Electrical conductivity and charge compensation in Nb doped TiO2 rutile

1977 ◽  
Vol 67 (3) ◽  
pp. 857 ◽  
Author(s):  
J. F. Baumard ◽  
E. Tani
2019 ◽  
Vol 104 (12) ◽  
pp. 1800-1805
Author(s):  
George M. Amulele ◽  
Anthony W. Lanati ◽  
Simon M. Clark

Abstract Starting with the same sample, the electrical conductivities of quartz and coesite have been measured at pressures of 1, 6, and 8.7 GPa, respectively, over a temperature range of 373–1273 K in a multi-anvil high-pressure system. Results indicate that the electrical conductivity in quartz increases with pressure as well as when the phase change from quartz to coesite occurs, while the activation enthalpy decreases with increasing pressure. Activation enthalpies of 0.89, 0.56, and 0.46 eV, were determined at 1, 6, and 8.7 GPa, respectively, giving an activation volume of –0.052 ± 0.006 cm3/mol. FTIR and composition analysis indicate that the electrical conductivities in silica polymorphs is controlled by substitution of silicon by aluminum with hydrogen charge compensation. Comparing with electrical conductivity measurements in stishovite, reported by Yoshino et al. (2014), our results fall within the aluminum and water content extremes measured in stishovite at 12 GPa. The resulting electrical conductivity model is mapped over the magnetotelluric profile obtained through the tectonically stable Northern Australian Craton. Given their relative abundances, these results imply potentially high electrical conductivities in the crust and mantle from contributions of silica polymorphs. The main results of this paper are as follows:The electrical conductivity of silica polymorphs is determined by impedance spectroscopy up to 8.7 GPa.The activation enthalpy decreases with increasing pressure indicating a negative activation volume across the silica polymorphs.The electrical conductivity results are consistent with measurements observed in stishovite at 12 GPa.


Materials ◽  
2018 ◽  
Vol 11 (10) ◽  
pp. 1934 ◽  
Author(s):  
Jing Xu ◽  
Haiying Wang ◽  
Zhongpo Zhou ◽  
Zhaorui Zou

In this work, undoped, N-doped, WO3-loaded undoped, and WO3-loaded with N-doped TiO2 rutile single-crystal wafers were fabricated by direct current (DC) magnetron sputtering. N-doping into TiO2 and WO3 loading onto TiO2 surface were used to increase and decrease oxygen vacancies. Various measurements were conducted to analyze the structural and magnetic properties of the samples. X-ray diffraction results showed that the N-doping and WO3 loading did not change the phase of all samples. X-ray photoelectron spectroscopy results revealed that W element loaded onto rutile single-crystal wafers existed in the form of WO3. UV-Vis spectrometer results showed that the absorption edge of WO3-loaded undoped and WO3-loaded with N-doped TiO2 rutile single-crystal wafers had red shift, resulting in a slight decrease in the corresponding band gap. Photoluminescence spectra indicated that oxygen vacancies existed in all samples due to the postannealing atmosphere, and oxygen vacancies density increased with N-doping, while decreasing with WO3 loading onto TiO2 surface. The magnetic properties of the samples were investigated, and the saturation magnetization values were in the order N-doped > WO3-loaded with N-doped > undoped > WO3-loaded undoped rutile single-crystal wafers, which was the same order as the oxygen vacancy densities of these samples. N-doping improved the saturation magnetization values, while WO3-loaded decreased the saturation magnetization values. This paper reveals that the magnetic properties of WO3-loaded with N-doped rutile single-crystal wafers originate from oxygen vacancies.


2011 ◽  
Vol 695 ◽  
pp. 65-68 ◽  
Author(s):  
Kwan Ho Park ◽  
Il Ho Kim

Co4-xFexSb12-ySny skutterudites were synthesized by mechanical alloying and hot pressing, and thermoelectric properties were examined. The carrier concentration increased by doping and thereby the electrical conductivity increased compared with intrinsic CoSb3. Every specimen had a positive Seebeck coefficient. Fe doping caused a decrease in the Seebeck coefficient but it could be enhanced by Fe/Sn double doping possibly due to charge compensation. The thermal conductivity was desirably very low and this originated from ionized impurity-phonon scattering. Thermoelectric properties were improved remarkably by Fe/Sn doping, and a maximum figure of merit, ZT = 0.5 was obtained at 723 K in the Co3FeSb11.2Sn0.8 specimen.


2015 ◽  
Vol 41 (5) ◽  
pp. 6281-6285 ◽  
Author(s):  
Román Alvarez Roca ◽  
Fidel Guerrero ◽  
José A. Eiras ◽  
J.D.S. Guerra

1978 ◽  
Vol 45 (2) ◽  
pp. 617-624 ◽  
Author(s):  
V. Cristea ◽  
V. Babeş

2009 ◽  
Vol 404 (18) ◽  
pp. 2838-2840 ◽  
Author(s):  
A.M. Mudarra Navarro ◽  
V. Bilovol ◽  
A.F. Cabrera ◽  
C.E. Rodríguez Torres ◽  
F.H. Sánchez

2013 ◽  
Vol 86 (12) ◽  
pp. 1178-1185
Author(s):  
A. Fakhim Lamrani ◽  
M. Belaiche ◽  
A. Benyoussef ◽  
A. El Kenz

2011 ◽  
Vol 50 (2R) ◽  
pp. 025501 ◽  
Author(s):  
Akiyuki Matsushita ◽  
Masahiko Shimoda ◽  
Takashi Naka ◽  
Yuh Yamada

2020 ◽  
Vol 8 (39) ◽  
pp. 20666-20676 ◽  
Author(s):  
Die Su ◽  
Li Liu ◽  
Zhixiao Liu ◽  
Jing Dai ◽  
Jiaxing Wen ◽  
...  

Ta-doped TiO2/C nanofibers can enhance the electrical conductivity, shorten the ion transport distance. Thus it shows outstanding electrochemical performance in both Li/K-metal half cells and Li/K full cells..


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