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Related papers: Growing a LaAlO3/SrTiO3 heterostructure on Ca2Nb3O…

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The two-dimensional electron gas occurring between the band insulators SrTiO$_3$ and LaAlO$_3$ continues to attract considerable interest, due to the possibility of dynamic control over the carrier density, and the ensuing phenomena such as…

Materials Science · Physics 2017-12-13 A. J. H. van der Torren , Z. Liao , C. Xu , N. Gauquelin , C. Yin , J. Aarts , S. J. van der Molen

The novel electronic properties emerging at interfaces between transition metal oxides, and in particular the discovery of conductivity in heterostructures composed of LaAlO$_3$ (LAO) and SrTiO$_3$ (STO) band insulators, have generated new…

We have investigated how the recently-developed water-leaching method for atomically-flat SrTiO3 (STO) substrates affects the transport properties of LaAlO3 (LAO) and STO heterointerfaces. Using pulsed laser deposition at identical growth…

Materials Science · Physics 2016-04-04 J. G. Connell , J. Nichols , J. H. Gruenewald , D. -W. Kim , S. S. A. Seo

The structure and interface characteristics of (LaVO3)6m(SrVO3)m superlattices deposited on (100)-SrTiO3 (STO) substrate were studied using Transmission Electron Microscopy (TEM). Cross-section TEM studies revealed that both LaVO3 (LVO) and…

Materials Science · Physics 2015-05-20 P. Boullay , A. David , W. C. Sheets , U. Lüders , W. Prellier , H. Tan , J. Verbeeck , G. Van Tendeloo , C. Gatel , G. Vincze , Z. Radi

The conducting quasi-two dimensional electron system (q2DES) formed at the interface between LaAlO3 and SrTiO3 band insulators is confronting the condensed matter physics community with new paradigms. While the mechanism for the formation…

Materials Science · Physics 2014-09-11 M. Salluzzo

Nanoscale control of the quasi-two-dimensional electron gas at the LaAlO3/SrTiO3 (LAO/STO) interface by a conductive probe tip has triggered the development of a number of electronic devices. While the spatial distribution of the…

Mesoscale and Nanoscale Physics · Physics 2018-01-17 Zhanzhi Jiang , Xiaoyu Wu , Hyungwoo Lee , Jung-Woo Lee , Jianan Li , Guanglei Cheng , Chang-Beom Eom , Jeremy Levy , Keji Lai

Oxide heterostructures represent a unique playground for triggering the emergence of novel electronic states and for implementing new device concepts. The discovery of 2D conductivity at the $LaAlO_3/SrTiO_3$ interface has been linking for…

We demonstrate the possibility of growing textured La$_{2/3}$Sr$_{1/3}$MnO$_3$ (LSMO) thin films on silicon substrates with magneto-optical and optical properties comparable to high-quality epitaxial layers grown on bulk SrTiO$_3$ (STO).…

Depositing disordered Al on top of SrTiO$_3$ is a cheap and easy way to create a two-dimensional electron system in the SrTiO$_3$ surface layers. To facilitate future device applications we passivate the heterostructure by a disordered…

The interface between the band gap insulators LaAlO3 and SrTiO3 is known to host a highly mobile two-dimensional electron gas. Here we report on the fabrication and characterization of the NdGaO3/SrTiO3 interface, that shares with…

The properties of single-crystal SrTiO$_{3}$ substrates and homoepitaxial SrTiO$_{3}$ films grown by pulsed laser deposition have been compared, in order to understand the loss of interfacial conductivity when more than a critical thickness…

LaAlO$_{3}$ and NdGaO$_{3}$ thin films of different thickness have been grown by pulsed laser deposition on TiO$_2$-terminated SrTiO$_{3}$ single crystals and investigated by soft X-ray photoemission spectroscopy. The surface sensitivity of…

The surface termination of (100)-oriented LaAlO3 (LAO) single crystals was examined by atomic force microscopy and optimized to produce a single-terminated atomically flat surface by annealing. Then the atomically flat STO film was achieved…

Materials Science · Physics 2012-05-09 Z. Q. Liu , Z. Huang , W. M. Lü , K. Gopinadhan , X. Wang , A. Annadi , T. Venkatesan , Ariando

We show that the growth of the heterostructure LaGaO3/SrTiO3 yields the formation of a highly conductive interface. Our samples were carefully analyzed by high resolution electron microscopy, in order to assess their crystal perfection and…

To form a conducting layer at the interface between the oxide insulators LaAlO3 and SrTiO3, the LaAlO3 layer on the SrTiO3 substrate must be at least four unit-cells-thick. The LaAlO3 SrTiO3 heterointerface thus formed exhibits various…

Strontium titanate, SrTiO3, a widely used substrate material for electronic oxide thin film devices, has provided many interesting features. In a combination with a similar oxide material, LaAlO3, it has recently received great interest. It…

Materials Science · Physics 2013-05-29 Alexey S. Kalabukhov , Robert Gunnarsson , Johan Borjesson , Eva Olsson , Tord Claeson , Dag Winkler

We have measured the electronic structure of the two-dimensional electron system (2DES) found at the Al/SrTiO3 (Al/STO) and LaAlO3/SrTiO3 (LAO/STO) interfaces by means of laser angle resolved photoemission spectroscopy, taking advantage of…

Emergent phases in the two-dimensional electron gas (2DEG) formed at the interface between two insulating oxides have attracted great attention in the past decade. We present ab-initio electronic structure calculations for the interface…

Materials Science · Physics 2015-12-24 Hrishit Banerjee , Sumilan Banerjee , Mohit Randeria , Tanusri Saha-Dasgupta

Variations in growth conditions associated with different deposition techniques can greatly affect the phase stability and defect structure of complex oxide heterostructures. We synthesized superlattices of the paramagnetic metal LaNiO3 and…

Strongly Correlated Electrons · Physics 2017-01-31 F. Wrobel , A. F. Mark , G. Christiani , W. Sigle , H. -U. Habermeier , P. A. van Aken , G. Logvenov , B. Keimer , E. Benckiser

The resistance of the electron gas at the interface between the two band insulators LaAlO3 (LAO) and SrTiO3 (STO) typically drops monotonically with temperature and R/T curves during cooling and warm-up look identical for large area…

Mesoscale and Nanoscale Physics · Physics 2017-03-21 M. Z. Minhas , A. Müller , F. Heyroth , H. H. Blaschek , G. Schmidt
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