Magnetic and Magnetoelectric Properties of AurivilliusThree- and Four-Layered Intergrowth Ceramics

In this work, we have prepared intergrowth of multiferroic compounds namely Bi4RTi3Fe0.7Co0.3O15-Bi3RTi2Fe0.7Co0.3O12−δ (BRTFCO15-BRTFCO12) (rare earth (R) = Dy, Sm, La) by solid-state reaction method. From the X-ray diffraction Rietveld refinement, the structure of the intergrowths was found to be orthorhombic in which satisfactory fittings establish the existence of three-layered (space group: b 2 c b) and four-layered compounds (space group: A21am). Analysis of magnetic measurements confirmed a larger magnetization for theSm-modified intergrowth compound (BSTFCO15-BSTFCO12) compared to Dy- and La-doped ones. The emergence of higher magnetic properties can be due to distortion in the unit cell when some Bi3+ ions are replaced with the Sm3+, bonding of Fe3+-O-Co3+ as well as a possible mixture of FexCoy-type nanoparticles that are formed generally in the synthesis of intergrowths. The changes in the magnetic state of the Aurivillius intergrowths have been reflected in the magnetoelectric (ME) coupling: higher ME coefficient (~30 mV/Cm-Oe) at lower magnetic fields and is constant up to 3 kOe. The results were corroborated by Raman spectroscopy and variation of temperature with magnetization data. The results revealed that the RE-modified intergrowth route is an effective preparative method for higher-layer Aurivillius multiferroic ceramics.

[1]  M. Nazemian,et al.  The enhanced of magnetic and electrical properties of Bi5FeTi3O15 compound with replacing Co for Ti sites , 2023, Journal of Magnetism and Magnetic Materials.

[2]  Venkata Sreenivas Puli,et al.  Electrical and magnetic studies on promising Aurivillius intergrowth compound , 2022, Journal of Materials Science: Materials in Electronics.

[3]  J. Eiras,et al.  Room-temperature multiferroic behaviour in Co/Fe co-substituted layer-structured Aurivillius phase ceramics , 2022, Ceramics International.

[4]  N. Lomanova Aurivillius Phases Bim+ 1Fem– 3Ti3O3m+ 3: Synthesis, Structure, and Properties (a Review) , 2022, Russian Journal of Inorganic Chemistry.

[5]  Yamei Zhang,et al.  Breakdown field enhancement and energy storage performance in four-layered Aurivillius films , 2022, Ceramics International.

[6]  S. Tidrow,et al.  Tailoring the ferroelectric and magnetic properties of Bi5Ti3FeO15 ceramics by doping with Co and Y , 2021, Solid State Sciences.

[7]  Xiaofeng Yin,et al.  Progress and Perspectives on Aurivillius-Type Layered Ferroelectric Oxides in Binary Bi4Ti3O12-BiFeO3 System for Multifunctional Applications , 2020, Crystals.

[8]  Feiyu Liu,et al.  Multiferroic properties of Bi5.75R0.25Fe1.4Ni0.6Ti3O18 (R = Eu, Sm, Nd, Bi and La) ceramics , 2020 .

[9]  F. Bohn,et al.  Effects of the Bi3+ substitution on the structural, vibrational, and magnetic properties of bismuth layer-structured ferroelectrics , 2020, Applied Physics A.

[10]  Xiangping Jiang,et al.  Effect of tantalum substitution on the structural and electrical properties of BaBi8Ti7O27 intergrowth ceramics , 2020 .

[11]  Zhijun Ma,et al.  Room temperature multiferroic properties of rare-earth-substituted Aurivillius phase Bi5Ti3Fe0.7Co0.3O15 ceramics , 2019, Materials Research Bulletin.

[12]  G. Prasad,et al.  Electrical and Raman Spectroscopic Studies on Aurivillius Layered-Pervoskite Ceramics , 2019, Advanced Materials Research.

[13]  F. Liu,et al.  Structural, electrical and photoluminescence properties of Er3+-doped SrBi4Ti4O15—Bi4Ti3O12 inter-growth ceramics , 2019, Frontiers of Materials Science.

[14]  L. Wang,et al.  Temperature dependent conductivity of Bi4Ti3O12 ceramics induced by Sr dopants , 2018, Journal of Advanced Ceramics.

[15]  E. Devi,et al.  Law of Approach to Saturation in Mn–Zn Ferrite Nanoparticles , 2018, Journal of Superconductivity and Novel Magnetism.

[16]  G. Hu,et al.  Enhanced ferro-and piezoelectric properties of Bi4Ti3O12-CaBi4Ti4O15 thin film on Pt(111)/Ti/SiO2/Si substrate , 2018 .

[17]  M. Mendoza,et al.  Raman effect in multiferroic Bi5Fe1+xTi3−xO15 solid solutions: A temperature study , 2018 .

[18]  R. Iskhakov,et al.  Law of approach to magnetic saturation in nanocrystalline and amorphous ferromagnets with improved transition behavior between power-law regimes , 2017 .

[19]  Yalin Lu,et al.  Engineering the exchange bias and bias temperature by modulating the spin glassy state in single phase Bi9Fe5Ti3O27. , 2017, Nanoscale.

[20]  Shengyu Zhu,et al.  Structural and electrical properties of La3+-doped Na0.5Bi4.5Ti4O15-Bi4Ti3O12 inter-growth high temperature piezoceramics , 2017 .

[21]  Z. Chen,et al.  Structure Evolution and Multiferroic Properties in Cobalt Doped Bi4NdTi3Fe1-xCoxO15-Bi3NdTi2Fe1-xCoxO12-δ Intergrowth Aurivillius Compounds , 2017, Scientific Reports.

[22]  María J. Hortigüela,et al.  Effect of samarium and vanadium co-doping on structure, ferroelectric and photocatalytic properties of bismuth titanate , 2017 .

[23]  Y. Huang,et al.  Layer Effects on the Magnetic Behaviors of Aurivillius Compounds Bin+1Fen−3Ti3O3n+1 (n = 6, 7, 8, 9) , 2016 .

[24]  S. Khalid,et al.  Dielectric relaxations and electrical properties of Aurivillius Bi3.5La0.5Ti2Fe0.5Nb0.5O12 ceramics , 2016 .

[25]  Xiaomei Lu,et al.  Multiferroic properties and magnetoelectric coupling in Fe/Co co-doped Bi3.25La0.75Ti3O12 ceramics , 2015 .

[26]  J. Chu,et al.  Cryogenic temperature relaxor-like dielectric responses and magnetodielectric coupling in Aurivillius Bi5Ti3FeO15 multiferroic thin films , 2014 .

[27]  E. Ramana,et al.  Observation of magnetoelectric coupling and local piezoresponse in modified (Na0.5Bi0.5)TiO3-BaTiO3-CoFe2O4 lead-free composites. , 2014, Dalton transactions.

[28]  S. Bhardwaj,et al.  Room-temperature multiferroic properties and magnetoelectric coupling in Bi4−xSmxTi3−xCoxO12−δ ceramics , 2014, Journal of Materials Science.

[29]  S. Bhardwaj,et al.  Room temperature multiferroic properties and magnetoelectric coupling in Sm and Ni substituted Bi4−xSmxTi3−xNixO12±δ (x = 0, 0.02, 0.05, 0.07) ceramics , 2014 .

[30]  J. Bera,et al.  Electrical properties of niobium doped Bi4Ti3O12-SrBi4Ti4O15 intergrowth ferroelectrics , 2014 .

[31]  Y. Jia,et al.  Synthesis of the superlattice complex oxide Sr5Bi4Ti8O27 and its band gap behavior , 2012 .

[32]  W. Cao,et al.  Large magnetic response in (Bi4Nd)Ti3(Fe0.5Co0.5)O15 ceramic at room-temperature , 2011 .

[33]  C. Wang,et al.  Structural, magnetic and dielectric properties of Bi5−xLaxTi3Co0.5Fe0.5O15 ceramics , 2011 .

[34]  M. Čeh,et al.  Structural evolution of the intergrowth bismuth-layered Bi7Ti4NbO21 , 2011, Journal of Materials Science.

[35]  Yongxiang Li,et al.  The Formation Mechanism of Intergrowth Bismuth Layer-Structured Ferroelectric Bi4Ti3O12-CaBi4Ti4O15 , 2010 .

[36]  E. Kharitonova,et al.  Synthesis and electrical properties of mixed-layer Aurivillius phases , 2007 .

[37]  S. Wu,et al.  Substitution of Sm3+ and Nd3+ for Bi3+ in SrBi8Ti7O27 Mixed Aurivillius Phase , 2003 .

[38]  Y. Noguchi,et al.  Ferroelectric properties of intergrowth Bi4Ti3O12–SrBi4Ti4O15 ceramics , 2000 .

[39]  K. Uchida,et al.  A family of mixed-layer type bismuth compounds , 1977 .

[40]  E. Subbarao,et al.  A family of ferroelectric bismuth compounds , 1962 .

[41]  G. Prasad,et al.  Structure and dielectric properties of Sm3+ modified Bi4Ti3O12- SrBi4Ti4O15 intergrowth ferroelectrics , 2020 .

[42]  P. R. Graves,et al.  The Raman Modes of the Aurivillius Phases: Temperature and Polarization Dependence , 1995 .