Academic literature on the topic 'Cu2V2O7'

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Journal articles on the topic "Cu2V2O7"

1

Suganya, P., J. Princy, N. Mathivanan, and Krishnasamy K. "One-Pot Synthesis of rGO@Cu2V2O7 Nanocomposite as High Stabled Electrode for Symmetric Electrochemical Capacitors." ECS Journal of Solid State Science and Technology 11, no. 4 (2022): 041005. http://dx.doi.org/10.1149/2162-8777/ac62f1.

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The rGO anchored copper vanadate nanostructures have been synthesized through facile hydrothermal synthesis for the high efficient energy storage applications. The prepared Cu2V2O7 and rGO@Cu2V2O7 nanostructures are fabricated as the electrode materials for three electrode and symmetric type electrochemical supercapacitors. Based on the electrochemical the electrodes shows the outstanding areal capacitance values of 340 and 545 F g−1 for Cu2V2O7 and rGO@Cu2V2O7 electrodes, respectively. Also the charge discharge curves of the rGO@Cu2V2O7 electrode revealed the higher specific capacitance value
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2

Shuang, Shuang, Leonardo Girardi, Gian Rizzi та ін. "Visible Light Driven Photoanodes for Water Oxidation Based on Novel r-GO/β-Cu2V2O7/TiO2 Nanorods Composites". Nanomaterials 8, № 7 (2018): 544. http://dx.doi.org/10.3390/nano8070544.

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This paper describes the preparation and the photoelectrochemical performances of visible light driven photoanodes based on novel r-GO/β-Cu2V2O7/TiO2 nanorods/composites. β-Cu2V2O7 was deposited on both fluorine doped tin oxide (FTO) and TiO2 nanorods (NRs)/FTO by a fast and convenient Aerosol Assisted Spray Pyrolysis (AASP) procedure. Ethylenediamine (EN), ammonia and citric acid (CA) were tested as ligands for Cu2+ ions in the aerosol precursors solution. The best-performing deposits, in terms of photocurrent density, were obtained when NH3 was used as ligand. When β-Cu2V2O7 was deposited on
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3

Krivovichev, S. V., S. K. Filatov, P. N. Cherepansky, T. Armbruster, and O. Yu Pankratova. "CRYSTAL STRUCTURE OF -Cu2V2O7 AND ITS COMPARISON TO BLOSSITE ( -Cu2V2O7) AND ZIESITE ( -Cu2V2O7)." Canadian Mineralogist 43, no. 2 (2005): 671–77. http://dx.doi.org/10.2113/gscanmin.43.2.671.

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4

Fontaine, Blandine, Youssef Benrkia, Jean-François Blach, et al. "Photoelectrochemical properties of copper pyrovanadate (Cu2V2O7) thin films synthesized by pulsed laser deposition." RSC Advances 13, no. 18 (2023): 12161–74. http://dx.doi.org/10.1039/d3ra01509b.

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The photoelectrochemical properties of copper pyrovanadate (bulk α-Cu2V2O7 and thin films β-Cu2V2O7 elaborated by pulsed laser deposition) were investigated. For thin films, the best photocurrent efficiency was obtained under blue light (450 nm).
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5

Krasnenko, Tatiana, Nadezhda Medvedeva, and Vitalii Bamburov. "Atomic and Electronic Structure of Zinc and Copper Pyrovanadates with Negative Thermal Expansion." Advances in Science and Technology 63 (October 2010): 358–63. http://dx.doi.org/10.4028/www.scientific.net/ast.63.358.

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Zinc and copper pyrovanadates are promising materials for micro- and optoelectronics due to their negative coefficient of volume thermal expansion (NTE). Besides, solid solutions on the base of these compounds can be used to obtain grade materials with variable thermal coefficients. Thermal deformation of both Zn2V2O7 and Cu2V2O7 structures was studied. According to the structural data, NTE of these substances is provided by the zigzag shape of zinc (copper) chains alongside with stable distances between layers. The structural and electronic characteristics depending on temperature were studie
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6

Benko, F. A., and F. P. Koffyberg. "Semiconductivity and optical interband transitions of CuV2O6 and Cu2V2O7." Canadian Journal of Physics 70, no. 2-3 (1992): 99–103. http://dx.doi.org/10.1139/p92-011.

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CuV2O6 and Cu2V2O7 are low-mobility n-type semiconductors; at room temperature [Formula: see text]. From photoelectron-chemical measurements optical interband transitions are found at 2.02 and 3.15 eV for indium-doped CuV2O6, and at 1.87 and 2.88 eV for Cu2V2O7. In both materials the valence band edge is 6.9 eV below the vacuum level; a qualitative analysis of all data indicates that the upper valence band is made up mainly of oxygen-2p wave functions, as in V2O5.
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7

Ponomarenko, L. A., A. N. Vasil'ev, E. V. Antipov, and Yu A. Velikodny. "Magnetic properties of Cu2V2O7." Physica B: Condensed Matter 284-288 (July 2000): 1459–60. http://dx.doi.org/10.1016/s0921-4526(99)02702-7.

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8

EGUCHI, M., I. FURUSAWA, T. MIURA, and T. KISHI. "Lithium insertion characteristics of ß-Cu2V2O7." Solid State Ionics 68, no. 1-2 (1994): 159–64. http://dx.doi.org/10.1016/0167-2738(94)90253-4.

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9

Wang, Hui, Mengjie Yang, Mingju Chao та ін. "Negative thermal expansion property of β-Cu2V2O7". Solid State Ionics 343 (грудень 2019): 115086. http://dx.doi.org/10.1016/j.ssi.2019.115086.

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10

Денисова, Л. Т., Н. В. Белоусова, В. М. Денисов та Н. А. Галиахметова. "Высокотемпературная теплоемкость оксидов системы CuO-V-=SUB=-2-=/SUB=-O-=SUB=-5-=/SUB=-". Физика твердого тела 59, № 6 (2017): 1243. http://dx.doi.org/10.21883/ftt.2017.06.44500.407.

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С помощью твердофазного синтеза из исходных компонентов CuO и V2O5 при ступенчатом обжиге получены CuV2O6 и Cu2V2O7. Методом дифференциальной сканирующей калориметрии измерена высокотемпературная теплоемкость оксидных соединений. По экспериментальным зависимостям CP=f(T) рассчитаны термодинамические свойства (изменение энтальпии, энтропии и приведенная энергия Гиббса). Установлено, что между удельной теплоемкостью и составом оксидов системы CuO-V2O5 имеется корреляция. DOI: 10.21883/FTT.2017.06.44500.407
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