© Local Structure And Redox State Of Vanadium In Vanadium Strontium Borate [(V2O5)(0 Center Dot 5)(SrO)(0 Center Dot 5)(SrO)(0 Center Dot 5-Y)(B2O3)(Y)]

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© Local Structure And Redox State Of Vanadium In Vanadium Strontium Borate [(V2O5)(0 Center Dot 5)(SrO)(0 Center Dot 5)(SrO)(0 Center Dot 5-Y)(B2O3)(Y)] Oxide Glasses Khattak, GD; Tabet, N; Mekki, A SOC GLASS TECHNOLOGY, PHYSICS AND CHEMISTRY OF GLASSES; pp: ; Vol: 46 King Fahd University of Petroleum & Minerals Summary The local structure of vanadium strontium borate glasses with the nominal composition [(V2O5)(0.5)(SrO)(0.5-y) (B2O3)y], where 0.1 <= y <= 0.4, as well as the valence state of the vanadium ions have been investigated by x-ray photoelectron spectroscopy (XPS). The core level binding energies of V 2p, Sr 3p, B Is and 0 Is have been measured. It was observed that there is a small increase in binding energies of the doublet peaks attributed to Sr 3p(3/2) and Sr 3p(1/2) in the Sr 3p spectra with an increase in the B2O3 content and also shifted by similar to 0-6 eV towards higher binding energies in comparison to their values in SrO powder The binding energies of the B 1s peak positions increase with an increase in the B2O3 content, have essentially the same FWHM but, in comparison to B2O3 powder, the peak positions have shifted towards lower binding energy side by similar to 0.7 e V The 0 Is core level spectra, however show asymmetry for all glass samples which results from two contributions, one from the presence of oxygen atoms in the V-O-V V-O-B, B-O-B environment (bridging oxygen BO) and the other from oxygen atoms in V-O-Sr, B-O- Sr V=O, environment (non-bridging oxygen NBO). The O 1s core level spectra were deconvoluted into two peaks (BO and NBO) and the ratio of NBO to total oxygen was found to decrease with increasing B2O3 content. The quantitative ratio, [V4+/V- Copyright: King Fahd University of Petroleum & Minerals;

© total], for each glass sample, has been determined from the analysis of the V 2p core level spectra. The ratio remains practically constant, independent of vanadium concentration within experimental uncertainties. References: ADLER D, 1971, AMORPHOUS SEMICONDUC ANDERSON GW, 1968, J APPL PHYS, V39, P1634 AUSTIN IG, 1969, ADV PHYS, V18, P41 AUSTIN IG, 1973, ELECT STRUCTURAL PRO BAMFORD CR, 1977, COLOUR GENERATION CO BRIGGS D, 1974, CHEM PHYS LETT, V25, P493 CULEA E, 1986, SOLID STATE COMMUN, V58, P545 DHAWAN VK, 1982, J NONCRYSTALLINE SOL, V51, P87 GOSH A, 1986, J NONCRYST SOLIDS, V83, P151 GOSH A, 1988, J APPL PHYS, V64, P2652 GRISCOM DL, 1978, MATERIALS SCI RES BO, V12, P36 HIRASHIMA H, 1982, YOGYO-KYOKAI-SHI, V90, P411 HIRASHIMA H, 1987, J NON-CRYST SOLIDS 2, V95, P817 HIRASHIMA H, 1988, GLASTECH BER, V61, P151 HIRASHIMA H, 1989, NIPPON SERAM KYO GAK, V97, P1144 HIRASHIMA H, 1990, SERAMIKKUSU RONBUN S, V97, P1150 KHATTAK GD, 1996, J NON-CRYST SOLIDS, V194, P1 KHATTAK GD, 1999, J NON-CRYST SOLIDS, V244, P128 KHATTAK GD, 2000, J NON-CRYST SOLIDS, V262, P66 KHATTAK GD, 2003, J ELECTRON SPECTROSC, V133, P103 LEBRUN N, 1990, SOLID STATE IONICS, V40, P718 LINARES RC, 1962, J AM CERAM SOC, V45, P307 LINSLEY GS, 1970, J NONCRYST SOLIDS, V4, P208 LIVAGE J, 1990, J NON-CRYST SOLIDS, V121, P35 MACKENZIE JD, 1964, MODERN ASPECTS VIREO, V3 MORI H, 1993, NIPPON SERAM KYO GAK, V101, P347 MOTT NF, 1968, J NONCRYST SOLIDS, V1, P1 PANTANO CG, 1993, EXPT TECHNIQUES GLAS, P129 PROCTOR A, 1980, ANAL CHEM, V52, P2315 SAKURAI Y, 1985, J ELECTROCHEM SOC, V132, P512 SAYER M, 1972, PHYS REVB, V6, P4629 SMETS BMJ, 1981, J NONCRYST SOLIDS, V46, P21 SMETS BMJ, 1984, PHYS CHEM GLASSES, V25, P113 For pre-prints please write to: Copyright: King Fahd University of Petroleum & Minerals;