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024 7 _ |a 10.1103/PhysRevB.77.115350
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037 _ _ |a PreJuSER-2330
041 _ _ |a eng
082 _ _ |a 530
084 _ _ |2 WoS
|a Physics, Condensed Matter
100 1 _ |a Ishida, H.
|b 0
|0 P:(DE-HGF)0
245 _ _ |a Origin of metallicity of LaTiO3/SrTiO3 heterostructures
260 _ _ |a College Park, Md.
|b APS
|c 2008
300 _ _ |a 11
336 7 _ |a Journal Article
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440 _ 0 |a Physical Review B
|x 1098-0121
|0 4919
|v 77
500 _ _ |a Record converted from VDB: 12.11.2012
520 _ _ |a It is shown that LaTiO3, in superlattices with SrTiO3, is a strongly correlated metal rather than a Mott insulator. The tetragonal lattice geometry imposed by the SrTiO3 substrate leads to an increase of the Ti 3dt(2g) bandwidth and a reversal of the t(2g) crystal field relative to the orthorhombic bulk geometry. Using dynamical mean field theory based on finite-temperature multiband exact diagonalization, we show that, as a result of these effects, local Coulomb interactions are not strong enough to induce a Mott transition in tetragonal LaTiO3. The experimentally observed metallicity of LaTiO3/SrTiO3 heterostructures is therefore caused not only by the interface but also by the tetragonal geometry of the LaTiO3 layers.
536 _ _ |a Kondensierte Materie
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542 _ _ |i 2008-03-26
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588 _ _ |a Dataset connected to Web of Science
650 _ 7 |a J
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700 1 _ |a Liebsch, A.
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773 1 8 |a 10.1103/physrevb.77.115350
|b American Physical Society (APS)
|d 2008-03-26
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|p 115350
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|t Physical Review B
|v 77
|y 2008
|x 1098-0121
773 _ _ |a 10.1103/PhysRevB.77.115350
|g Vol. 77, p. 11
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856 7 _ |u http://dx.doi.org/10.1103/PhysRevB.77.115350
856 4 _ |u https://juser.fz-juelich.de/record/2330/files/PhysRevB.77.115350.pdf
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914 1 _ |y 2008
915 _ _ |a American Physical Society Transfer of Copyright Agreement
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920 1 _ |k IFF-1
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|d 31.12.2010
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