Novel ABO(3) oxides related to perovskite and YAlO3 structure types in the La-B-V-O (B = Ni, Cu) systems

The synthesis, structure and magnetic properties of mixed-metal oxides of ABO(3) composition in the La-B-V-O (B = Ni, Cu) systems are described in the present paper. While the B = Ni oxides adopt GdFeO3-like perovskite structure containing disordered nickel and vanadium at the octahedral B site, La3Cu2VO9 crystallizes in a YAlO3-type structure. A detailed investigation of the superstructure of nominal La3Cu2VO9 by WDS analysis and Rietveld refinement of powder XRD data reveal that the likely composition of the phase is La13Cu9V4O38.5, where the Cu and V atoms are ordered in a root13a(h) (a(h) = hexagonal a parameter of YAlO3-like subcell) superstructure. Magnetic susceptibility data support the proposed superstructure consisting of triangular Cu-3 clusters. At low temperatures, the magnetic moment corresponds to S = 1/2 per Cu-3 cluster, while at high temperatures the behavior is Curie-Weiss like, showing S = 1/2 per copper. The present work reveals the contrasting behavior of La-Cu-V-O and La-Ni-V-O systems: while a unique line-phase related to YAlO3 structure is formed around La3Cu2VO9 Composition in the copper system, a continuous series of perovskite-GdFeO3 solid solutions, LaNi1-xVxO3 for 0 less than or equal to x less than or equal to 1/3 seems to be obtained in the nickel system, where the oxidation state of nickel varies from 3+ to 2+.

The central region of meso-3,4-diphenylhexane-2,5-dione

As with 1,2-diphenylethane (dpe), X-ray crystallographic methods measure the central bond in meso-3,4-diphenylhexane-2,5-done (dphd) as significantly shorter than normal for an sp(3)-sp(3) bond. The same methods measure the benzylic (ethane C-Ph) bonds in dphd as unusually long for sp(3)-sp(2) liaisons. Torsional motions of the phenyl rings about the C-Ph bonds have been proposed as the artifacts behind the result of a 'short' central bond in dpe. While a similar explanation can, presumably, hold for the even 'shorter' central bond in dphd, it cannot account for the 'long' C-Ph bonds. The phenyl groups, departing much from regular hexagonal shape, adopt highly skewed conformations with respect to the plane constituted by the four central atoms. It is thought that-the thermal motions of the phenyl rings, conditioned by the potential wells in which they are ensconced in the unit cell, are largely libratory around their normal axes. In what appears to be a straightforward explanation under the 'rigid-body' concept, it appears that these libratory motions of the phenyl rings, that account, at the same time, for the 'short' central bond, are the artifacts behind the 'long' measurement of the C-Ph bonds. These motions could be superimposed on torsional motions analogous to those proposed in the case of dpe. An inspection of the ORTEP diagram from the 298 K data on dphd clearly suggests these possibilities. Supportive evidence for these qualitative explanations from an analysis of the differences between the mean square displacements of C(1) and C(7)/C(1a) and C(7a) based on the 'rigid-body model' is discussed. (C) 2002 Elsevier Science B.V. All rights reserved.

Structural and phase dependent thermo and photoluminescent properties of Dy(OH)(3) and Dy2O3 nanorods

Hexagonal Dy(OH)(3) and cubic Dy2O3 nanorods were prepared by hydrothermal method. Dy(OH)(3) nanorods was directly obtained at 180 degrees C for 20 h after hydrothermal treatment whereas subsequently heat treatment at 750 degrees C for 2 h gives pure cubic Dy2O3. SEM micrographs reveal that needle shaped rods with different sizes were observed in both the phases. TEM results also confirm this. The TL response of hexagonal Dy(OH)(3) and cubic Dy2O3 nanorods have been analyzed for gamma-irradiation over a wide range of exposures (1-5 kGy). TL glow peak intensity increases with gamma dose in both the phases. The activation energy (E), order of kinetics (6), and frequency factor (s) for both the phases have been determined using Chen's peak shape method. The simple glow curve shape, structure and linear response to gamma-irradiation over a large span of exposures makes the cubic Dy2O3 as a useful dosimetric material to estimate high exposures of gamma-rays. (c) 2012 Elsevier Ltd. All rights reserved.

Direct hexagonal transition of amorphous (Ge2Sb2Te5)(0.9)Se-0.1 thin films

Ge2Sb2Te5 (GST) is well known for its phase change properties and applications in memory and data storage. Efforts are being made to improve its thermal stability and transition between amorphous and crystalline phases. Various elements are doped to GST to improve these properties. In this work, Se has been doped to GST to study its effect on phase change properties. Amorphous GST film crystallized in to rock salt (NaCl) type structure at 150 degrees C and then transformed to hexagonal structure at 250 degrees C. Interestingly, Se doped GST ((GST)(0.9)Se-0.1) film crystallized directly into hexagonal phase and the intermediate phase of NaCl is not observed. The crystallization temperature (T-c) of (GST)(0.9)Se-0.1 is around 200 degrees C, which is 50 degrees C higher than the T-c of GST. For (GST)(0.9)Se-0.1, the threshold switching occurs at about 4.5V which is higher than GST (3 V). Band gap (E-opt) values of as deposited films are calculated from Tauc plot which are 0.63 eV for GST and 0.66 eV for (GST)(0.9)Se-0.1. The E-opt decreases for the films annealed at higher temperatures. The increased T-c, E-opt, the contrast in resistance and the direct transition to hexagonal phase may improve the data readability and thermal stability in the Se doped GST film. (C) 2014 AIP Publishing LLC.

Robust dielectric properties of B-site size-disordered hexagonal Ln(2)CuTiO(6) (Ln = Y, Dy, Ho, Er, and Yb)

Hexagonal Ln(2)CuTiO(6) (Ln = Y, Dy, Ho, Er, and Yb) exhibits a rare combination of interesting dielectric properties, in the form of relatively large dielectric constants (epsilon' > 30), low losses, and extremely small temperature and frequency dependencies, over large ranges of temperature and frequency Choudhury et al., Appl. Phys. Lett. 96, 162903 (2010) and Choudhury et al., Phys. Rev. B 82, 134203 (2010)], making these compounds promising as high-k dielectric materials. The authors present a brief review of the existing literature on this interesting class of oxides, complimenting it with spectroscopic data in conjunction with first-principles calculation results, revealing a novel mechanism underlying these robust dielectric properties. These show that the large size differences in Cu2+ and Ti4+ at the B-site, aided by an inherent random distribution of CuO5 and TiO5 polyhedral units, frustrates the ferroelectric instability, inherent to the noncentrosymmetric P6(3) cm space group of this system, and gives rise to the observed relatively large dielectric constant values. Additionally, the phononic contributions to the dielectric constant are dominated primarily by mid-frequency (>100 cm(-1)) polar modes, involving mainly Ti4+ 3d(0) ions. In contrast, the soft polar phonon modes with frequencies typically less than 100 cm(-1), usually responsible for dielectric properties of materials, are found to be associated with non-d(0) Cu2+ ions and to contribute very little, giving rise to the remarkable temperature stability of dielectric properties of these compounds. (C) 2014 American Vacuum Society.

Photoluminescence, thermoluminescence and EPR studies of solvothermally derived Ni2+ doped Y(OH)(3) and Y2O3 multi-particle-chain microrods

Rod like structures of hexagonal Y(OH)(3):Ni2+ and cubic Y2O3:Ni2+ phosphors have been successfully synthesized by solvothermal method. X-ray diffraction studies of as-formed product shows hexagonal phase, whereas the product heat treated at 700 degrees C shows pure cubic phase. Scanning electron micrographs (SEM) of Y(OH)(3):Ni2+ show hexagonal rods while Y2O3:Ni2+ rods were found to consist of many nanoparticles stacked together forming multi-particle-chains. EPR studies suggest that the site symmetry around Ni2+ ions is predominantly octahedral. PL spectra show emission in blue, green and red regions due to the T-3(1)(P-3)->(3)A(2)(F-3), T-1(2)(D-1)->(3)A(2)(F-3) and T-1(2)(D-1)-> T-3(2)(F-3) transitions of Ni2+ ions, respectively. TL studies were carried out for Y(OH)(3):Ni2+ and Y2O3:Ni2+ phosphor upon gamma-dose for 1-6 kGy. A single well resolved glow peaks at 195 and 230 degrees C were recorded for Y(OH)(3):Ni2+ and Y2O3:Ni2+, respectively. The glow peak intensity increases linearly up to 4 kGy and 5 kGy for Y(OH)(3):Ni2+ and Y2O3:Ni2+, respectively. The kinetic parameters such as activation energy (E), frequency factor (s) and order of kinetics (b) were estimated by different methods. The phosphor follows simple glow peak structure, linear response with gamma dose, low fading and simple trap distribution, suggesting that it is quite suitable for radiation dosimetry. (C) 2014 Elsevier B.V. All rights reserved.

Synthesis, luminescence properties and EPR investigation of hydrothermally derived uniform ZnO hexagonal rods

One-dimensional (1D) zinc oxide (ZnO) hexagonal rods have been successfully synthesized by surfactant free hydrothermal process at different temperatures. It can be found that the reaction temperature play a crucial role in the formation of ZnO uniform hexagonal rods. The possible formation processes of 1-D ZnO hexagonal rods were investigated. The zinc hydroxide acts as the morphology-formative intermediate for the formation of ZnO nanorods. Upon excitation at 325 nm, the sample prepared at 180 degrees C show several emission bands at 400 nm (similar to 3.10 eV), 420 nm (similar to 2.95 eV), 482 nm (similar to 2.57 eV) and 524 nm (similar to 2.36 eV) corresponding to different kind of defects. TL studies were carried out by pre-irradiating samples with gamma-rays ranging from 1 to 7 kGy at room temperature. A well resolved glow peak at similar to 354 degrees C was recorded which can be ascribed to deep traps. Furthermore, the defects associated with surface states in ZnO nano-structures are characterized by electron paramagnetic resonance. (C) 2014 Elsevier B.V. All rights reserved.

Online_DPI: a web server to calculate the diffraction precision index for a protein structure

An online computing server, Online_DPI (where DPI denotes the diffraction precision index), has been created to calculate the `Cruickshank DPI' value for a given three-dimensional protein or macromolecular structure. It also estimates the atomic coordinate error for all the atoms available in the structure. It is an easy-to-use web server that enables users to visualize the computed values dynamically on the client machine. Users can provide the Protein Data Bank (PDB) identification code or upload the three-dimensional atomic coordinates from the client machine. The computed DPI value for the structure and the atomic coordinate errors for all the atoms are included in the revised PDB file. Further, users can graphically view the atomic coordinate error along with `temperature factors' (i.e. atomic displacement parameters). In addition, the computing engine is interfaced with an up-to-date local copy of the Protein Data Bank. New entries are updated every week, and thus users can access all the structures available in the Protein Data Bank. The computing engine is freely accessible online at http://cluster.physics.iisc.ernet.in/dpi/.

Nonlinear Optical Properties and Temperature-Dependent UV-Vis Absorption and Photoluminescence Emission in 2D Hexagonal Boron Nitride Nanosheets

Recently, a lot of interest has been centred on the optical properties of hexagonal boron nitride (h-BN), which has a similar lattice structure to graphene. Interestingly, h-BN has a wide bandgap and is biocompatible, so it has potential applications in multiphoton bioimaging, if it can exhibit large nonlinear optical (NLO) properties. However, extensive investigation into the NLO properties of h-BN have not been done so far. Here, NLO properties of 2D h-BN nanosheets (BNNS) are reported for the first time, using 1064-nm NIR laser radiation with a pulse duration of 10 ns using the Z-scan technique. The reverse saturable absorption occurs in aqueous colloidal solutions of BNNS with a very large two-photon absorption cross section (sigma(2PA)) of approximate to 57 x 10(-46) cm(4) s(-1) photon(-1). Also, by using UV-Vis absorption spectroscopy, the temperature coefficient of the bandgap (dE(g)/dT) of BNNS is determined to be 5.9 meV K-1. Further defect-induced photoluminescence emission in the UV region is obtained in the 283-303 K temperature range, under excitations of different wavelengths. The present report of large sigma(2PA) combined with stability and biocompatibility could open up new possibilities for the application of BNNS as a potential optical material for multiphoton bioimaging and advanced photonic devices.

Construcción 3. Construcción industrializada

Nivel educativo: Grado. Duración (en horas): Más de 50 horas

4th European Conference on Energy Efficiency and Sustainability in Architecture and Planning : Donostia-San Sebastián, 1-3 Julio 2013

XXXII Cursos de Verano de la UPV/EHU

II Materialen Zientzia eta Teknologia Kongresua. Donostian, 2014 uztailak 3, 4

Egurra, sua; zura, mahaia; larrua, abarka; artila, galtzerdia; burnia, ardatza; altzairua, iltzea; buztina, teila; porlana, pareta; galipota, kaminoa… Materialak, tresnak. Zenbat aldiz aipatuak Euskal Herriko eguneroko berbeta, hizketa eta solasaldi arruntetan! Harria, herria, zioen Aresti poetak ere. Teknologiaren alorrari dagokionean, materialen gaia gehienbat metalurgiarekin lotu izan zen mundu osoan eta batik bat gure herrian. XX. mendearen hasieran garapen industrialak egundoko bultzada izan zuen, bereziki automobilgintzaren eta hegazkingintzaren hedapenarekin. Halaber, elektrizitatea arras zabaldu zelarik, etxetresnen kontzeptua bera ere aldatu egin zen. Horrela, tresna eta baliabide berriek gizartearen ohituren eta izaera beraren aldaketa sakonak erakarri zituzten. Baina, hori guztia material berriak sortu eta garatzeari zor zitzaion: polimeroak, metal eta zeramika berriak, estaldura sintetikoak, etab. ezinbestekoak bilakatu ziren. Orduan ikusi zen materialek arlo berezi bat merezi zutela zientziaren eremuan. Eta horrela, premiak eraginda, Fisika eta Kimika oinarrizko zientzietatik abiatua eta ingeniaritzaren gorpuzkera sendoaz hornituta, Materialen Zientzia sortu zen. Materialen Zientzia eta Teknologia euskaraz, beranduago etorriko zen. Askoz lehenagokoak dira “Pisia” eta “Kimia”, 1935 inguran Jauregi apaiz karmeldar aitzindariak idatzitako liburuak. Eta gero, iluntasunean bidexka ia ezinezkoak jorratuz, Elhuyar Taldea 1972an, Udako Euskal Unibertsitatea 1973an eta UZEI 1977an sortu ziren; euskara irakaskuntzara, unibertsitatera eta zientziara jalgi zedin. Hurrengo urtetan emaitzak gauzatzen hasiak ziren, bai eta Materialen Zientzia eta Teknologiaren arlo berrian ere. Izan ere, mugarria da, besteen artean, Nafarroako Unibertsitateko Donostiako Goi Mailako Injineru Eskolan 1979an Jon Nazabalek aurkeztu zuen “Zenbait mekanizapen errazeko altzairuren berotako erresistentzia mekanikoa eta duktibilitatea” doktoretzatesia. 1991ko uztailean, Udako Euskal Unibertsitateak “Materialen ezagutza teknika ezberdinen bitartez” topaketa antolatu zuen Iruñean, bertan 30en bat zientzialari euskaldun bildu ginelarik. Gaur egun, Euskal Herrian baditugu hainbat ingeniari, fisikari, kimikari eta biologo euskaldun, Materialen Zientzia eta Teknologia garatzen ari direnak, bai unibertsitate, bai zentro teknologiko eta enpresetan. Pertsona horien interesak, ikuspegiak eta lorpenak euskaraz azaltzeko antolatu zen 2012an Arrasaten Materialen Zientzia eta Teknologia I kongresua, ehunen bat pertsona bilduz. Orain dela bi urte hartutako konpromisoari helduz, eta harian haritik jarraituz, aurten Materialen Zientzia eta Teknologia II kongresua UPV/EHUko Polymat institutuak antolatu du. Aldez aurretik, mila esker dagoeneko parte hartzeko izena eman duten guztiei eta gure esker onenak erakunde laguntzaileei: Euskal Herriko Unibertsitatea, Kutxa, CicNanogune eta Elhuyar. Zientziak eta euskarak elkartzen gaituzte. Eta bietan badago elkartze gune bat: kinka larrian daudela beti. Ez baitago zientziarik zientzialariaren zalantzarik gabe, ez eta euskara euskaldun bakoitzaren nahi pertsonalik barik. Antxon Santamaria, Batzorde Antolatzailearen izenean

Odontología preventiva y comunitaria. 3º curso de Odontología. Cuaderno de prácticas preclínicas

La realización de las prácticas preclínicas de odontología preventiva y comunitaria tiene como principal objetivo ser un complemento de las enseñanzas teóricas, y situar al alumno en un escenario sanitario de situaciones y problemáticas asistenciales, comparables a las que podrían presentarse en su ejercicio profesional, contribuyendo a capacitarle, por tanto, para la realización de las prácticas clínicas con pacientes. El adecuado desarrollo de las prácticas deberá permitir al alumno adquirir las siguientes competencias específicas en odontología preventiva y comunitaria: - Recordar y utilizar las normas básicas de funcionamiento en la clínica dental, en el manejo del paciente y las medidas preventivas. - Adquirir los conocimientos, destrezas y actitudes necesarias en la exploración clínica del paciente, así como para el adecuado registro de los datos derivados de la misma. - Explicar y realizar los principales métodos para el control, la prevención de las enfermedades orales y la promoción de la salud oral. - Interpretar los datos clínicos, radiológicos y complementarios, y construir un planteamiento diagnóstico, pronóstico y terapéutico del estado de salud buco-dental a nivel individual y comunitario. - Planificar, realizar y evaluar programas de asistencia sanitaria, de prevención y de promoción de la salud en la comunidad recordando la necesidad de la coordinación interinstitucional e interprofesional. - Capacidad de organización, análisis, síntesis y razonamiento crítico para la toma de decisiones y resolución de problemas.

Turbomáquinas térmicas: 1. Turbomáquinas térmicas. 2. Estudio y diseño de turbinas de gas. 3. Problemas

Contenido: - Instalaciones de turbina de gas. - Análisis de los procesos termodinámicos. - Conceptos básicos para el análisis de turbinas de gas: a) Instalación de turbina de gas. b) Turbina como máquina térmica. - Análisis mediante el software Turgas.