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Metal Interface (metal + interface)
Selected AbstractsAnomalous current,voltage characteristics of thin polymer filmsPHYSICA STATUS SOLIDI (A) APPLICATIONS AND MATERIALS SCIENCE, Issue 2 2003V. A. Kolesnikov Abstract In this paper we have investigated organic light emitting diodes with such electroluminescent materials as aromatic polyimide, poly,N-vinylcarbazole (PVK) and dye doped PVK. N-type current,voltage characteristics with negative differential resistance for the thin polymeric and organic films are analyzed. No reasonable explanation has been provided for this phenomenon until now. Here we suggest that a polymer(organic)/metal interface containing various inhomogeneities and metal spikes is responsible for this effect. We detect also the black-body radiation, whose temperature exceeds both the melting point and the sublimation temperature of the metal of the electrode. We suppose that the current density through the spike in any cases is large enough to cause the explosion of the tip of the spike and the detected radiation has the hot plasma origin. (© 2003 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [source] Stability of surface waves at magnetized plasma , metal interfaceCONTRIBUTIONS TO PLASMA PHYSICS, Issue 7 2003Yu. A. Akimov Abstract The stability of high-frequency potential surface waves at a dense magnetized plasma , metal interface with respect to a low-frequency plasma density modulation is studied in the point of view of the surface waves control. The discussion is addressed to the situation, when an external steady magnetic field is directed perpendicularly to the interface. The nonlinear interaction process of the high-frequency surface wave, its satellites and the low-frequency plasma density perturbation is investigated. It is shown that the low-frequency plasma density perturbation can be represented as a superposition of forced waves of surface and volume types and can lead to an additional attenuation of the surface waves. This attenuation arises when the surface wave amplitude exceeds the threshold value. (© 2003 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [source] Femtosecond dynamics of electron transfer, localization, and solvation processes at the ice,metal interfaceISRAEL JOURNAL OF CHEMISTRY, Issue 1-2 2005Uwe Bovensiepen The ultrafast dynamics of excess electrons in amorphous ice layers on single-crystal metal surfaces are investigated by femtosecond time- and angle-resolved two-photon-photoemission spectroscopy. Photoexcited electrons are injected from the metal substrate into delocalized states of the conduction band of ice and localize in the ice layer within 100 fs. Subsequently, energetic stabilization of this localized species is observed on a time scale of ,1 ps, which is attributed to electron solvation by nonadiabatic coupling to nuclear degrees of freedom of the surrounding polar molecular environment. Concomitant with this stabilization process, residual wave function overlap of the solvated electron with the metal substrate results in back-transfer by tunneling through the solvation shell. At such interfaces the correlation of electronic and molecular structure with the resulting solvation dynamics can be explored using different substrates as a template. Here we compare data on molecularly thin D2O ice layers grown on Cu(111) and Ru(001). On Ru(001) both the stabilization and back-transfer proceed about three times faster compared to Cu(111), which is attributed to different interfacial structures and the role of d-states, and projected band gaps in the electron transfer process. [source] Stress distribution associated with loaded acrylic,metal,cement crowns by using finite element methodJOURNAL OF ORAL REHABILITATION, Issue 11 2002M. Toparli SUMMARY, The axisymmetrical finite element method (FEM) was used to compare stress distribution in a maxillary second premolar restored tooth. The three models were evaluated by crowning the tooth with Au,Pd alloy, Ni,Cr alloy and Ti alloy with acrylic. A longitudinal static force, 200 N in magnitude at an angle of 45° was applied on the occlusal margin of each model. The tooth was assumed isotropic, homogenous and elastic. This numerical study was carried out using axisymmetric finite element models and calculation programmes were prepared by the authors using FORTRAN 77. Comparison of stress distributions was made in four regions of apex, cole, dentin,metal interface and metal,acrylic interface. The highest stress values were obtained when NiCr alloy with acrylic was used. [source] Glass-to-Metal Seal Interfacial Analysis using Electron Probe Microscopy for Reliable Solid Oxide Fuel CellsJOURNAL OF THE AMERICAN CERAMIC SOCIETY, Issue 4 2009Scarlett J. Widgeon The chemical compatibility between sealing glasses and interconnect materials for solid oxide fuel cells (SOFCs) has been studied in SOFC environments. Two borate-based glass compositions were sealed to interconnect materials, 441 stainless-steel (441SS) and Mn1.5Co1.5O4 -coated 441SS. The Mn1.5Co1.5O4 -coated 441SS coupons were analyzed as-received using X-ray diffraction (XRD) and electron probe microanalysis (EPMA) to obtain structural information and concentration profiles, respectively. The concentration profiles and the lack of Fe-containing phases present in the XRD spectrum show Fe is present throughout the coating, suggesting that Fe is partially substituted in the Mn1.5Co1.5O4 spinel. The glass,metal coupons were heat treated in air at 750°C for 500 h. The specimens were analyzed by EPMA and scanning electron microscope (SEM) to obtain images of the glass microstructure at the interface, to verify seal adherence, and to record concentration profiles across the glass,metal interface, with an emphasis on Cr. In total, four seal configurations were tested and analyzed, and in all cases the glasses remained well adhered to the metal and coating, and there was no microstructural evidence of new reaction phases present at the interface. There was slight diffusion of Cr from the 441SS into the sealing glasses, and Cr diffusion was hindered by the coating on the coated 441SS samples. [source] Low- and high-frequency C,V characteristics of the contacts formed by sublimation of the nonpolymeric organic compound on p-type Si substratePHYSICA STATUS SOLIDI (A) APPLICATIONS AND MATERIALS SCIENCE, Issue 14 2004C. Temirci Abstract The Sn/pyronine- B/p-Si Schottky structures have been obtained by sublimation of the organic compound pyronine- B onto the top of a p-Si surface. Barrier height and ideality factor value of 0.79 eV and 1.13, respectively, for the device have been determined from the forward-bias current,voltage (I,V) characteristics. The interface state density obtained from the forward bias high and low capacitance,voltage characteristics increases exponentially with bias between the midgap and the top of the valance band, from 2.15 × 1010 cm,2 eV,1 at (0.79,Ev) eV to 1.16 × 1012 cm,2 eV,1 at (0.53,Ev) eV. These values have been compared to those of the metal/Si structures in the literature, and it is seen that the presence of the nonreactive organic materials at the inorganic semiconductor and metal interface may obstruct the generation of the interface states at the semiconductor surface that strongly influence the Schottky barrier formation. (© 2004 WILEY-VCH Verlag GmbH & Co. KGaA, Weinheim) [source] The bone,metal interface of defect and press-fit ingrowth of microwave plasma-chemical vapor deposition implants in the rabbit modelCLINICAL ORAL IMPLANTS RESEARCH, Issue 1 2005Stephan Rupprecht Abstract Purpose: The histological differences between the defect and contact areas of the implant surface to bone were tested in 35 New Zealand White rabbits in a standardized model. Microwave plasma chemical vapor-coated implant probes were tested in control and uncoated materials. Material and methods:, In each femur of 35 rabbits, cylindrical implant rods with a planed side were inserted. Three groups, divided in coated and uncoated material at half, were observed 42, 84 and 168 days. The probes were examined histologically for bone,implant contact in the curved and plane (defect area) sides. Results: Generally the bone,implant contact seems to be nearly constant in time in the curved area of coated and uncoated probes. Here the implant was inserted in the press-fit mode. Diamond-coated probes showed similar bone,implant contact (51.9% (42 days), 62.5% (84 days), 56.1% (168 days)) compared to uncoated material (56.2%, 65.4%, 62.9%). The defect area (plane side) had no bone,implant contact at the time of insertion and showed increasing values on longer observation times with only significant differences in the 42-day group between coated (17.85%, 35.2%, 47.7%) and uncoated materials (35.5%, 40.55%, 51.81%). Conclusion: The evaluation of the curved side of the implant probe showed no great variation of bone,implant contact within the described observation times. This model simulates the usual implant insertion situation. The diamond-coated material becomes osseointegrated at a later time point. The bone,implant contact was only statistically relevant in one group in comparison to uncoated material. Résumé Les différences histologiques entre la lésion et les aires de contact de la surface implantaire à l'os ont été testées chez 35 lapins blancs de Nouvelle-Zélande dans un modèle standardisé. Des sondes implantaires recouvertes d'une vapeur chimique de plasma par micro-ondes ont été testées par rapport à du matériel non-recouvert. Dans chaque fémur des 35 lapins, des baguettes implantaires cylindriques avec un côté plat ont été insérées. Trois groupes, divisés en matériel couvert et non-couvert à moitié ont été observés après 42, 84 et 168 jours. Les sondes ont été examinées histologiquement pour le contact os-implant dans les sites courbe et plat (aire de la lésion). Généralement le contact os-implant semblait constant dans la durée dans la zone courbe des sondes couvertes et non-couvertes. Ici l'implant a été inséré par la méthode de pressé-fixé (=fit après insertion). Les sondes recouvertes de diamant montraient un contact os-implant semblable (52%à 42 J, 63%à 84 J et 56%à 168 J) comparées au matériel non-recouvert (56%, 65%, 63%). L'aire de la lésion (partie plate) n'avait pas de contact os-implant au moment de l'insertion et montrait des valeurs grandissantes avec le temps avec seulement des différences significatives dans les groupes à 42 jours entre le matériel recouvert (18%, 35% et 48%) et le non-recouvert (36%, 41% et 52%). L'évaluation du côté arrondi de la sonde implantaire ne montrait pas de grande variation dans le contact os-implant dans les temps d'observation décrits. Ce modèle simule la situation d'insertion implantaire usuelle. Le matériel recouvert de diamant devient ostéoïntégré plus tardivement. Le contact os-implant n'était statistiquement valable que dans un groupe en comparaison avec le matériel non-recouvert. Zusammenfassung Ziel: Mit einem standartisierten Modell untersuchte man an 35 weissen New Zealand Kaninchen die histologischen Unterschiede zwischen in direktem Kontakt mit dem Implantat stehendem Knochen und Defektstellen. Testimplantate, die mit Diamant beschichtet worden sind, verglich man mit unbeschichtetem Material als Kontrolle. Material und Methode: In jeden Femur der 35 Kaninchen inserierte man zylindrische Implantate, die auf einer Seite abgeplattet waren. Man beobachtete drei Gruppen, je hälftig unterteilt in beschichtete und unbeschichtete Implantate, während 42, 84 und 168 Tagen. Die Blockbiopsien wurden in der runden und abgeflachten (Defektzone) Region histologisch auf ihren Implantat-Knochen-Kontakt hin untersucht. Resultate: Allgemein stellte man fest, dass der Knochen-Implantat-Kontakt während der ganzen Beobachtungszeit in der runden Region der beschichteten und unbeschichteten Implantate ziemlich konstant zu bleiben scheint. Die Implantate sind eingeklopft worden. Die diamantbeschichteten Prüfkörper zeigten einen ähnlichen Knochen-Implantat-Kontakt (51.9% (42d), 62.5% (84d), 56.1% (168d)) wie die unbeschichteten Prüfkörper (56.2%, 65.4%, 62.9%). Die Defektzonen (abgeflechte Stellen) hatten zum Zeitpunkt der Implantation natürlich keinen Kontakt zum Knochen, zeigten aber während der Beobachtungszeit zunehmend Kontakt. Einzig nach 42 Tagen zeigten sich zwischen den beschichteten (17.85%, 35.2%, 47.7%) und den unbeschichteten Implantaten (35.5%, 40.55%, 51.81%) signifikante Unterschiede. Zusammenfassung: Innerhalb der umschriebenen Beobachtungszeit zeigte die Untersuchung der runden Seite der Implantate keine grossen Unterschiede bei der Ausdehnung der Kontaktflächen zum Knochen. Dieses Modell empfindet die übliche Implantationssituation nach. Das mit Diamant beschichtete Material wird zu einem etwas späteren Zeitpunkt osseointegriert. Die Unterschiede im Knochen-Implantat-Kontakt waren im Vergleich mit dem unbeschichteten Material nur in einer Gruppe statistisch gesehen von Bedeutung. Resumen Propósito: Se probaron las diferencias histológicas entre los defectos y las áreas de contacto de la superficie del implante al hueso en 35 conejos blancos de Nueva Zelanda en un modelo estandarizado. Se investigaron implantes de prueba cubiertos de plasma de vapor químico de microonda frente a material sin cubierta como control. Material y Métodos: Se insertaron en cada fémur de 35 conejos barras cilíndricas de implantes con un lado plano. Se observaron tres grupos divididos en material cubierto y no cubierto a la mitad durante 42, 84 y 168 días. Las pruebas se examinaron histológicamente para contacto hueso-implante en los lados curvado y plano (área de defecto). Resultados: Generalmente el contacto hueso implante suele ser constante en el tiempo en el área curvada de las pruebas cubiertas y no cubiertas. Aquí el implante se insertó en el modo press-fit. Las pruebas cubiertas de diamantes mostraron un contacto hueso implante similar (51.9% (42d), 62.5% (84d), 56.1% (168)) comparados con el material no cubierto (56.2%, 65.4%, 62.9%). El área de defecto (lado plano) no tuvo contacto hueso implante en el momento de la inserción y mostró valores crecientes en periodos mas largos de observación con solo diferencias significativas en el grupo del día 42 entre materiales cubiertos (17.85, 32.2%, 47%) y no cubiertos (35.5%, 40.55%, 51.81%). Conclusión: La evaluación del lado curvado del implante de prueba no mostró una gran variación del contacto hueso implante dentro de los tiempos de observación descritos. Este modelo simula la situación usual de inserción del implante. El material cubierto de diamante se osteointegra en un momento posterior. El contacto hueso implante fue solo estadísticamente relevante en un grupo en comparación con el material no cubierto. [source] Metal-Ceramic Interface Evaluation of a Gold-Infiltrated AlloyJOURNAL OF PROSTHODONTICS, Issue 7 2009Rupal Vasani BDS Abstract Purpose: The success of metal-ceramic systems partially depends on the formation of a stable bond between metal and porcelain. The purpose of this study was to investigate the porcelain/metal interface and the mechanism of interfacial bonding in a gold-infiltrated alloy (Captek). Materials and Methods: Captek specimens with feldspathic porcelain were evaluated by optical microscopy, scanning electron microscopy (SEM), electron probe microanalysis (EPMA), X-ray diffraction (XRD), and the Schwickerath crack initiation test for metal-ceramic bond compatibility. Specimens were processed with or without Capbond, a bonding agent. A traditional metal-ceramic alloy was also analyzed with microscopy for comparative purposes. Results: Optical and scanning electron micrographs of Captek specimens processed with Capbond revealed close adaptation of porcelain to the surface of the metal with sporadic nodules extending from the Captek surface. In contrast, the specimens of Captek without Capbond showed a much flatter porcelain/metal interface. Comparatively, the porcelain/metal interface of the traditional metal-ceramic crown showed greater surface roughness than the Captek specimens. No metal oxides were observed at the porcelain/metal interface of the Captek specimens with XRD. During the Schwickerath test, the Captek specimens permanently deformed, not allowing for crack initiation at the porcelain/metal interface. Conclusions: Microscopy and XRD analysis showed that micromechanical interlocking is the primary mechanism of porcelain adherence to Captek metal. The use of Capbond prior to porcelain application to Captek results in gold nodules on the surface to aid retention. Existing metal-ceramic bond compatibility standardized tests are not sufficient for evaluating Captek, primarily due to the flexibility of the material. [source] | |||||||||||||