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作 者:K.Chandrakanta R.Jena P.Pal Md.F.Abdullah S.D.Kaushik A.K.Singh
机构地区:[1]Department of Physics and Astronomy,National Institute of Technology,Rourkela-769008,Odisha,India [2]UGC-DAE Consortium for Scientific Research Mumbai Centre,R-5 Shed,BARC,Mumbai-400085,India
出 处:《International Journal of Minerals,Metallurgy and Materials》2021年第11期1861-1867,共7页矿物冶金与材料学报(英文版)
基 金:UGC-DAE CSR,Mumbai(Sanction No.CRS-M-187,225);Board of Research in Nuclear Science(BRNS),Mumbai(Sanction No.2012/37P/40/BRNS/2145);Science and Engineering Research Board(SERB),New Delhi(Sanction No.SR/FTP/PS-187/2011)for funding and fellowships.
摘 要:Cobalt(Co)-modified brownmillerite KBiFe_(2)O_(5)(KBFO;[KBiFe_(2(1−x))Co_(2x)O_(5)(x=0,0.05)])polycrystalline is synthesized following the solid-state reaction route.Rietveld refinement of X-ray diffraction data confirmed the phase purity of KBFO and KBiFe_(1.9)Co_(0.1)O_(5)(KBFCO).The optical bandgap energy(Eg)of KBFO decreased from 1.59 to 1.51 eV because of Co substitution.The decrease in bandgap can be attributed to the tilting of the Fe–O tetrahedral structure of KBFCO.The observed room-temperature Raman peaks of KBFCO shifted by 3 cm^(−1) toward a lower wavenumber than that of KBFO.The shift in Raman active modes can be attributed to the change in the bond angles and bond lengths of the Fe–O tetrahedral structure and modification in response to oxygen deficiency in KBFO because of Co doping.Compared with that of KBFO,the frequency-dependent dielectric constant and dielectric loss of KBFCO decrease at room temperature,which is a consequence of the reduction in oxygen migration and modification in response to vibrational modes present in the sample.
关 键 词:BROWNMILLERITE rietveld refinement Raman spectroscopy bandgap
分 类 号:TB34[一般工业技术—材料科学与工程]
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