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dc.contributor.authorDutta, Alo
dc.contributor.authorSinha, Tripurari Prasad
dc.date.accessioned2012-11-20T05:57:59Z
dc.date.available2012-11-20T05:57:59Z
dc.date.issued2011-02-03
dc.identifierFOR ACCESS / DOWNLOAD PROBLEM -- PLEASE CONTACT LIBRARIAN, BOSE INSTITUTE, akc@bic.boseinst.ernet.inen_US
dc.identifier.citationDutta A and Sinha T P (2011) Dielectric relaxation and conduction mechanism in LaNi314M11P 3 (M=Mo, W) at low temperature, Journal of Alloys and Compounds, 509, 1705-1710.en_US
dc.identifier.issn0925-8388
dc.identifier.uri1. Full Text Link ->en_US
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dc.identifier.urihttp://www.scopus.com/record/display.url?eid=2-s2.0-78651366282&origin=resultslist&sort=plf-f&src=s&st1=Dielectric+relaxation+and+conduction+mechanism+in+LaNi&sid=jO0ZcG0VyBv6ZfqYHI0ku_z%3a120&sot=q&sdt=b&sl=74&s=TITLE-ABS-KEY-AUTH%28Dielectric+relaxation+and+conduction+mechanism+in+LaNi%29&relpos=0&relpos=0&searchTerm=TITLE-ABS-KEY-AUTH(Dielectric%20relaxation%20and%20conduction%20mechanism%20in%20LaNi)en_US
dc.descriptionDOI : 10.1016/j.jallcom.2010.10.012en_US
dc.description.abstractIn order to investigate the electrical transport in LaNi3/4Mo1/4O3 and LaNi3/4W1/4O3, the dc conductivity and dielectric properties in these polycrystalline materials are investigated in the temperature range from 163K to 383 K and frequency range from 50 Hz to 1 MHz. The X-ray diffraction patterns of the samples show monoclinic phase at room temperature. The homogeneity of the samples is determined by energy dispersive analysis of X-ray (EDAX) attached with a scanning electron microscope. The temperature dependence of dc conductivity shows the semiconducting nature of the materials. The complex impedance plane plots show that the relaxation (conduction) mechanism in these materials is purely a bulk effect arising from the semiconductive grains. The frequency-dependent electrical data are also analyzed in the framework of ac conductivity formalism. The ac conductivity spectra follow the universal power law. The activation energies required for bulk conduction is 0.143 and 0.165 eV for LNM and LNVV respectively. The scaling behaviour of loss tangent suggests that the relaxation describes the same mechanism at various temperatures.en_US
dc.description.sponsorshipDepartment of Science and Technology of India SR/S2/CMP-01/2008 CSIR, New Delhien_US
dc.language.isoenen_US
dc.publisherELSEVIER SCIENCEen_US
dc.subjectELECTRICAL-TRANSPORTen_US
dc.subjectPOLARONIC CONDUCTIONen_US
dc.subjectMAGNETIC-PROPERTIESen_US
dc.subjectHOPPING CONDUCTIONen_US
dc.subjectTRANSITIONen_US
dc.subjectLACOO3en_US
dc.subjectLA2O3en_US
dc.subjectLIen_US
dc.subjectWOS:000287167700075en_US
dc.titleDielectric relaxation and conduction mechanism in LaNi3/4M1/4O3 (M = Mo, W) at low temperatureen_US
dc.title.alternativeJOURNAL OF ALLOYS AND COMPOUNDSen_US
dc.typeArticleen_US


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