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Journal ArticleDOI

Magnetic, magnetocapacitance and dielectric properties of Cr doped bismuth ferrite nanoceramics

Abstract
BiFe 1− x Cr x O 3 ( x  = 0, 004, 006 and 008) nanoceramics were prepared by sol–gel method Nanoceramics were calcined at 450 °C Calcined powders were leached in diluted nitric acid to get single phase TEM analysis shows the particle size to be ∼80 nm Thermogravimetric analysis of as prepared powder indicates that the single phase is formed at around 450 °C Magnetization was found to increase as the concentration of Cr was increased Dielectric constant and dielectric loss were found to decrease with increase in frequency for all the compositions Magnetocapacitance was found to increase with magnetic field For BiFe 1− x Cr x O 3 ( x  = 004, 006 and 008) nanoceramics, the change of dielectric constant induced by magnetic field may be well approximated by Δ ɛ / ɛ  =  γ M 2 , here, γ (magnetoelectric interaction) is small and positive A linear fit gave the value of γ of ∼184 × 10 −2 , 123 × 10 −2 and 33 × 10 −2 for BiFe 1− x Cr x O 3 ( x  = 004, 006 and 008) nanoceramics, respectively

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Study of structural, dielectric and magnetic behaviour of Ni0.75Zn0.25Fe2O4–Ba(Ti0.85Zr0.15)O3 composites

TL;DR: In this paper, a class of hybrid composites (x)Ni0.75Zn0.25Fe2O4?(1???x)Ba(Ti 0.85Zr 0.15)O 3 synthesized via a solid state reaction method is investigated.
Journal ArticleDOI

Study of structural, electrical, magnetic and optical properties of 0.65BaTiO3–0.35Bi0.5Na0.5TiO3–BiFeO3 multiferroic composite

TL;DR: In this paper, a solid state reaction method was used to prepare (1 − x )[0.65BaTiO 3 −0.35Bi 0.5 Na 0.20] composite.
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Enhanced multiferroic properties in La and Ce co-doped BiFeO3 nanoparticles

TL;DR: In this article, Raman et al. showed that the (La,Ce) co-doped sample possesses dense microstructure made of smaller particles, and the Raman study accounts for the weakening of the strong hybridization between Bi-O by the substitution of La and Ce ions.
References
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Journal ArticleDOI

Multiferroic and magnetoelectric materials

TL;DR: A ferroelectric crystal exhibits a stable and switchable electrical polarization that is manifested in the form of cooperative atomic displacements that arises through the quantum mechanical phenomenon of exchange.
Journal ArticleDOI

Revival of the Magnetoelectric Effect

Abstract: Recent research activities on the linear magnetoelectric (ME) effect?induction of magnetization by an electric field or of polarization by a magnetic field?are reviewed. Beginning with a brief summary of the history of the ME effect since its prediction in 1894, the paper focuses on the present revival of the effect. Two major sources for 'large' ME effects are identified. (i) In composite materials the ME effect is generated as a product property of a magnetostrictive and a piezoelectric compound. A linear ME polarization is induced by a weak ac magnetic field oscillating in the presence of a strong dc bias field. The ME effect is large if the ME coefficient coupling the magnetic and electric fields is large. Experiments on sintered granular composites and on laminated layers of the constituents as well as theories on the interaction between the constituents are described. In the vicinity of electromechanical resonances a ME voltage coefficient of up to 90?V?cm?1?Oe?1 is achieved, which exceeds the ME response of single-phase compounds by 3?5 orders of magnitude. Microwave devices, sensors, transducers and heterogeneous read/write devices are among the suggested technical implementations of the composite ME effect. (ii) In multiferroics the internal magnetic and/or electric fields are enhanced by the presence of multiple long-range ordering. The ME effect is strong enough to trigger magnetic or electrical phase transitions. ME effects in multiferroics are thus 'large' if the corresponding contribution to the free energy is large. Clamped ME switching of electrical and magnetic domains, ferroelectric reorientation induced by applied magnetic fields and induction of ferromagnetic ordering in applied electric fields were observed. Mechanisms favouring multiferroicity are summarized, and multiferroics in reduced dimensions are discussed. In addition to composites and multiferroics, novel and exotic manifestations of ME behaviour are investigated. This includes (i) optical second harmonic generation as a tool to study magnetic, electrical and ME properties in one setup and with access to domain structures; (ii) ME effects in colossal magnetoresistive manganites, superconductors and phosphates of the LiMPO4 type; (iii) the concept of the toroidal moment as manifestation of a ME dipole moment; (iv) pronounced ME effects in photonic crystals with a possibility of electromagnetic unidirectionality. The review concludes with a summary and an outlook to the future development of magnetoelectrics research.
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Why Are There so Few Magnetic Ferroelectrics

TL;DR: In this paper, the fundamental physics behind the scarcity of ferromagnetic ferroelectric coexistence was explored and the properties of known magnetically ordered ferro-electric materials were examined.
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Spiral magnetic ordering in bismuth ferrite

TL;DR: In this article, the magnetic ordering of the iron ions in bismuth ferrite BiFeO3 was obtained by a study with a high-resolution time-of-flight neutron diffractometer.
Journal ArticleDOI

Magnetoelectric phase diagrams of orthorhombic R MnO 3 ( R = Gd , Tb, and Dy)

TL;DR: The magnetoelectric phase diagram of rare-earth manganites with orthorhombically distorted perovskite structure has been investigated in this paper, showing that a ferroelectric phase with electric polarization along the $a$ axis appears by applying $H(g\ensuremath{\sim}1\phantom{\rule{0.3em}{0ex}}\mathrm{T})$ along the b$ axis.
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