Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/8009
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dc.contributor.authorSoni, Kavitaen_US
dc.contributor.authorYadav, Ektaen_US
dc.contributor.authorSaseendra, Harisankaren_US
dc.contributor.authorMavani, Krushna R.en_US
dc.date.accessioned2022-03-17T01:00:00Z-
dc.date.accessioned2022-03-21T11:14:42Z-
dc.date.available2022-03-17T01:00:00Z-
dc.date.available2022-03-21T11:14:42Z-
dc.date.issued2020-
dc.identifier.citationSoni, K., Yadav, E., Harisankar, S., & Mavani, K. R. (2020). Influence of ce doping and thickness on the structure and non-fermi liquid behavior of LaNiO3 thin films. Journal of Physics and Chemistry of Solids, 141 doi:10.1016/j.jpcs.2020.109398en_US
dc.identifier.issn0022-3697-
dc.identifier.otherEID(2-s2.0-85080914352)-
dc.identifier.urihttps://doi.org/10.1016/j.jpcs.2020.109398-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/8009-
dc.description.abstractThin films of La1-xCexNiO3 (x = 0, 0.1, and 0.3) are grown with two different thickness (8 and 24 nm) on single-crystal LaAlO3 (001) (LAO) substrate using pulsed laser deposition. The films with x = 0 and 0.1 are highly oriented toward the (00l) axis despite different thickness, whereas the higher doped films (x = 0.3) of both thicknesses show two crystallographic orientations. A significant shifting of Raman modes is observed due to increased Ce doping, clearly indicating a large change in Ni–O–Ni bond-angle and NiO6 octahedra distortion. Also, Raman modes show a red-shift in all the thin films with increases in temperature. These films remain metallic until low temperatures. The resistivity increases with increased Ce doping as well as with increased thickness. The resistivity data fit well with the power-law equation, indicating a non-Fermi liquid state. This study helps to distinguish the effects of Ce doping and thickness on the structure and Raman modes. © 2020en_US
dc.language.isoenen_US
dc.publisherElsevier Ltden_US
dc.sourceJournal of Physics and Chemistry of Solidsen_US
dc.subjectAluminum compoundsen_US
dc.subjectCeriumen_US
dc.subjectCerium compoundsen_US
dc.subjectFermi liquidsen_US
dc.subjectFermionsen_US
dc.subjectLanthanum compoundsen_US
dc.subjectLiquidsen_US
dc.subjectNickel compoundsen_US
dc.subjectPulsed laser depositionen_US
dc.subjectPulsed lasersen_US
dc.subjectRaman spectroscopyen_US
dc.subjectRed Shiften_US
dc.subjectSemiconductor dopingen_US
dc.subjectSingle crystalsen_US
dc.subjectCrystallographic orientationsen_US
dc.subjectDifferent thicknessen_US
dc.subjectLaNiO3 thin filmen_US
dc.subjectLow temperaturesen_US
dc.subjectNickelatesen_US
dc.subjectNon-Fermi liquidsen_US
dc.subjectNon-Fermi-liquid behavioren_US
dc.subjectPower law equationen_US
dc.subjectThin filmsen_US
dc.titleInfluence of Ce doping and thickness on the structure and non-Fermi liquid behavior of LaNiO3 thin filmsen_US
dc.typeJournal Articleen_US
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