POF3-511)$$cPOF3-511$$fPOF III$$x0
000888620 536__ $$0G:(DE-Juel1)jjsc45_20190501$$aHigh-resolution Functional Renormalisation Group (fRG) calculations for the 2d Hubbard model (jjsc45_20190501)$$cjjsc45_20190501$$fHigh-resolution Functional Renormalisation Group (fRG) calculations for the 2d Hubbard model$$x1
000888620 536__ $$0G:(DE-Juel1)SDLQM$$aSimulation and Data Laboratory Quantum Materials (SDLQM) (SDLQM)$$cSDLQM$$fSimulation and Data Laboratory Quantum Materials (SDLQM)$$x2
000888620 588__ $$aDataset connected to CrossRef
000888620 7001_ $$0P:(DE-HGF)0$$aHonerkamp , Carsten$$b1
000888620 773__ $$0PERI:(DE-600)2886659-9$$a10.21468/SciPostPhys.9.6.084$$gVol. 9, no. 6, p. 084$$n6$$p084$$tSciPost physics$$v9$$x2542-4653$$y2020
000888620 8564_ $$uhttps://juser.fz-juelich.de/record/888620/files/SciPostPhys_9_6_084.pdf$$yOpenAccess
000888620 909CO $$ooai:juser.fz-juelich.de:888620$$pdnbdelivery$$pdriver$$pVDB$$popen_access$$popenaire
000888620 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)133032$$aForschungszentrum Jülich$$b0$$kFZJ
000888620 9101_ $$0I:(DE-588b)36225-6$$6P:(DE-HGF)0$$aRWTH Aachen$$b1$$kRWTH
000888620 9131_ $$0G:(DE-HGF)POF3-511$$1G:(DE-HGF)POF3-510$$2G:(DE-HGF)POF3-500$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bKey Technologies$$lSupercomputing & Big Data$$vComputational Science and Mathematical Methods$$x0
000888620 9141_ $$y2020
000888620 915__ $$0StatID:(DE-HGF)0150$$2StatID$$aDBCoverage$$bWeb of Science Core Collection$$d2020-09-10
000888620 915__ $$0LIC:(DE-HGF)CCBY4$$2HGFVOC$$aCreative Commons Attribution CC BY 4.0
000888620 915__ $$0StatID:(DE-HGF)1150$$2StatID$$aDBCoverage$$bCurrent Contents - Physical, Chemical and Earth Sciences$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0501$$2StatID$$aDBCoverage$$bDOAJ Seal$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0500$$2StatID$$aDBCoverage$$bDOAJ$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0113$$2StatID$$aWoS$$bScience Citation Index Expanded$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000888620 915__ $$0StatID:(DE-HGF)0030$$2StatID$$aPeer Review$$bDOAJ : Open peer review$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0160$$2StatID$$aDBCoverage$$bEssential Science Indicators$$d2020-09-10
000888620 915__ $$0StatID:(DE-HGF)0199$$2StatID$$aDBCoverage$$bClarivate Analytics Master Journal List$$d2020-09-10
000888620 920__ $$lno
000888620 9201_ $$0I:(DE-Juel1)JSC-20090406$$kJSC$$lJülich Supercomputing Center$$x0
000888620 9201_ $$0I:(DE-82)080012_20140620$$kJARA-HPC$$lJARA - HPC$$x1
000888620 980__ $$ajournal
000888620 980__ $$aVDB
000888620 980__ $$aI:(DE-Juel1)JSC-20090406
000888620 980__ $$aI:(DE-82)080012_20140620
000888620 980__ $$aUNRESTRICTED
000888620 9801_ $$aFullTexts