2017
DOI: 10.1016/j.matdes.2017.01.068
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Synthesis of 3D architecture CuO micro balls and nano hexagons and its electrochemical capacitive behavior

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Cited by 23 publications
(15 citation statements)
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“…The O 1s core spectra of CeO 2 and 6% CuO-CeO 2 (Figure 5c) exhibit two peaks, a broad intense peak at 529 eV and a less-intense peak at 530.7 eV in the case of CeO 2 and a broad intense peak at 529.2 eV and a less-intense peak at 531.3 in the case of CuO-CeO 2 . The main intense XPS peaks at a lower binding energy (529–529.2 eV) are ascribed to the lattice O 2− ions, whereas the less-intense shoulder peaks at a higher binding energy (530.7–531.3 eV) can be attributed to the hydroxyl (–OH) or polarized oxygen species present close to the oxygen vacancies [57,58]. The center of the main and shoulder peaks in the case of CuO-CeO 2 are slightly shifted to higher binding energy (blue-shift) when compared to pure CeO 2 , indicating the influence of the difference in electronegativity between copper and cerium on the chemical speciation of oxygen species.…”
Section: Resultsmentioning
confidence: 99%
“…The O 1s core spectra of CeO 2 and 6% CuO-CeO 2 (Figure 5c) exhibit two peaks, a broad intense peak at 529 eV and a less-intense peak at 530.7 eV in the case of CeO 2 and a broad intense peak at 529.2 eV and a less-intense peak at 531.3 in the case of CuO-CeO 2 . The main intense XPS peaks at a lower binding energy (529–529.2 eV) are ascribed to the lattice O 2− ions, whereas the less-intense shoulder peaks at a higher binding energy (530.7–531.3 eV) can be attributed to the hydroxyl (–OH) or polarized oxygen species present close to the oxygen vacancies [57,58]. The center of the main and shoulder peaks in the case of CuO-CeO 2 are slightly shifted to higher binding energy (blue-shift) when compared to pure CeO 2 , indicating the influence of the difference in electronegativity between copper and cerium on the chemical speciation of oxygen species.…”
Section: Resultsmentioning
confidence: 99%
“…The variation in lattice constant value was caused due to variation in crystallite size contributed by several factors like surface energy, lack of outermost bonding on the surface atoms and intra‐crystalline pressure. In the present investigation the observed variation in ‘a’ values was due to the self‐interstitials and mechanically induced strains developed during nucleation . Co 3 O 4 formation mechanism is given as below: trueCo2+4pt+4pt6H2normalO4pt4pt[Co(normalH2normalO)6]2+4pt trueNH34pt+4ptnormalH2normalO4pt4ptNH4+4pt+4ptOH- true[Co(normalH2normalO)6]2+4pt+4pt2OH-4pt4ptCo(OH)24pt+4pt6H2normalO true6Co(OH)4pt24pt+4ptnormalO24pt4pt2Co3normalO44pt+4pt6H2normalO …”
Section: Resultsmentioning
confidence: 99%
“…Carbon coating was found to be one of the effective ways to improve the performance of TMOs by increasing the conductivity of active material and also accommodating large volume expansion . Nano structured active materials with high surface to volume ratio enhanced the conductivity of TMOs . Reducing the particle size was also an efficient methodology to improve the electrochemical performance by shortening the diffusion path length and to create larger contact area between the electrode‐electrolyte interface ,.…”
Section: Introductionmentioning
confidence: 99%
“…The energy storage of pseudocapacitors is based on both ion adsorption and fast surface redox reactions, which can beneficially endow high specific capacitance and energy density compared to electrochemical double-layer capacitors [ 1 , 2 ]. The transition metal oxides, such as MnO x , RuO 2, CoO x , Cr 2 O 3 , CuO, NiO, CeO 2 , and FeO x , are widely employed, thanks to their low cost, low toxicity, and environmental friendliness, as active electrode materials for pseudocapacitors [ 3 , 4 , 5 , 6 ]. For example, manganese oxide (MnO 2 ) has stood out because of its amazingly high theoretical specific capacitance of 1370 F·g −1 [ 7 ].…”
Section: Introductionmentioning
confidence: 99%