2010
DOI: 10.1103/physrevb.82.201407
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Nonlinear Hall effect and multichannel conduction inLaTiO3/SrTiO3superlattices

Abstract: We report magneto-transport properties of heterointerfaces between the Mott insulator LaTiO 3 and the band insulator SrTiO 3 in a delta-doping geometry. At low temperatures, we have found a strong nonlinearity in the magnetic field dependence of the Hall resistivity, which can be effectively controlled by varying the temperature and the electric field. We attribute this effect to multichannel conduction of interfacial charges generated by an electronic reconstruction. In particular, the formation of a highly m… Show more

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Cited by 162 publications
(193 citation statements)
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“…Compensating mobile electrons are easily accessible for RTiO 3 /SrTiO 3 structures, as can be visualized by considering the atomically sharp interface as a 50:50 mixture of RTiO 3 and SrTiO 3 , which has the required free electron density [20]. Transport and optical measurements of LaTiO 3 /SrTiO 3 interfaces reveal densities close to those expected for electronic reconstruction [16,21], but interpretation is complicated by conduction by non-interfacial carriers from both substrates and films [15,16]; LaTiO 3 films reported in the literature are often metallic [22]. The sheet resistances of GdTiO 3 grown directly on LSAT and of GdTiO 3 grown on SrTiO 3 buffer layers with different thicknesses are shown in Fig.…”
Section: Two-dimensional Electron Gases (2degs) At Interfaces Betweenmentioning
confidence: 97%
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“…Compensating mobile electrons are easily accessible for RTiO 3 /SrTiO 3 structures, as can be visualized by considering the atomically sharp interface as a 50:50 mixture of RTiO 3 and SrTiO 3 , which has the required free electron density [20]. Transport and optical measurements of LaTiO 3 /SrTiO 3 interfaces reveal densities close to those expected for electronic reconstruction [16,21], but interpretation is complicated by conduction by non-interfacial carriers from both substrates and films [15,16]; LaTiO 3 films reported in the literature are often metallic [22]. The sheet resistances of GdTiO 3 grown directly on LSAT and of GdTiO 3 grown on SrTiO 3 buffer layers with different thicknesses are shown in Fig.…”
Section: Two-dimensional Electron Gases (2degs) At Interfaces Betweenmentioning
confidence: 97%
“…While too resistive for meaningful Hall measurements, the Seebeck coefficient was measured and is positive (ptype), as found for stoichiometric GdTiO 3 [23]. All bilayers are n-type and metallic if the was linear and n-type down to the lowest temperatures [29], in contrast to LaTiO 3 /SrTiO 3 [15,16]. All of the electrons contributing to the Hall resistance satisfy μB << 1 .…”
Section: Two-dimensional Electron Gases (2degs) At Interfaces Betweenmentioning
confidence: 99%
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“…[3][4][5][6][7] Most studies thus far have focused on 2DEGs at polar/nonpolar interfaces, such as LaAlO 3 / SrTiO 3,[8][9][10] LaTiO 3 /SrTiO 3,11,12 and GdTiO 3 /SrTiO 3.…”
mentioning
confidence: 99%
“…Examples include the discovery of a 2-dimensional electron gas (2DEG) and thermopower enhancement in LaTiO 3 /SrTiO 3 (STO) heterostructures [1][2][3] , electric-field control of spin polarization between ferroelectric and ferromagnetic film layers [4] and colossal ionic conductivity at the yttria-stabilized ZrO 2 (YSZ)/STO interface [5] . The strong property modification in heterostructures such as these suggests that the structural, electronic, lattice and orbital degrees of freedom at the interface can be tuned from the individual constituents.…”
mentioning
confidence: 99%