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A New Oxide Ion Conductor Family: Bi7(P1-yVy)O13

โœ Scribed by J.P. Wignacourt; M. Drache; P. Conflant


Publisher
Elsevier Science
Year
1993
Tongue
English
Weight
190 KB
Volume
105
Category
Article
ISSN
0022-4596

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โœฆ Synopsis


A new phase, (\mathrm{Bi}{7} \mathrm{PO}{13}), obtained at room temperature in the (\mathrm{Bi}{2} \mathrm{O}{3}-\mathrm{BiPO}{4}) system, has been identified as a superstructure of the (\delta \mathrm{Bi}{2} \mathrm{O}{3}) fcc form. Its conductivity level has been improved by a substitution of (\mathrm{V}) for (\mathrm{P}), in solid solution (\mathrm{Bi}{7}\left(\mathrm{P}{1-y} \mathrm{~V}{y}\right) \mathrm{O}{1,3}) with (0 \leq y \leq 0.5). Above (400^{\circ} \mathrm{C}) the conduction mechanism is due to the mobility of the (\mathrm{O}^{2-}) ions. The electrolyte (P{\mathrm{O}_{2}}) response time has been investigated vs time for successive thermal cycles. 1993 Academic Press. Inc.


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Bi23M4O44.5 (M = P and V): new oxide-ion
โœ Akiteru Watanabe ๐Ÿ“‚ Article ๐Ÿ“… 1997 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 501 KB

27(l)", p = 87.51(l)", and y = 119.82( 1)" for M =V Two formula weights are contained in the'unit cell. The structure is based on a pseudo-fee subcell with a' = 5.5 A. The axial relations between the triclinic cell and the subcell are a = b = (3 &/2)a' and c = (3 v'&2)a'. The compounds show a good o