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Dive into the research topics where Despoina M. Kepaptsoglou is active.

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Featured researches published by Despoina M. Kepaptsoglou.


Nano Letters | 2013

Ion implantation of graphene-toward IC compatible technologies.

Ursel Bangert; W. Pierce; Despoina M. Kepaptsoglou; Quentin M. Ramasse; R. Zan; Mhairi Gass; J. A. van den Berg; C. B. Boothroyd; J. Amani; H. Hofsäss

Doping of graphene via low energy ion implantation could open possibilities for fabrication of nanometer-scale patterned graphene-based devices as well as for graphene functionalization compatible with large-scale integrated semiconductor technology. Using advanced electron microscopy/spectroscopy methods, we show for the first time directly that graphene can be doped with B and N via ion implantation and that the retention is in good agreement with predictions from calculation-based literature values. Atomic resolution high-angle dark field imaging (HAADF) combined with single-atom electron energy loss (EEL) spectroscopy reveals that for sufficiently low implantation energies ions are predominantly substitutionally incorporated into the graphene lattice with a very small fraction residing in defect-related sites.


ACS Nano | 2014

Thickness-dependent crossover from charge- to strain-mediated magnetoelectric coupling in ferromagnetic/piezoelectric oxide heterostructures.

Steven R. Spurgeon; Jennifer D. Sloppy; Despoina M. Kepaptsoglou; Prasanna V. Balachandran; Siamak Nejati; J. Karthik; Anoop R. Damodaran; Craig L. Johnson; Hailemariam Ambaye; Richard Goyette; Valeria Lauter; Quentin M. Ramasse; Juan Carlos Idrobo; Kenneth K. S. Lau; Samuel E. Lofland; James M. Rondinelli; Lane W. Martin; Mitra L. Taheri

Magnetoelectric oxide heterostructures are proposed active layers for spintronic memory and logic devices, where information is conveyed through spin transport in the solid state. Incomplete theories of the coupling between local strain, charge, and magnetic order have limited their deployment into new information and communication technologies. In this study, we report direct, local measurements of strain- and charge-mediated magnetization changes in the La0.7Sr0.3MnO3/PbZr0.2Ti0.8O3 system using spatially resolved characterization techniques in both real and reciprocal space. Polarized neutron reflectometry reveals a graded magnetization that results from both local structural distortions and interfacial screening of bound surface charge from the adjacent ferroelectric. Density functional theory calculations support the experimental observation that strain locally suppresses the magnetization through a change in the Mn-eg orbital polarization. We suggest that this local coupling and magnetization suppression may be tuned by controlling the manganite and ferroelectric layer thicknesses, with direct implications for device applications.


Nature Communications | 2015

Polarization screening-induced magnetic phase gradients at complex oxide interfaces

Steven R. Spurgeon; Prasanna V. Balachandran; Despoina M. Kepaptsoglou; Anoop R. Damodaran; J. Karthik; Siamak Nejati; Lewys Jones; Haile Ambaye; Valeria Lauter; Quentin M. Ramasse; Kenneth K. S. Lau; Lane W. Martin; James M. Rondinelli; Mitra L. Taheri

Thin-film oxide heterostructures show great potential for use in spintronic memories, where electronic charge and spin are coupled to transport information. Here we use a La0.7Sr0.3MnO3 (LSMO)/PbZr0.2Ti0.8O3 (PZT) model system to explore how local variations in electronic and magnetic phases mediate this coupling. We present direct, local measurements of valence, ferroelectric polarization and magnetization, from which we map the phases at the LSMO/PZT interface. We combine these experimental results with electronic structure calculations to elucidate the microscopic interactions governing the interfacial response of this system. We observe a magnetic asymmetry at the LSMO/PZT interface that depends on the local PZT polarization and gives rise to gradients in local magnetic moments; this is associated with a metal-insulator transition at the interface, which results in significantly different charge-transfer screening lengths. This study establishes a framework to understand the fundamental asymmetries of magnetoelectric coupling in oxide heterostructures.


Nanotechnology | 2013

Factors that determine and limit the resistivity of high-quality individual ZnO nanowires

Alex M. Lord; Thierry G.G. Maffeis; Alex S. Walton; Despoina M. Kepaptsoglou; Quentin M. Ramasse; Michael B. Ward; Jürgen Köble; Steve P. Wilks

Knowing and controlling the resistivity of an individual nanowire (NW) is crucial for the production of new sensors and devices. For ZnO NWs this is poorly understood; a 10(8) variation in resistivity has previously been reported, making the production of reproducible devices almost impossible. Here, we provide accurate resistivity measurements of individual NWs, using a four-probe scanning tunnelling microscope (STM), revealing a dependence on the NW dimensions. To correctly interpret this behaviour, an atomic level transmission electron microscopy technique was employed to study the structural properties of the NWs in relation to three growth techniques: hydrothermal, catalytic and non-catalytic vapour phase. All NWs were found to be defect free and structurally equivalent; those grown with a metallic catalyst were free from Au contamination. The resistivity measurements showed a distinct increase with decreasing NW diameter, independent of growth technique. The increasing resistivity at small NW diameters was attributed to the dominance of surface states removing electrons from the bulk. However, a fundamental variance in resistivity (10(2)) was observed and attributed to changes in occupied surface state density, an effect which is not seen with other NW materials such as Si. This is examined by a model to predict the effect of surface state occupancy on the measured resistivity and is confirmed with measurements after passivating the ZnO surface. Our results provide an understanding of the primary influence of the reactive nature of the surface and its dramatic effect on the electrical properties of ZnO NWs.


Nano Letters | 2015

Controlling the Electrical Transport Properties of Nanocontacts to Nanowires

Alex M. Lord; Thierry G.G. Maffeis; Olga Kryvchenkova; R. J. Cobley; K. Kalna; Despoina M. Kepaptsoglou; Quentin M. Ramasse; Alex S. Walton; Michael B. Ward; Jürgen Köble; Steve P. Wilks

The ability to control the properties of electrical contacts to nanostructures is essential to realize operational nanodevices. Here, we show that the electrical behavior of the nanocontacts between free-standing ZnO nanowires and the catalytic Au particle used for their growth can switch from Schottky to Ohmic depending on the size of the Au particles in relation to the cross-sectional width of the ZnO nanowires. We observe a distinct Schottky to Ohmic transition in transport behavior at an Au to nanowire diameter ratio of 0.6. The current-voltage electrical measurements performed with a multiprobe instrument are explained using 3-D self-consistent electrostatic and transport simulations revealing that tunneling at the contact edge is the dominant carrier transport mechanism for these nanoscale contacts. The results are applicable to other nanowire materials such as Si, GaAs, and InAs when the effects of surface charge and contact size are considered.


Advanced Materials Interfaces | 2016

Interface-Induced Polarization in SrTiO3-LaCrO3 Superlattices

Ryan Comes; Steven R. Spurgeon; Steve M. Heald; Despoina M. Kepaptsoglou; Lewys Jones; Phuong Vu Ong; Mark E. Bowden; Quentin M. Ramasse; Peter V. Sushko; Scott A. Chambers

Epitaxial interfaces and superlattices comprised of polar and non-polar perovskite oxides have generated considerable interest because they possess a range of desirable properties for functional devices. In this work, emergent polarization in superlattices of SrTiO


Energy and Environmental Science | 2018

Effect of composition on the structure of lithium- and manganese-rich transition metal oxides

Alpesh K. Shukla; Quentin M. Ramasse; Colin Ophus; Despoina M. Kepaptsoglou; Fredrik S. Hage; Christoph Gammer; Charles Bowling; Pedro Alejandro Hern andez Gallegos; Subramanian Venkatachalam

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Materials Science Forum | 2014

Atomic-Resolution Elemental Mapping of Precipitates in a 7449 Aluminium Alloy

Sigurd Wenner; Calin Daniel Marioara; W. Lefebvre; Quentin M. Ramasse; Despoina M. Kepaptsoglou; Fredrik S. Hage; Randi Holmestad

(STO) and LaCrO


Journal of Physics: Condensed Matter | 2018

Magnetic and structural depth profiles of Heusler alloy Co2FeAl0.5Si0.5 epitaxial films on Si(1 1 1)

Stephanie E. Glover; Thomas Saerbeck; Balati Kuerbanjiang; Arsham Ghasemi; Despoina M. Kepaptsoglou; Quentin M. Ramasse; Shinya Yamada; Kohei Hamaya; Thomas P. A. Hase; Vlado K. Lazarov; Gavin R. Bell

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Nano Letters | 2017

Modifying the Interface Edge to Control the Electrical Transport Properties of Nanocontacts to Nanowires

Alex M. Lord; Quentin M. Ramasse; Despoina M. Kepaptsoglou; Jonathan E. Evans; Philip Rosser Davies; Michael B. Ward; Steve P. Wilks

(LCO) is demonstrated. By controlling the interfaces between polar LCO and non-polar STO, polarization is induced throughout the STO layers of the superlattice. Using x-ray absorption near-edge spectroscopy and aberration-corrected scanning transmission electron microscopy displacements of the Ti cations off-center within TiO6 octahedra along the superlattice growth direction are measured. This distortion gives rise to built-in potential gradients within the STO and LCO layers, as measured by in situ x-ray photoelectron spectroscopy. Density functional theory models explain the mechanisms underlying this behavior, revealing the existence of both an intrinsic polar distortion and a built-in electric field, which are due to alternately positively and negatively charged interfaces in the superlattice. This study paves the way for controllable polarization for carrier separation in multilayer materials and highlights the crucial role that interface structure plays in governing such behavior.

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Steven R. Spurgeon

Pacific Northwest National Laboratory

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Peter V. Sushko

Pacific Northwest National Laboratory

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