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dc.contributor.authorNayak, S.en_US
dc.contributor.authorDasari, K.en_US
dc.contributor.authorJoshi, D. C.en_US
dc.contributor.authorPramanik, P.en_US
dc.contributor.authorPalai, R.en_US
dc.contributor.authorSathe, V.en_US
dc.contributor.authorChauhan, R. N.en_US
dc.contributor.authorTiwari, N.en_US
dc.contributor.authorThota, S.en_US
dc.date.accessioned2017-04-21T06:55:54Z-
dc.date.available2017-04-21T06:55:54Z-
dc.date.issued2016-11en_US
dc.identifier.issn0370-1972en_US
dc.identifier.urihttp://dx.doi.org/10.1002/pssb.201600295en_US
dc.identifier.urihttp://hdl.handle.net/11536/132858-
dc.description.abstractIn this article, we report a comparative analysis of various spectroscopic studies including low-temperature (25T300K) Raman spectroscopy of cobalt-orthotitanate (Co2TiO4) and tricobalt-tetraoxide (Co3O4), and their solid solutions (1-x) Co3O4+x of Co2TiO4 (0x1 (100wt.%)). For all the lower and intermediate compositions, five Raman-active modes were recognized at 689,618,518,480, and 195cm-1 that are associated with A1g, Eg, and 3F2g phonon symmetries. Conversely, pure Co2TiO4 exhibits a broad spectrum of width approximate to 93.3cm-1 without any signatures of F2g(3) mode. At low-temperatures (down to 25K) the A1g and F2gpeaks of both Co2TiO4 and Co3O4 shift toward the high-frequency side with anomalies across the ferrimagnetic Neel temperature (TN approximate to 48 +/- 5K) and antiferromagnetic Neel temperature (TN approximate to 30 +/- 10 K), respectively. All the investigated samples exhibit two distinct bands at 576cm-1 (B1) and 665cm-1 (B2) in the Fourier transform infrared spectra recorded at 300 +/- 10 K, associated with the vibrational stretching of the metal-oxygen bonds of length approximate to 195.8pm (B-O) and approximate to 185.4pm (A-O), respectively. The intensity of these sharp bands gradually decreases as the crystal structure transforms from normal-spinel (a=8.07 angstrom) to inverse-spinel structure (a=8.45 angstrom). The X-ray photoelectron spectroscopy (XPS) studies revealed that the Ti was incorporated into the octahedral B-sites of inverse-spinel structure of Co2TiO4. Interestingly, the XPS spectra of Co2TiO4 provide evidence of the trivalent character of Ti instead of tetravalent cationic configuration together with a weak Co3+ character at the octahedral sites. These results are discussed in terms of the binding-energy (BE) difference between the O-1s and Ti-2p3/2 ([O-Ti-2p3/2]=BE(O-1s) -BE(Ti-2p3/2)) and the mean chemical bond length l[Ti-O]. The peculiarities of all these results in consonance with the crystal-structure (bond angles and bond lengths) and electron-spin-resonance studies are discussed in detail.en_US
dc.language.isoen_USen_US
dc.subjectantiferromagnetismen_US
dc.subjectCo3O4en_US
dc.subjectCo2TiO4en_US
dc.subjectRaman spectroscopyen_US
dc.subjectSolid solutionsen_US
dc.subjectspinelsen_US
dc.subjectvibrational modesen_US
dc.titleSpectroscopic studies of Co2TiO4 and Co3O4 two-phase compositesen_US
dc.identifier.doi10.1002/pssb.201600295en_US
dc.identifier.journalPHYSICA STATUS SOLIDI B-BASIC SOLID STATE PHYSICSen_US
dc.citation.volume253en_US
dc.citation.issue11en_US
dc.citation.spage2270en_US
dc.citation.epage2282en_US
dc.contributor.department光電工程學系zh_TW
dc.contributor.department顯示科技研究所zh_TW
dc.contributor.departmentDepartment of Photonicsen_US
dc.contributor.departmentInstitute of Displayen_US
dc.identifier.wosnumberWOS:000387453800027en_US
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