Results 201 to 210 of about 15,176,180 (253)
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Multiplied magnetoelectric effect in multi-faceted magnetoelectric composite
Applied Physics Letters, 2014A four-faceted magnetoelectric (ME) composite consisting of one cuboid bonded Terfenol-D composite and four plates of Pb(Zr,Ti)O3 (PZT) was fabricated. The ME voltage coefficients were measured along the length direction of the composite when PZT plates were parallelly or serially connected.
Z. J. Zuo +6 more
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MAGNETOELECTRIC EFFECTS IN MULTIFERROICS
Izvestia Ufimskogo Nauchnogo Tsentra RAN, 2021Research of magnetoelectric effects and multiferroic materials, in which these effects are manifested, is among key areas in modern magnetism. This is associated with promising aspects of applying the results to spintronics, orbitronics, and new generation systems for information storage and processing.
Z.V. GAREEVA, E.I. BADERTDINOVA
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Lack of linear magnetoelectric effect in ferrimagnetic distorted honeycomb Ni4Nb2O9
, 2020M4A2O9 transition metal oxides, with M a divalent cation and A Nb or Ta, that exhibit a structure derived from corundum constitute an interesting class of materials due to their possible magnetoelectric properties.
E. Tailleur +4 more
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Magnetoelectric effect in superconductors with d -wave magnetization
Physical review BWe report on a study of the interplay between the supercurrent and spin-polarization in a two-dimensional superconducting system in the presence of a d-wave symmetric antiferromagnetic exchange interaction (altermagnetism).
A. Zyuzin
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Materials Today Chemistry, 2021
Ba0.8Sr0.2TiO3 (BST) and Cu0.5Co0.5Fe2O4 (CCFO) nanopowders were prepared by hydrothermal method and chemical coprecipitation, respectively. Barium strontium titanate nanopowder–nano mixed oxides containing copper, cobalt, and iron (BST-CCFO ...
H. Wu +10 more
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Ba0.8Sr0.2TiO3 (BST) and Cu0.5Co0.5Fe2O4 (CCFO) nanopowders were prepared by hydrothermal method and chemical coprecipitation, respectively. Barium strontium titanate nanopowder–nano mixed oxides containing copper, cobalt, and iron (BST-CCFO ...
H. Wu +10 more
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Magnetoelectric Effect in Polar Superconductors
Physical Review Letters, 1995The question of how the lack of spatial reflection symmetry can affect properties of a superconductor is investigated. A novel magnetoelectric effect is predicted: The supercurrent in a metal of polar symmetry must be accompanied by the spin polarization of the carriers. The relevance to some known pyro- and antipyroelectric superconductors including a
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Theoretical investigation of magnetoelectric effect in multilayer magnetoelectric composites
Composite Structures, 2015Abstract The aim of this paper is the modeling of an arbitrary magneto–elasto-electric multilayer constitute by magnetostrictive, piezoelectric and elastic substrate layers under free–free boundary conditions. A dynamic theory corresponding to the driving frequency of magnetoelectric (ME) response coupled flexural and extensional oscillations was ...
Guo-Liang Yu +4 more
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Computational materials science, 2019
A multiscale numerical investigation into the origin of the magnetoelectric effect in multiferroic composite materials was performed. Specifically, a well-known but unconfirmed mechanism for generating a macroscopic magnetoelectric effect through ...
Y. Uetsuji, T. Wada, K. Tsuchiya
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A multiscale numerical investigation into the origin of the magnetoelectric effect in multiferroic composite materials was performed. Specifically, a well-known but unconfirmed mechanism for generating a macroscopic magnetoelectric effect through ...
Y. Uetsuji, T. Wada, K. Tsuchiya
semanticscholar +1 more source
Magnetoelectric Effects in Antiferromagnetics
Journal of Applied Physics, 1962Spin-ordered materials may exhibit a magnetic polarization which is proportional to an applied electric field and an electric polarization which is proportional to an applied magnetic field. In this paper a comprehensive discussion is given of the present knowledge of these magnetoelectric (ME) effects.
G. T. Rado, V. J. Folen
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Magnetoelectric Effect for Phonons
2021The phonon angular momentum for each mode \(\mathbf {l}_{\sigma }\) is an odd (even) function of phonon wave vector \(\mathbf {k}\) when the system has time-reversal (inversion) symmetry. Thus, to make phonon angular momentum nonzero \(\mathbf {l}_{\sigma }(\mathbf {k})\ne 0\), at least one of these symmetries must be broken.
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