000059216 001__ 59216 000059216 005__ 20200423204541.0 000059216 0247_ $$2DOI$$a10.1103/PhysRevLett.98.216403 000059216 0247_ $$2WOS$$aWOS:000246776100042 000059216 0247_ $$2Handle$$a2128/7753 000059216 037__ $$aPreJuSER-59216 000059216 041__ $$aeng 000059216 082__ $$a550 000059216 084__ $$2WoS$$aPhysics, Multidisciplinary 000059216 1001_ $$0P:(DE-Juel1)VDB941$$aLiebsch, A.$$b0$$uFZJ 000059216 245__ $$aSubband Filling and Mott Transition in Ca2-xSrxRuO4 000059216 260__ $$aCollege Park, Md.$$bAPS$$c2007 000059216 300__ $$a216403 000059216 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article 000059216 3367_ $$2DataCite$$aOutput Types/Journal article 000059216 3367_ $$00$$2EndNote$$aJournal Article 000059216 3367_ $$2BibTeX$$aARTICLE 000059216 3367_ $$2ORCID$$aJOURNAL_ARTICLE 000059216 3367_ $$2DRIVER$$aarticle 000059216 440_0 $$04925$$aPhysical Review Letters$$v98$$x0031-9007 000059216 500__ $$aRecord converted from VDB: 12.11.2012 000059216 520__ $$aA new concept is proposed for the paramagnetic metal insulator transition in the layer perovskite Ca2-xSrxRuO4. Whereas the pure Sr compound is metallic up to large Coulomb energies due to strong orbital fluctuations, structural changes induced by doping with Ca give rise to an interorbital charge transfer which makes the material extremely sensitive to local correlations. Using dynamical mean field theory based on finite temperature multiband exact diagonalization, it is shown that the combination of crystal field splitting and on-site Coulomb interactions leads to complete filling of the d(xy) band and to a Mott transition in the half-filled d(xz,yz) bands. 000059216 536__ $$0G:(DE-Juel1)FUEK414$$2G:(DE-HGF)$$aKondensierte Materie$$cP54$$x0 000059216 588__ $$aDataset connected to Web of Science 000059216 650_7 $$2WoSType$$aJ 000059216 7001_ $$0P:(DE-HGF)0$$aIshida, H.$$b1 000059216 773__ $$0PERI:(DE-600)1472655-5$$a10.1103/PhysRevLett.98.216403$$gVol. 98, p. 216403$$p216403$$q98<216403$$tPhysical review letters$$v98$$x0031-9007$$y2007 000059216 8567_ $$uhttp://dx.doi.org/10.1103/PhysRevLett.98.216403 000059216 8564_ $$uhttps://juser.fz-juelich.de/record/59216/files/FZJ-59216.pdf$$yOpenAccess$$zPublished final document. 000059216 8564_ $$uhttps://juser.fz-juelich.de/record/59216/files/FZJ-59216.jpg?subformat=icon-1440$$xicon-1440$$yOpenAccess 000059216 8564_ $$uhttps://juser.fz-juelich.de/record/59216/files/FZJ-59216.jpg?subformat=icon-180$$xicon-180$$yOpenAccess 000059216 8564_ $$uhttps://juser.fz-juelich.de/record/59216/files/FZJ-59216.jpg?subformat=icon-640$$xicon-640$$yOpenAccess 000059216 909CO $$ooai:juser.fz-juelich.de:59216$$pdnbdelivery$$pVDB$$pdriver$$popen_access$$popenaire 000059216 9131_ $$0G:(DE-Juel1)FUEK414$$bMaterie$$kP54$$lKondensierte Materie$$vKondensierte Materie$$x0$$zentfällt bis 2009 000059216 9141_ $$y2007 000059216 915__ $$0StatID:(DE-HGF)0010$$aJCR/ISI refereed 000059216 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess 000059216 915__ $$0LIC:(DE-HGF)APS-112012$$2HGFVOC$$aAmerican Physical Society Transfer of Copyright Agreement 000059216 9201_ $$0I:(DE-Juel1)VDB781$$d31.12.2010$$gIFF$$kIFF-1$$lQuanten-Theorie der Materialien$$x1 000059216 970__ $$aVDB:(DE-Juel1)93189 000059216 980__ $$aVDB 000059216 980__ $$aConvertedRecord 000059216 980__ $$ajournal 000059216 980__ $$aI:(DE-Juel1)PGI-1-20110106 000059216 980__ $$aUNRESTRICTED 000059216 980__ $$aFullTexts 000059216 9801_ $$aFullTexts 000059216 981__ $$aI:(DE-Juel1)PGI-1-20110106