[1] ThomasN. W.,Crystal structure–physical property relationships in perovskites,Acta Cryst.B45,337(1989).
[2] HazenR. M.,Perovskites,Sci. Am.258,52(1988).
[3] TrianaC. A.,Landínez TéllezD. A. andRoa-RojasJ.,Synthesis process and structural characterization of the Sr2EuRuO6 complex perovskite,J. Alloys Compd.516,179(2012).
[4] Grisales CerónJ. A.,Arbey RodríguezJ.,Rosales-RiveraA.,SalazarN. A.,Cuervo FarfánH. J. A.,Cardona VasquezJ. A.,Landínez TéllezD. A. andRoa-RojasJ.,Mott insulator behavior in the yttrium-based antimoniate oxide Ba2YSbO6,J. Mater. Res. Technol.8,3978(2019).
[5] KingG. andWoodwardP. M.,Cation ordering in perovskites,J. Mater. Chem.20,5785(2010).
[6] GoldschmidtV. M.,Die Gesetze der Krystallochemie.Naturwissenschaften14,477(1926).
[7] WoodwardP. M.,Octahedral tilting in perovskites. I. Geometrical considerations,Acta Cryst.B53,32(1997).
[8] AleksandrovK. S.,Mechanisms of the ferroelectric and structural phase transitions. structural distortions in perovskites,Ferroelectrics20,61(2011).
[9] LufasoM. W. andWoodwardP. M.,Jahn–Teller distortions, cation ordering and octahedral tilting in perovskites,Acta Cryst.B60,10(2004).
[10] JonkerG. H. andVan SantenJ. H.,Magnetic compounds wtth perovskite structure III. ferromagnetic compounds of cobalt,Physica19,120(1953).
[11] JonkerG. H. andVan SantenJ. H.,Ferromagnetic compounds of manganese with perovskite structure,Physica16,337(1950).
[12] Van SantenJ. H. andJonkerG. H.,Electrical conductivity of ferromagnetic compounds of manganese with perovskite structure,Physica16,599(1950).
[13] JinS.,TiefelT. H.,McCormackM.,FastnachtR. A.,RameshR. andChenL. H.,Thousandfold change in resistivity in magnetoresistive La-Ca-Mn-O Films,Science264,413(1994).
[14] GoodenoughJ. B.,An interpretation of the magnetic properties of the perovskite-type mixed crystals La1−xSrxCoO3−λ,J. Chem. Phys. Solids6,287(1958).
[15] NaimanC. S.,GilmoreR.,DiBartoloB.,LinzA. andSantoroR.,Lanthanum rhodium and lanthanum cobalt oxides,J. Appl. Phys.36,1044(1965).
[16] RaccahP. M. andGoodenoughJ. B.,First-order localized-electron collective-electron transition in LaCoO3,Phys. Rev.155,932(1967).
[17] BhideV. G.,RajoriaD. S.,RaoG. R. andRaoC. N. R.,Mössbauer studies of the high-spin-low-spin equilibria and the localized-collective electron transition in LaCoO3,Phys. Rev. B6,1021(1972).
[18] KorotinM. A.,EzhovS. Yu.,SolovyevI. V.,AnisimovV. I.,KhomskiiD. I. andSawatzkyG. A.,Electronic and spin configurations of Co3+ and Ni3+ ions in oxides of K2NiF4 structure: A magnetic susceptibility study,Phys. Rev. B54,5309(1996).
[19] NatileM. M.,UgelE.,MaccatoC. andGlisentiA.,LaCoO3: Effect of synthesis conditions on properties and reactivity,Appl. Catal. B72,351(2007).
[20] KoehlerW. C. andWollanE. O.,Neutron-diffraction study of the magnetic properties of perovskite-like compounds LaBO3,J. Phys. Chem. Solids2,100(1957).
[21] SeoJ. W.,FullertonE. E.,NoltingF.,SchollA.,FompeyrineJ. andLocquetJ. P.,Antiferromagnetic LaFeO3 thin films and their effect on exchange bias,J. Phys. Condens. Matter20,264014(2008).
[22] AcharyaS.,MondalJ.,GhoshS.,RoyS. K. andChakrabartiP. K.,Multiferroic behavior of lanthanum orthoferrite (LaFeO3),Mater. Lett.64,415(2010).
[23] PhokhaS.,PinitsoontornS.,MaensiriS. andRujirawatS.,Structure, optical and magnetic properties of LaFeO3 nanoparticles prepared by polymerized complex method,J. Sol-Gel Sci. Technol.71,333(2014).
[24] MitraA.,MahapatraA. S.,MallickA.,ShawA.,GhoshM. andChakrabartiP. K.,Simultaneous enhancement of magnetic and ferroelectric properties of LaFeO3 by co-doping with Dy3+ and Ti4+,J. Alloy. Comp.726,1195(2017).
[25] FuhH.-R.,WengK.-C.,LiuY.-P. andWangY.-K.,New ferromagnetic semiconductor double perovskites: La2FeMO6 (M = Co, Rh, and Ir),J. Alloy. Comp.622,657(2015).
[26] FuhH.-R.,WengK.-C.,ChangC.-R. andWangY.-K.,Electronic structure of ferromagnetic semiconductor material on the monoclinic and rhombohedral ordered double perovskites La2FeCoO6,J. Appl. Phys.117,17B902(2015).
[27] TirmaliP. M.,MishraD. K.,BenglorkarB. P.,ManeS. M.,KadamS. L. andKulkarniS. B.,Structural, magnetic and dielectric relaxation behaviour study of La2MnCoO6 and fully substituted B-site La2FeCoO6,J. Chin. Adv. Mater. Soc.6,207(2018).
[28] GinellK. M.,HornC.,Von DreeleR. B. andTobyB. H.,Materials for learning use of GSAS-II,Powder Diffr.34,184(2019).
[29] TobyB. H.,EXPGUI, a graphical user interface for GSAS,J. Appl. Cryst.34,210(2001).
[30] Alarcón-SuescaC. E.,Deluque ToroC. E.,Gil RebazaA. V.,Landínez TéllezD. A. andRoa-RojasJ.,Ab-initio studies of electronic, structural and thermophysical properties of the Sr2TiMoO6 double perovskite,J. Alloys Compd.771,1080(2019).
[31] CullityB. D.,Elements of X-ray Diffraction,2nd edn.(Addison Wesley Publishing Company,Reading, MA,1978).
[32] SaleemM.,FangL.,RuanH. B.,WuF.,HuangQ. L.,XuC. L. andKongC. Y.,Effect of zinc acetate concentration on the structural and optical properties of ZnO thin films deposited by Sol-Gel method,Int. J. Phys. Sci.7,2971(2012).
[33] KumarB. R. andHymavathiB.,X-ray peak profile analysis of solid-state sintered alumina doped zinc oxide ceramics by Williamson–Hall and size-strain plot methods,J. Asian Ceram. Soc.5,94(2017).
[34] ParthéE.,GelatoL.,ChabotB.,PenzoM.,CenzualK. andGladyshevskiiR.,TYPIX Standardized and crystal chemical characterization of inorganic structure types, inGmelein Handbook of Inorganic and Organometallic Chemistry,8th edn.(Springer,Berlin,1993).
[35] WondratschekW.,Special topics on space groups, inInternational Tables for Crystallography, Vol.A,Chap. 8.3(International Union of Crystallography2006), p.732.
[36] GlazerA. M.,The classification of tilted octahedra in perovskites,Acta Cryst. B28,3384(1972).
[37] SchneiderC. A.,RasbandW. S. andEliceiriK. W.,NIH image to ImageJ: 25 years of image analysis,Nat. Meth.9,671(2012).
[38] AguiarE. C.,RamirezM. A.,CortesJ. A.,RochaL. S.,BorsariaE. andSimõesA. Z.,Magnetoelectric coupling of LaFeO3/BiFeO3 heterostructures,Ceram. Int.41,13126(2015).
[39] YaoQ.,TianCh.,WangJ.,ZhouH. andRaoG.,Antiferromagnetic-ferromagnetic transition in Bi-doped LaFeO3 nanocrystalline ceramics,Ceram. Int.46,20472(2020).
[40] WeiheH. andGüdelH. U.,Quantitative interpretation of the Goodenough-Kanamori rules: A critical analysis,Inorg. Chem.36,3632(1997).
[41] KhetreaS. M.,JadhavH. V.,JagadaleP. N.,KulalS. R. andBamaneS. R.,Studies on electrical and dielectric properties of LaFeO3,Adv. Appl. Sci. Res.2,503(2011).
[42] SudheendraL.,SeikhM.,RajuA. R.,NarayanaC. andRaoC. N. R.,Dielectric properties of rare earth cobaltates, LnCoO3 (Ln = La, Pr, Nd), across the spin-state transition,Ferroelectrics,306,227(2004).
[43] FelixJ. F.,da SilvaE. F.Jr,De VasconcelosE. A. andde AzevedoW. M.,Tailoring the electrical properties of ZnO/Polyaniline heterostructures for device applications,J. Korean Phys. Soc.58,1256(2011).
[44] Cuervo FarfánJ. A.,Deluque ToroC. E.,Parra VargasC. A.,Landínez TéllezD. A. andRoa-RojasJ.,Experimental and theoretical determination of physical properties of Sm2Bi2Fe4O12 ferromagnetic semiconductors,J. Mater. Chem. C8,14925(2020).
[45] VojtaA.,WenQ. andClarkeD. R.,Influence of microstructural disorder on the current transport behavior of varistor ceramics,Comput. Mater. Sci.6,51(1996).
[46] PandeyR. K.,StapletonW. A. andSutantoI.,The effect of doping with some rare earth oxides on electrical features of ZnO,IEEE J. Electron Dev. Soc.3,276(2015).
[47] JüngelA.,Quasi-hydrodynamic Semiconductor Equations(Springer Basel AG, 2001).