<?xml version="1.0" encoding="UTF-8"?><xml><records><record><source-app name="Biblio" version="6.x">Drupal-Biblio</source-app><ref-type>17</ref-type><contributors><authors><author><style face="normal" font="default" size="100%">Bianchi, C.</style></author><author><style face="normal" font="default" size="100%">Ferreira, L.M.</style></author><author><style face="normal" font="default" size="100%">Loureiro, J.</style></author><author><style face="normal" font="default" size="100%">Rodrigues, A.</style></author><author><style face="normal" font="default" size="100%">Duarte, P.</style></author><author><style face="normal" font="default" size="100%">Baptista, A.C.</style></author><author><style face="normal" font="default" size="100%">Ferreira, I.M.</style></author></authors></contributors><titles><title><style face="normal" font="default" size="100%">Vanadium Pentoxide Alloyed with Graphite for Thin-Film Thermal Sensors</style></title><secondary-title><style face="normal" font="default" size="100%">Journal of Electronic Materials</style></secondary-title></titles><keywords><keyword><style  face="normal" font="default" size="100%">Carrier concentration</style></keyword><keyword><style  face="normal" font="default" size="100%">Electrical conductivity</style></keyword><keyword><style  face="normal" font="default" size="100%">Graphite</style></keyword><keyword><style  face="normal" font="default" size="100%">Graphite powder</style></keyword><keyword><style  face="normal" font="default" size="100%">Infrared wavelengths</style></keyword><keyword><style  face="normal" font="default" size="100%">Temperature sensors</style></keyword><keyword><style  face="normal" font="default" size="100%">Thermal evaporation</style></keyword><keyword><style  face="normal" font="default" size="100%">Thermal evaporation technique</style></keyword><keyword><style  face="normal" font="default" size="100%">Thermal sensors</style></keyword><keyword><style  face="normal" font="default" size="100%">Thermoelectric</style></keyword><keyword><style  face="normal" font="default" size="100%">Thin films</style></keyword><keyword><style  face="normal" font="default" size="100%">Vanadium</style></keyword><keyword><style  face="normal" font="default" size="100%">Vanadium compounds</style></keyword><keyword><style  face="normal" font="default" size="100%">Vanadium pentoxide</style></keyword><keyword><style  face="normal" font="default" size="100%">Variable weight</style></keyword></keywords><dates><year><style  face="normal" font="default" size="100%">2016</style></year></dates><urls><web-urls><url><style face="normal" font="default" size="100%">https://www.scopus.com/inward/record.uri?eid=2-s2.0-84961286738&amp;doi=10.1007%2fs11664-016-4363-2&amp;partnerID=40&amp;md5=bf6eaccafb26f5793cbd46ae314f7f39</style></url></web-urls></urls><number><style face="normal" font="default" size="100%">3</style></number><publisher><style face="normal" font="default" size="100%">Springer New York LLC</style></publisher><volume><style face="normal" font="default" size="100%">45</style></volume><pages><style face="normal" font="default" size="100%">1987-1991</style></pages><language><style face="normal" font="default" size="100%">eng</style></language><abstract><style face="normal" font="default" size="100%">The thermoelectric (TE) properties of vanadium pentoxide (V2O5) alloyed with graphite (G) were studied as a function of its incorporation percentage. Variable weight percentages of graphite powder (0–50%) were added to V2O5 powder and their mixtures were evaporated by a thermal evaporation technique to form thin films with a thickness in the range of 30–80Â nm. In the infrared wavelength region, the transmittance of the obtained films increased as the G percentage was increased, while in the visible range, it decreased with G up to 10%. The TE properties were improved when G was in the range of 10–30%, while it decreased for the other percentages: Seebeck coefficient (S) changed from 0.6Â mV/K to 0.9Â mV/K and was zero with a G of 50%; the electrical conductivity varied slightly from 5Â (Ωm)−1 to 0.7Â (Ωm)−1 while the mobility improved from 0.07Â cm2/VÂ s to 1.5Â cm2/VÂ s and the respective carrier concentration was reduced, from 1Â Ã&amp;#151;Â 1018Â cm−3 to 4Â Ã&amp;#151;Â 1016Â cm−3. These films were applied as temperature sensors evaluating the thermovoltage as a function of thermal gradient between two electrodes, in which one was maintained at room temperature. Â© 2016, The Minerals, Metals &amp; Materials Society.</style></abstract><notes><style face="normal" font="default" size="100%">cited By 0</style></notes></record></records></xml>