11 results on '"Scotti Di Uccio, U"'
Search Results
2. Conducting interfaces between band insulating oxides: The LaGaO3/SrTiO3 heterostructure.
- Author
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Perna, P., Maccariello, D., Radovic, M., Scotti di Uccio, U., Pallecchi, I., Codda, M., Marré, D., Cantoni, C., Gazquez, J., Varela, M., Pennycook, S. J., and Granozio, F. Miletto
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SEMICONDUCTOR junctions ,LANTHANUM compounds ,STRONTIUM compounds ,HETEROSTRUCTURES ,ELECTRON distribution ,ATOMIC structure ,ELECTRONIC structure ,ELECTRON gas - Abstract
We show that the growth of the heterostructure LaGaO
3 /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 evaluate the abruptness of the interface. Their carrier density and sheet resistance are compared to the case of LaAlO3 /SrTiO3 and a superconducting transition is found. The results open the route to widening the field of polar-nonpolar interfaces, pose some phenomenological constrains to their underlying physics and highlight the chance of tailoring their properties for future applications by adopting suitable polar materials. [ABSTRACT FROM AUTHOR]- Published
- 2010
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3. Magnetic and magnetotransport properties of La0.7Sr0.3MnO3/Permalloy heterostructures.
- Author
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Ruotolo, A., Oropallo, A., Miletto Granozio, F., Pepe, G. P., Perna, P., and Scotti di Uccio, U.
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HETEROSTRUCTURES ,CRYSTALS ,SUPERLATTICES ,MAGNETIC fields ,MANGANESE ores ,OXIDE minerals - Abstract
The magnetic and magnetotransport properties of La
0.7 Sr0.3 MnO3 /Permalloy heterostructures are investigated. La0.7 Sr0.3 MnO3 films were grown on (110) SrTiO3 in order to induce an in-plane anisotropy with the easy axis along the [001] direction. An easy axis of magnetization was induced in the Permalloy in the same direction through the application of a magnetic field during the growth. The magnetic characterization of the bilayer is presented and discussed. The transport properties of devices operated in the current perpendicular to plane mode are shown. The possibility of fabricating magnetoresistive devices by simply depositing a ferromagnetic counterelectrode on a manganite film is demonstrated. [ABSTRACT FROM AUTHOR]- Published
- 2006
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4. Critical influence of target-to-substrate distance on conductive properties of LaGaO3/SrTiO3 interfaces deposited at 10-1 mbar oxygen pressure.
- Author
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Aruta, C., Amoruso, S., Ausanio, G., Bruzzese, R., Di Gennaro, E., Lanzano, M., Miletto Granozio, F., Riaz, Muhammad, Sambri, A., Scotti di Uccio, U., and Wang, X.
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SUBSTRATES (Materials science) ,HETEROSTRUCTURES ,ELECTRON gas ,LANTHANUM compounds ,MICROSTRUCTURE ,PULSED laser deposition - Abstract
We investigate pulsed laser deposition of LaGaO3/SrTiO3 at 10-1 mbar oxygen background pressure, demonstrating the critical effect of the target-to-substrate distance, dTS, on the interface sheet resistance, Rs. The interface turns from insulating to metallic by progressively decreasing dTS. The analysis of the LaGaO3 plume evidences the important role of the plume propagation dynamics on the interface properties. These results demonstrate the growth of conducting interfaces at an oxygen pressure of 10-1 mbar, an experimental condition where a well-oxygenated heterostructures with a reduced content of oxygen defects is expected. [ABSTRACT FROM AUTHOR]
- Published
- 2012
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5. Publisher's Note: 'Conducting interfaces between band insulating oxides: The LaGaO3/SrTiO3 heterostructure' [Appl. Phys. Lett. 97, 152111 (2010)].
- Author
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Perna, P., Maccariello, D., Radovic, M., Scotti di Uccio, U., Pallecchi, I., Codda, M., Marré, D., Cantoni, C., Gazquez, J., Varela, M., Pennycook, S. J., and Granozio, F. Miletto
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ELECTRIC conductivity ,INTERFACES (Physical sciences) ,ENERGY bands ,ELECTRIC insulators & insulation ,OXIDES ,HETEROSTRUCTURES - Published
- 2010
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6. Synthesis, structure and superconducting properties of laminated thin film composites of YBа2 Cu3 O7–d /Y2 O3 as components of 2G HTS wires
- Author
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Alexander E. Shchukin, Andrey R. Kaul, Alexander L. Vasiliev, and Igor A. Rudnev
- Subjects
Superconductivity ,Materials science ,mocvd ,Heterojunction ,Atomic and Molecular Physics, and Optics ,y2o3 ,Electronic, Optical and Magnetic Materials ,lcsh:Chemistry ,superconductor ,heterostructures ,lcsh:QD1-999 ,ybco ,Materials Chemistry ,buffer layers ,Metalorganic vapour phase epitaxy ,hts ,Physical and Theoretical Chemistry ,Thin film ,Composite material - Abstract
2G HTS wires are capable of transferring huge amounts of electrical energy without loss. An increase in the current-carrying capacity in these materials is possible due to an increase in the thickness of the superconducting layer; however, there is a problem with the appearance of impurity orientations and other defects with increasing thickness. We have proposed a solution of this problem by increasing the thickness of the superconducting layer by the MOCVD method using interlayers of yttrium oxide.The aim of this study was the production of thick composite films with yttrium oxide interlayers and high critical current density. In addition, we want to show the effectiveness of the approach of introducing yttrium oxide interlayers for the reduction of the number of parasitic orientations and defects with an increase in HTS film thickness.The deposition of YBа2Cu3O7–dand Y2O3 films was carried out layer by layer using reel-to-reel MOCVD equipment. A 12 mm wire of the following architecture was used as a substrate: 200 nm CeO2(Gd2O3)/30–50 nm LaMnO3/5–7 nm IBAD-MgO/50 nm LaMnO3/50 nm Al2O3/60 μ Hastelloy 276. The resulting films were annealed in oxygen for obtaining the orthorhombic YBCO phase. YBа2Cu3O7–d/Y2O3composites were obtained. In these composites, obtained using the MOCVD method, the amount of side (с║) orientation of the HTS layer was reduced and high values of the critical current density, exceeding 1 MA/cm at a thickness of > 2 μm remained. The efficiency of the approach of introducing yttrium oxide interlayers for the increase in the current characteristics with increasing film thickness was shown. It was found that further thickening of films with interlayers is prevented by the formation of nanopores, reducing the critical current density. REFERENCES 1. Fleshler S., Buczek D., Carter B., Ogata M. Scaleup of 2G wire manufacturing at American Superconductor Corporation. Physica C. 2009;469(15-20): 1316–1321. https://doi.org/10.1016/j.physc.2009.05.234 2. Nagaishi T., Shingai Y., Konishi M., Taneda T., Ota H., Honda G., Kato T., Ohmatsu K. Development of REBCO coated conductors on textured metallic substrates. Physica C. 2009;469(15-20): 1311–1315. https://doi.org/10.1016/j.physc.2009.05.2533. Rosner C. H. Superconductivity: star technology for the 21st century. IEEE Transactions on Applied Superconductivity. 2001;11(1): 39–48. https://doi.org/10.1109/77.919283 4. Mansour R. R. Microwave superconductivity. IEEE Transactions on Microwave Theory and Techniques. 2002;50(3): 750–759. https://doi.org/10.1109/22.989959 5. Hayakawa H., Yoshikawa N., Yorozu S., Fujimaki A. Superconducting digital electronics. Proceedings of the IEEE. 2004;92(10): 1549–1563. https://doi.org/10.1109/JPROC.2004.8336586. Wimbush S. C. Large scale applications of HTS in New Zealand. Physics Procedia. 2015;65: 221–224. https://doi.org/10.1016/j.phpro.2015.05.1257. Zhu J., Zheng X., Qiu M., Zhang Z., Li J., Yuan W. Application simulation of a resistive type superconducting fault current limiter (SFCL) in a transmission and wind power system. Energy Procedia. 2015;75: 716–721. https://doi.org/10.1016/j.egypro.2015.07.4988. Iwasaki H., Inaba S., Sugioka K., Nozaki Y., Kobayashi N. Superconducting anisotropy in the Y-based system substituted for the Y, Ba and Cu sites. Physica C. 1997;290: 113. https://doi.org/10.1016/S0921-4534(97)00634-59. Freyhardt H. C., Hellstrom E. E. High-temperature superconductors: A Review of YBa2Cu3O6+x and (Bi,Pb)2Sr2Ca2Cu3O10. Cryogenic Engineering. New York:Springer; 2007. pp. 309–339. https://doi.org/10.1007/0-387-46896-X10. Dimos D., Chaudhari P., Mannhart J. Superconducting transport properties of grain boundaries in YBa2Cu3O7bicrystals. Phys. Rev. B. 1990;41: 4038–4049. http://dx.doi.org/10.1103/PhysRevB.41.403811. Goyal A. (ed.) Second-Generation HTS Conductors. Boston/Dordrecht/New York/London: Kluwer Academic Publ.; 2009. 432 p. 12. Zhang H., Yang J., Wang S., Wu Y., Lv Q., Li S. Film thickness dependence of microstructure and superconductive property of PLD prepared YBCO layers. Physica C. 2014;499: 54–56. https://doi.org/10.1016/j.physc.2014.01.00113. Markelov A. V., Samoilenkov S. V., Akbashev A. R., Vasiliev A. L., Kaul A. R. Control of orientation of RBa2Cu3O7films on substrates with low lattice mismatch via seed layer formation. IEEE Transactions on Applied Superconductivity. 2011;21(3): 3066–3069. https://doi.org/10.1109/TASC.2010.210299214. Granozio F. M., Salluzzo M., Scotti di Uccio U., Maggio-Aprile I., Fischer O. Competition between a-axis and c-axis growth in superconducting RBa2Cu3O7−x thin films. Phys. Rev. B. 2000;61(1): 756–765. https://doi.org/10.1103/PhysRevB.61.75615. Jeschke R. Schneider G. Ulmer G. Linker influence of the substrate material on the growth direction of YBaCuO thin films. Physica C. 1995;243: 243–251. https://doi.org/10.1016/0921-4534(95)00019‑416. Moyzykh M., Boytsova O., Amelichev V, Samoilenkov S., Voloshin I., Kaul A., Lacroix B., Paumier F., Gaboriaud R. Effects of yttrium oxide inclusions on the orientation and superconducting properties of YBCO films. Kondensirovannye sredy i mezhfaznye granitsy = Condensed Matter and Interphases. 2013;15(2): 91-98. Available at: http://www.kcmf.vsu.ru/resources/t_15_2_2013_001.pdf17. 2G HTS Wire Specification Overview. Available at: http://www.superpower-inc.com/system/filesSP_2G+Wire+Spec+Sheet_2014_web_v1_0.pdf (accessed 29 October 2016).18. Murakami M., Gotoh S., Fujimoto H., Yamaguchi K., Koshizuka N., Tanaka S. Flux pinning and critical currents in melt processed YBaCuO superconductors. Superconductor Science and Technology . 1991;4: S43–S50. https://doi.org/10.1088/0953-2048/4/1S/00519. Zhao P., Ito A., Goto T. Rapid deposition of YBCO films by laser CVD and effect of lattice mismatch on their epitaxial growth and critical temperature.Ceramics International. 2013;39: 7491–7497. https://doi.org/10.1016/j.ceramint.2013.02.09820. Zhao P., Ito A., Goto T., Tu R. High-speed growth of YBa2Cu3O7−d film with high critical temperature on MgO single crystal substrate by laser chemical vapor deposition. Superconductor Science and Technology. 2010;23(12): 125010. https://doi.org/10.1088/0953-2048/23/12/12501021. Zhao P., Ito A., Goto T., Tu R. Fast epitaxial growth of a-axis- and c-axis-oriented YBa2Cu3O7–dfilms on (1 0 0) LaAlO3substrate by laser chemical vapor deposition. Applied Surface Science. 2010;257: 4317–4320. https://doi.org/10.1016/j.apsusc.2010.12.04722. Hammond R. H., Bormann R. Correlation between the in situ growth conditions of YBCO thin films and the thermodynamic stability criteria. Physica C. 1989;162-164: 703–704. https://doi.org/10.1016/0921-4534(89)91218-5 23. Voronin G. F., Degterov S. A. Solid State Equilibria in the Ba-Cu-O System. J. Solid State Chem. 1994;110(1): 50–57. (and references therein). https://doi.org/10.1006/jssc.1994.113424. Lindemer T. B., Specht E. D. The BaO-Cu-CuO system. Solid-liquid equilibria and thermodynamics of BaCuO2and BaCu2O2. Physica C. 1995;255(1-2): 81–94. (and references therein). https://doi.org/10.1016/0921-4534(95)00460-225. Samoylenkov S. V., Gorbenko O. Yu, Graboy I. E., Kaul A. R., Zandbergen H. W., Connolly E. Secondary phases in (001)RBa2Cu3O7–depitaxial thin films. Chemistry of Materials. 1999:11(9): 2417–2428. https://doi.org/10.1021/cm991016v26. Kaul A. R., Gorbenko O. Yu., Kamenev A. A. The role of heteroepitaxy in the development of new thin film oxide-based functional materials. Russian Chemical Reviews. 2004;73(9): 932–953. https://doi.org/10.1070/RC2004v073n09ABEH00091927. Murakami Y., Goto H., Taguchi Y., Nagasaka Y. Measurement of out-of-plane thermal conductivity of epitaxial YBa2Cu3O7–dthin films in the temperature range from 10 K to 300 K by photothermal reflectance. International Journal of Thermophysics. 2017;38(10): 160. https://doi.org/10.1007/s10765-017-2294-728. Agababov S. G., Vliyanie sherohovatosti poverhnosti tverdogo tela na ego radiatsionnie svoistva I metody ih eksperimentalnogo opredeleniya[Influence of the surface roughness of a solid on its radiation properties and methods of their experimental determination]. Teplofizika visokih temperatur. 1968;6(1): 78–88. (In Russ.)29. Sayapina V. I., Svet D. Ya., Popova О. R., Vliyanie sherohovatosti poverhnosti na izluchatelnuyu sposobnost metallov [Influence of surface roughness on the emissivity of metals]. Teplofizika visokih temperatur. 1972;10(3): 528–535. (In Russ.)30. Mukaida M., Miyazawa S. Nature of preferred orientation of YBa2Cu3Oxthin films. Japanese Journal of Applied Physics. 1993;32(10): 4521–4528. https://doi.org/10.1143/jjap.32.452131. Markelov A. V. The influence of buffer layers on the oriented growth of RBa2Cu3O7–d (R – rare earth element) films and their superconducting characteristics.Thesis of Cand. in Chem. Moscow: MSU (Lomonosov University); 2011. 108р.
- Published
- 2021
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7. Evolution of nanostructures of anatase TiO thin films grown on (001) LaAlO.
- Author
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Ciancio, Regina, Vittadini, Andrea, Selloni, Annabella, Arpaia, Riccardo, Aruta, Carmela, Miletto Granozio, Fabio, Scotti di Uccio, Umberto, Rossi, Giorgio, and Carlino, Elvio
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METALLIC thin films ,TITANIUM dioxide films ,TRANSMISSION electron microscopy ,ELECTRON diffraction ,HETEROSTRUCTURES ,CRYSTALLOGRAPHIC shear ,SCANNING transmission electron microscopy ,SPECTRUM analysis - Abstract
Combining reflection high-energy electron diffraction, high-resolution transmission electron microscopy, and high-angle annular dark field scanning transmission electron microscopy we unveil the existence of a peculiar transition from a three-dimensional to a two-dimensional growth mode in anatase TiO/LaAlO heterostructures. Such a growth dynamics is accompanied by Al interdiffusion from substrate to the growing film up to a critical thickness of 20 nm. With the extra support of ab initio calculations, we show that the crossover between the two growth modes corresponds to the formation of two distinct regions characterized by (103)- and (101)-oriented crystallographic shear superstructures, occurring in the upmost film region and in proximity of the film/substrate interface, respectively. [ABSTRACT FROM AUTHOR]
- Published
- 2013
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8. Design and Manipulation of Ferroic Domains in Complex Oxide Heterostructures.
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Strkalj, Nives, Gradauskaite, Elzbieta, Nordlander, Johanna, and Trassin, Morgan
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HETEROSTRUCTURES ,THIN films ,MULTIFERROIC materials ,ENGINEERING design ,OXIDES - Abstract
The current burst of device concepts based on nanoscale domain-control in magnetically and electrically ordered systems motivates us to review the recent development in the design of domain engineered oxide heterostructures. The improved ability to design and control advanced ferroic domain architectures came hand in hand with major advances in investigation capacity of nanoscale ferroic states. The new avenues offered by prototypical multiferroic materials, in which electric and magnetic orders coexist, are expanding beyond the canonical low-energy-consuming electrical control of a net magnetization. Domain pattern inversion, for instance, holds promises of increased functionalities. In this review, we first describe the recent development in the creation of controlled ferroelectric and multiferroic domain architectures in thin films and multilayers. We then present techniques for probing the domain state with a particular focus on non-invasive tools allowing the determination of buried ferroic states. Finally, we discuss the switching events and their domain analysis, providing critical insight into the evolution of device concepts involving multiferroic thin films and heterostructures. [ABSTRACT FROM AUTHOR]
- Published
- 2019
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9. Conductivity and band alignment of LaCrO3/SrTiO3 (111) heterostructure.
- Author
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Yan-Peng Hong, Xin-Xin Wang, Guo-Liang Qu, Cheng-Jian Li, Hong-Xia Xue, Ke-Jian Liu, Yong-Chun Li, Chang-Min Xiong, Rui-Fen Dou, Lin He, and Jia-Cai Nie
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TITANIUM dioxide nanoparticles ,CHROMIUM oxide ,HETEROSTRUCTURES ,PHOTOELECTRON spectroscopy ,THICKNESS measurement - Abstract
In this work, we investigate the electrical transport property and electronic structure of oxide heterostructure LaCrO
3 /SrTiO3 (111). The interface grown under relatively low oxygen partial pressure is found to be metallic with a conducting critical thickness of 11 unit cells of LaCrO3 . This criticality is also observed by x-ray photoelectron spectroscopy, in which the Ti3+ signal intensity at the spectrum edge of the Ti-2p3/2 core level increases rapidly when the critical thickness is reached. The variations of the valence band offset and full width at half maximum of the core-level spectrum with LaCrO3 thickness suggest that the built-in fields exist both in LaCrO3 and in SrTiO3 . Two possible origins are proposed: the charge transfer from LaCrO3 and the formation of a quantum well in SrTiO3 . Our results shed light on the understanding of the doping mechanism at the polar/non-polar oxide interface. Moreover, due to the interesting lattice and spin structure of LCO in the (111) direction, our work provides a basis for further exploring the novel topological quantum phenomena in this system. [ABSTRACT FROM AUTHOR]- Published
- 2018
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10. Screening mechanisms at polar oxide heterointerfaces.
- Author
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Seungbum Hong, Serge M Nakhmanson, and Dillon D Fong
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ELECTRONIC band structure ,HETEROSTRUCTURES ,OXIDES ,FERROELECTRIC crystals ,POLAR interactions - Abstract
The interfaces of polar oxide heterostructures can display electronic properties unique from the oxides they border, as they require screening from either internal or external sources of charge. The screening mechanism depends on a variety of factors, including the band structure at the interface, the presence of point defects or adsorbates, whether or not the oxide is ferroelectric, and whether or not an external field is applied. In this review, we discuss both theoretical and experimental aspects of different screening mechanisms, giving special emphasis to ways in which the mechanism can be altered to provide novel or tunable functionalities. We begin with a theoretical introduction to the problem and highlight recent progress in understanding the impact of point defects on polar interfaces. Different case studies are then discussed, for both the high thickness regime, where interfaces must be screened and each interface can be considered separately, and the low thickness regime, where the degree and nature of screening can be manipulated and the interfaces are close enough to interact. We end with a brief outlook toward new developments in this rapidly progressing field. [ABSTRACT FROM AUTHOR]
- Published
- 2016
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11. Stability and electronic structure studies of LaAlO3/SrTiO3 (110) heterostructures.
- Author
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Yan-Ling Du, Chun-Lei Wang, Ji-Chao Li, Pan-Pan Xu, Xin-Hua Zhang, Jian Liu, Wen-Bin Su, and Liang-Mo Mei
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ELECTRONIC structure ,HETEROSTRUCTURES ,MAGNETISM ,HIGH temperature superconductivity ,INTERFACE stability - Abstract
The first-principles calculations are employed to investigate the stability, magnetic, and electrical properties of the oxide heterostructure of LaAlO
3 /SrTiO3 (110). By comparing their interface energies, it is obtained that the buckled interface is more stable than the abrupt interface. This result is consistent with experimental observation. At the interface of LaAlO3 /SrTiO3 (110) heterostructure, the Ti—O octahedron distortions cause the Ti t2g orbitals to split into the two-fold degenerate dxz /dyz and nondegenerate dxy orbitals. The former has higher energy than the latter. The partly filled two-fold degenerate t2g orbitals are the origin of two-dimensional electron gas, which is confined at the interface. Lattice mismatch between LaAlO3 and SrTiO3 leads to ferroelectric-like lattice distortions at the interface, and this is the origin of spin-splitting of Ti 3d electrons. Hence the magnetism appears at the interface of LaAlO3 /SrTiO3 (110). [ABSTRACT FROM AUTHOR]- Published
- 2014
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