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Search for "X-ray spectroscopy" in Full Text gives 194 result(s) in Beilstein Journal of Nanotechnology.

A single-source precursor route to anisotropic halogen-doped zinc oxide particles as a promising candidate for new transparent conducting oxide materials

  • Daniela Lehr,
  • Markus R. Wagner,
  • Johanna Flock,
  • Julian S. Reparaz,
  • Clivia M. Sotomayor Torres,
  • Alexander Klaiber,
  • Thomas Dekorsy and
  • Sebastian Polarz

Beilstein J. Nanotechnol. 2015, 6, 2161–2172, doi:10.3762/bjnano.6.222

Graphical Abstract
  • selected-area energy dispersive X-ray spectroscopy (EDX) (Figure 2b) and X-ray photoelectron spectroscopy (Figure 2c). The maximum concentration of Cl in the ZnO lattice we could reach via this method is 3.6 atom % (≡ZnO0.964Cl0.036). The low chlorine values compared to the molecular precursor shows that
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Published 18 Nov 2015

Paramagnetism of cobalt-doped ZnO nanoparticles obtained by microwave solvothermal synthesis

  • Jacek Wojnarowicz,
  • Sylwia Kusnieruk,
  • Tadeusz Chudoba,
  • Stanislaw Gierlotka,
  • Witold Lojkowski,
  • Wojciech Knoff,
  • Malgorzata I. Lukasiewicz,
  • Bartlomiej S. Witkowski,
  • Anna Wolska,
  • Marcin T. Klepka,
  • Tomasz Story and
  • Marek Godlewski

Beilstein J. Nanotechnol. 2015, 6, 1957–1969, doi:10.3762/bjnano.6.200

Graphical Abstract
  • -ray absorption fine structure (EXAFS) spectroscopy, scanning electron microscopy (SEM), energy dispersive X-ray spectroscopy (EDS) and with magnetometry using superconducting quantum interference device (SQUID). Irrespective of the Co content, nanoparticles in their initial state present a similar
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Published 30 Sep 2015

Optimized design of a nanostructured SPCE-based multipurpose biosensing platform formed by ferrocene-tethered electrochemically-deposited cauliflower-shaped gold nanoparticles

  • Wicem Argoubi,
  • Maroua Saadaoui,
  • Sami Ben Aoun and
  • Noureddine Raouafi

Beilstein J. Nanotechnol. 2015, 6, 1840–1852, doi:10.3762/bjnano.6.187

Graphical Abstract
  • employed to perform the electrochemical experiments. Each SPCE comprises of a 3 mm disk used as a carbon working electrode, a printed Ag/AgCl reference electrode and a carbon counter-electrode. SEM micrographs and energy-dispersive X-ray spectroscopy (EDX) analysis were recorded using a FEI Quanta 650 FEG
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Published 01 Sep 2015

Possibilities and limitations of advanced transmission electron microscopy for carbon-based nanomaterials

  • Xiaoxing Ke,
  • Carla Bittencourt and
  • Gustaaf Van Tendeloo

Beilstein J. Nanotechnol. 2015, 6, 1541–1557, doi:10.3762/bjnano.6.158

Graphical Abstract
  • , different from optical microscopes, accelerated electrons carry high energy and interact with the material in a highly dynamic manner. Elastically scattered electrons, inelastically scattered electrons (for electron energy loss spectroscopy, i.e., EELS) and X-rays (for energy dispersive X-ray spectroscopy
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Published 16 Jul 2015

Influence of the shape and surface oxidation in the magnetization reversal of thin iron nanowires grown by focused electron beam induced deposition

  • Luis A. Rodríguez,
  • Lorenz Deen,
  • Rosa Córdoba,
  • César Magén,
  • Etienne Snoeck,
  • Bert Koopmans and
  • José M. De Teresa

Beilstein J. Nanotechnol. 2015, 6, 1319–1331, doi:10.3762/bjnano.6.136

Graphical Abstract
  • decreased to the range from 3 × 10−6 to 4 × 10−6 mbar, the deposits did not show the granular structure and the magnetization reversal was found to be dominated by shape anisotropy (see next section). In situ compositional analysis by energy dispersive X-ray spectroscopy (EDS) indicated that the Fe content
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Published 15 Jun 2015

Structural transitions in electron beam deposited Co–carbonyl suspended nanowires at high electrical current densities

  • Gian Carlo Gazzadi and
  • Stefano Frabboni

Beilstein J. Nanotechnol. 2015, 6, 1298–1305, doi:10.3762/bjnano.6.134

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  • was performed with a JEOL 2010 microscope, equipped with energy dispersive X-ray spectroscopy (EDX) system (Oxford INCA 100) for composition analysis. Results and Discussion In Figure 1a, an example of Co–carbonyl SNW deposited by FEBID is shown. The suspended wire is deposited across the slit and
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Published 11 Jun 2015

Growth and morphological analysis of segmented AuAg alloy nanowires created by pulsed electrodeposition in ion-track etched membranes

  • Ina Schubert,
  • Loic Burr,
  • Christina Trautmann and
  • Maria Eugenia Toimil-Molares

Beilstein J. Nanotechnol. 2015, 6, 1272–1280, doi:10.3762/bjnano.6.131

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  • length in ion-track etched polymer templates was developed. Detailed analysis by cyclic voltammetry in ion-track membranes, energy-dispersive X-ray spectroscopy and scanning electron microscopy was performed to determine the dependency between the chosen potential and the segment composition
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Published 08 Jun 2015

Electrocatalysis on the nm scale

  • R. Jürgen Behm

Beilstein J. Nanotechnol. 2015, 6, 1008–1009, doi:10.3762/bjnano.6.103

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  • pushed by the rapid development of modern in situ spectroscopy and microscopy tools, such as in situ vibrational spectroscopy, in situ X-ray spectroscopy/diffraction, and in situ scanning probe microscopy, just to name a few, as well as the enormous progress that has been made in the theoretical
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Published 21 Apr 2015

Electron-stimulated purification of platinum nanostructures grown via focused electron beam induced deposition

  • Brett B. Lewis,
  • Michael G. Stanford,
  • Jason D. Fowlkes,
  • Kevin Lester,
  • Harald Plank and
  • Philip D. Rack

Beilstein J. Nanotechnol. 2015, 6, 907–918, doi:10.3762/bjnano.6.94

Graphical Abstract
  • ]. Consistent with the energy dispersive X-ray spectroscopy (EDS) measurements, the measured thickness versus time (Figure 2b) reveals an approximately linear purification rate (R2 value of 0.97). The thickness of the pad after 2 and 4 min of purification shown on the plot is included for completeness, but the
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Published 08 Apr 2015

Nanostructuring of GeTiO amorphous films by pulsed laser irradiation

  • Valentin S. Teodorescu,
  • Cornel Ghica,
  • Adrian V. Maraloiu,
  • Mihai Vlaicu,
  • Andrei Kuncser,
  • Magdalena L. Ciurea,
  • Ionel Stavarache,
  • Ana M. Lepadatu,
  • Nicu D. Scarisoreanu,
  • Andreea Andrei,
  • Valentin Ion and
  • Maria Dinescu

Beilstein J. Nanotechnol. 2015, 6, 893–900, doi:10.3762/bjnano.6.92

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  • annular dark field (STEM-HAADF) imaging and energy-dispersive X-ray spectroscopy (EDX). The estimation of the film surface temperature was performed by using the Heat Flow software [24]. Results A quasi-coherent wave relief with a periodicity of about 200 nm and 10 nm amplitude was observed on the surface
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Published 07 Apr 2015

Low-cost formation of bulk and localized polymer-derived carbon nanodomains from polydimethylsiloxane

  • Juan Carlos Castro Alcántara,
  • Mariana Cerda Zorrilla,
  • Lucia Cabriales,
  • Luis Manuel León Rossano and
  • Mathieu Hautefeuille

Beilstein J. Nanotechnol. 2015, 6, 744–748, doi:10.3762/bjnano.6.76

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  • has been clearly identified by the presence of fluorescent compounds inside the channels. The composition of the combustion residues has been characterized first with a NORAN energy dispersive X-ray spectroscopy (EDX) system working at 20 keV in a scanning electron microscope (Jeol JSM-5600LV). The
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Published 16 Mar 2015

Overview of nanoscale NEXAFS performed with soft X-ray microscopes

  • Peter Guttmann and
  • Carla Bittencourt

Beilstein J. Nanotechnol. 2015, 6, 595–604, doi:10.3762/bjnano.6.61

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  • nanostructures needs spatial resolution in the nanoscale range together with X-ray spectroscopy methods. X-ray microscopy reaches a higher Rayleigh resolution than optical microscopy as the resolution is decreasing linear with the wavelength. Additionally, the larger penetration depth and smaller radiation
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Published 27 Feb 2015

Multifunctional layered magnetic composites

  • Maria Siglreitmeier,
  • Baohu Wu,
  • Tina Kollmann,
  • Martin Neubauer,
  • Gergely Nagy,
  • Dietmar Schwahn,
  • Vitaliy Pipich,
  • Damien Faivre,
  • Dirk Zahn,
  • Andreas Fery and
  • Helmut Cölfen

Beilstein J. Nanotechnol. 2015, 6, 134–148, doi:10.3762/bjnano.6.13

Graphical Abstract
  • distribution of magnetite nanoparticles inside the hybrid material was determined with electron dispersive X-ray spectroscopy (EDX) (Figure 4d). The mapping of the elements shows that Fe and C are homogeneously distributed throughout the material surface whereas there is less C detected at the freshly broken
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Published 12 Jan 2015

Interaction of dermatologically relevant nanoparticles with skin cells and skin

  • Annika Vogt,
  • Fiorenza Rancan,
  • Sebastian Ahlberg,
  • Berouz Nazemi,
  • Chun Sik Choe,
  • Maxim E. Darvin,
  • Sabrina Hadam,
  • Ulrike Blume-Peytavi,
  • Kateryna Loza,
  • Jörg Diendorf,
  • Matthias Epple,
  • Christina Graf,
  • Eckart Rühl,
  • Martina C. Meinke and
  • Jürgen Lademann

Beilstein J. Nanotechnol. 2014, 5, 2363–2373, doi:10.3762/bjnano.5.245

Graphical Abstract
  • spectroscopic data. Following similar approaches, Adachi et al. performed transmission electron microscopy (TEM) and energy dispersive X-ray spectroscopy (EDX) measurements on murine skin after up to 8 weeks of daily sunscreen application with similar results [10]. However, a loss of particles during fixation
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Published 08 Dec 2014

PVP-coated, negatively charged silver nanoparticles: A multi-center study of their physicochemical characteristics, cell culture and in vivo experiments

  • Sebastian Ahlberg,
  • Alexandra Antonopulos,
  • Jörg Diendorf,
  • Ralf Dringen,
  • Matthias Epple,
  • Rebekka Flöck,
  • Wolfgang Goedecke,
  • Christina Graf,
  • Nadine Haberl,
  • Jens Helmlinger,
  • Fabian Herzog,
  • Frederike Heuer,
  • Stephanie Hirn,
  • Christian Johannes,
  • Stefanie Kittler,
  • Manfred Köller,
  • Katrin Korn,
  • Wolfgang G. Kreyling,
  • Fritz Krombach,
  • Jürgen Lademann,
  • Kateryna Loza,
  • Eva M. Luther,
  • Marcelina Malissek,
  • Martina C. Meinke,
  • Daniel Nordmeyer,
  • Anne Pailliart,
  • Jörg Raabe,
  • Fiorenza Rancan,
  • Barbara Rothen-Rutishauser,
  • Eckart Rühl,
  • Carsten Schleh,
  • Andreas Seibel,
  • Christina Sengstock,
  • Lennart Treuel,
  • Annika Vogt,
  • Katrin Weber and
  • Reinhard Zellner

Beilstein J. Nanotechnol. 2014, 5, 1944–1965, doi:10.3762/bjnano.5.205

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  • (TEM), this technique requires thin samples and, hence, slicing of the samples as well as additional staining, which both might change the properties of the samples. Furthermore, energy dispersive X-ray spectroscopy (EDX) combined with TEM has only limited spectral and spatial resolution and
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Published 03 Nov 2014

Electronic and electrochemical doping of graphene by surface adsorbates

  • Hugo Pinto and
  • Alexander Markevich

Beilstein J. Nanotechnol. 2014, 5, 1842–1848, doi:10.3762/bjnano.5.195

Graphical Abstract
  • in this case is the reaction in Equation 1. The water molecules required for the reaction are assumed to be located at the graphene/SiO2 interface. Indeed, the presence of water layers on the surface of SiO2 films grown on Si has been confirmed by Kelvin probe microscopy, X-ray spectroscopy and FTIR
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Published 23 Oct 2014

Nanocrystalline ceria coatings on solid oxide fuel cell anodes: the role of organic surfactant pretreatments on coating microstructures and sulfur tolerance

  • Chieh-Chun Wu,
  • Ling Tang and
  • Mark R. De Guire

Beilstein J. Nanotechnol. 2014, 5, 1712–1724, doi:10.3762/bjnano.5.181

Graphical Abstract
  • measured by using energy-dispersive X-ray spectroscopy (EDXS).) The NiO particles ranged in size from 0.5 to 1.5 μm and had faceted, polygonal faces (Figure 5a). The GDC particles were more rounded; many were sintered agglomerates ca. 3 μm long and ca. 1 μm wide. Direct-treated ceria coatings (treatment 2
  • carefully peeled from the electrodes before analysis. Cell characterization Scanning electron microscope (SEM) images of the anodes were taken (FEI xT Nova Nanolab) at 5 kV accelerating voltage. Energy-dispersive X-ray spectroscopy (EDXS) mapping at beam energy of 15 keV, combined with SEM images, was used
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Published 06 Oct 2014

Ionic liquid-assisted formation of cellulose/calcium phosphate hybrid materials

  • Ahmed Salama,
  • Mike Neumann,
  • Christina Günter and
  • Andreas Taubert

Beilstein J. Nanotechnol. 2014, 5, 1553–1568, doi:10.3762/bjnano.5.167

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  • -14476 Potsdam, Germany 10.3762/bjnano.5.167 Abstract Cellulose/calcium phosphate hybrid materials were synthesized via an ionic liquid-assisted route. Scanning electron microscopy, transmission electron microscopy, energy-dispersive X-ray spectroscopy, X-ray diffraction, infrared spectroscopy, and
  • (Plano GmbH). Samples were cut at 1 mm/s at room temperature. Energy dispersive X-ray spectroscopy was done on a JEOL JSM 6510 SEM with tungsten hairpin filament (15 kV) and an Oxford INCAx-act SN detector with a resolution of 135 eV at 5.9 keV. Elemental analysis was done on a Vario EL III analyzer
  • summarizes data obtained from energy dispersive X-ray spectroscopy (EDXS). The samples grown in the presence of GAA have a Ca/P ratio of 0.8 to 0.9. This is on the order of the Ca/P ratio of 1 in stoichiometric DCPD or DCPA [12][13][56]. Moreover, CPGAA24 also contains roughly equivalent amounts of sodium
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Published 16 Sep 2014

Growth evolution and phase transition from chalcocite to digenite in nanocrystalline copper sulfide: Morphological, optical and electrical properties

  • Priscilla Vasthi Quintana-Ramirez,
  • Ma. Concepción Arenas-Arrocena,
  • José Santos-Cruz,
  • Marina Vega-González,
  • Omar Martínez-Alvarez,
  • Víctor Manuel Castaño-Meneses,
  • Laura Susana Acosta-Torres and
  • Javier de la Fuente-Hernández

Beilstein J. Nanotechnol. 2014, 5, 1542–1552, doi:10.3762/bjnano.5.166

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  • were made by applying a potential of 1 V at the sample: 20 s in darkness, 50 s under illumination and another 50 s in darkness. For this, two rectangular metallic contacts (0.5 × 0.2 cm) were painted on the surface of the films with silver paint in a square sample of 0.5 cm2. Energy dispersive X-ray
  • spectroscopy (EDS) was carried out in a JSM-6060LV SEM at 20 keV by using KBr pellets containing granules of CuxS powder to make the punctual analysis. X-ray patterns of copper sulfide synthesized in organic solution at a) 230 and 220 °C, the chalcocite phase is obtained and at b) 240 and 260 °C, the
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Published 15 Sep 2014

Probing the electronic transport on the reconstructed Au/Ge(001) surface

  • Franciszek Krok,
  • Mark R. Kaspers,
  • Alexander M. Bernhart,
  • Marek Nikiel,
  • Benedykt R. Jany,
  • Paulina Indyka,
  • Mateusz Wojtaszek,
  • Rolf Möller and
  • Christian A. Bobisch

Beilstein J. Nanotechnol. 2014, 5, 1463–1471, doi:10.3762/bjnano.5.159

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  • a gas injection system by the electron beam and the FIB beam was used to cut out the lamella. The high resolution (HR) TEM and high angle annular dark field (HAADF) scanning TEM images together with energy dispersive X-ray spectroscopy (EDX) analysis of the sample were obtained by the FEI Tecnai
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Published 05 Sep 2014

Synthesis, characterization, and growth simulations of Cu–Pt bimetallic nanoclusters

  • Subarna Khanal,
  • Ana Spitale,
  • Nabraj Bhattarai,
  • Daniel Bahena,
  • J. Jesus Velazquez-Salazar,
  • Sergio Mejía-Rosales,
  • Marcelo M. Mariscal and
  • Miguel José-Yacaman

Beilstein J. Nanotechnol. 2014, 5, 1371–1379, doi:10.3762/bjnano.5.150

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  • the average diameter of the Cu–Pt nanoclusters is 3.0 ± 1.0 nm. The high angle annular dark field (HAADF-STEM) images, intensity profiles, and energy dispersive X-ray spectroscopy (EDX) line scans, allowed us to study the distribution of Cu and Pt with atomistic resolution, finding that Pt is embedded
  • –Pt clusters; energy dispersive X-ray spectroscopy (EDX); grand-canonical Langevin dynamics; nanoalloys; scanning transmission electron microscopy (STEM); Introduction The study of bimetallic (BM) nanoclusters has received particular interest because of their myriad properties and applications in
  • ) techniques. The use of high angle annular dark field (HAADF-STEM) images, intensity profiles, and energy dispersive X-ray spectroscopy (EDX) line scans, allowed us to study the atomic positions of Cu and Pt, and to compare the structure of the particles with the results of atomistic simulations. We applied a
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Published 27 Aug 2014

Magnesium batteries: Current state of the art, issues and future perspectives

  • Rana Mohtadi and
  • Fuminori Mizuno

Beilstein J. Nanotechnol. 2014, 5, 1291–1311, doi:10.3762/bjnano.5.143

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  • operando soft X-ray spectroscopy. Their results, combined with the transport properties of the magnesium species, also suggested the interfacial electroactive species to be MgCl+·5THF. The dimeric Mg2Cl3+ species present in the bulk, was discounted from being electrochemically active at the interface
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Published 18 Aug 2014

Electron-beam induced deposition and autocatalytic decomposition of Co(CO)3NO

  • Florian Vollnhals,
  • Martin Drost,
  • Fan Tu,
  • Esther Carrasco,
  • Andreas Späth,
  • Rainer H. Fink,
  • Hans-Peter Steinrück and
  • Hubertus Marbach

Beilstein J. Nanotechnol. 2014, 5, 1175–1185, doi:10.3762/bjnano.5.129

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  • -dispersive X-ray spectroscopy (EDX) [23][24][25]. The composition is almost independent of the applied beam current and energy, apart from a slight increase in oxygen content for increasing beam power [23]. The deposition yield decreases for higher electron energy, and increases strongly above 403 K
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Published 30 Jul 2014

Optimizing the synthesis of CdS/ZnS core/shell semiconductor nanocrystals for bioimaging applications

  • Li-wei Liu,
  • Si-yi Hu,
  • Ying Pan,
  • Jia-qi Zhang,
  • Yue-shu Feng and
  • Xi-he Zhang

Beilstein J. Nanotechnol. 2014, 5, 919–926, doi:10.3762/bjnano.5.105

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  • redshift of about 45–55 nm for CdS/ZnS QDs. This is due to the quantum confinement. CdS/ZnS QDs were further characterized by energy dispersive X-ray spectroscopy (EDX), as shown in Figure 3. The spectra exhibit the composition of the CdS/ZnS QDs and indicating Cd, S, and Zn as components of the CdS/ZnS
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Published 27 Jun 2014

Enhanced photocatalytic activity of Ag–ZnO hybrid plasmonic nanostructures prepared by a facile wet chemical method

  • Sini Kuriakose,
  • Vandana Choudhary,
  • Biswarup Satpati and
  • Satyabrata Mohapatra

Beilstein J. Nanotechnol. 2014, 5, 639–650, doi:10.3762/bjnano.5.75

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  • square of the atomic number Z. Figure 3c shows the STEM-HAADF image of ZnO nanostructures in sample PZ. Energy dispersive X-ray spectroscopy (EDX) data from the regions marked by area 1 in Figure 3c and area 2 in Figure 4c is plotted in Figure 3d for ZnO and Ag–ZnO. The C and Cu signals in the EDX
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Published 15 May 2014
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