Electric-field control of non-volatile magnetization switching without external-magnetic-field bias in CoFeB/(011)-PMN-0.3PT heterostructures

Lane formation dynamics in externally driven pair-ion plasma (PIP) particles is studied in the presence of external magnetic field using Langevin dynamics (LD) simulation. The phase diagram obtained distinguishing the no-lane and lane states is systematically determined from a study of various Coulomb coupling parameter values. A peculiar lane formation-disintegration parameter space is identified; lane formation area extended to a wide range of Coulomb coupling parameter values is observed before disappearing to a mixed phase. The different phases are identified by calculating the order parameter. This and the critical parameters are calculated directly from LD simulation. The critical electric field strength value above which the lanes are formed distinctly is obtained, and it is observed that in the presence of the external magnetic field, the PIP system requires a higher value of the electric field strength to enter into the lane formation state than that in the absence of the magnetic field. We further find out the critical value of electric field frequency beyond which the system exhibits a transition back to the disordered state and this critical frequency is found as an increasing function of the electric field strength in the presence of an external magnetic field. The movement of the lanes is also observed in a direction perpendicular to that of the applied electric and magnetic field directions, which reveals the existence of the electric field drift in the system under study. We also use an oblique force field as the external driving force, both in the presence and absence of the external magnetic field. The application of this oblique force changes the orientation of the lane structures for different applied oblique angle values.

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Adjustability of resonance frequency by external magnetic field and bias electric field of sandwich magnetoelectric PZT/NFO/PZT composites

Applied Physics A ◽

10.1007/s00339-017-1082-3 ◽

2017 ◽

Vol 123 (7) ◽

Cited By ~ 2

Author(s):

Ling-Fang Xu ◽

Xing Feng ◽

Kang Sun ◽

Ze-Yu Liang ◽

Qian Xu ◽

...

Keyword(s):

Magnetic Field ◽

External Magnetic Field ◽

Electric Field ◽

Resonance Frequency ◽

Bias Electric Field

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Large linear magnetoelectric effect and field-induced ferromagnetism and ferroelectricity in DyCrO4

NPG Asia Materials ◽

10.1038/s41427-019-0151-9 ◽

2019 ◽

Vol 11 (1) ◽

Cited By ~ 3

Author(s):

Xudong Shen ◽

Long Zhou ◽

Yisheng Chai ◽

Yan Wu ◽

Zhehong Liu ◽

...

Keyword(s):

Magnetic Field ◽

Electric Field ◽

Spin Structure ◽

Magnetoelectric Effect ◽

Electric Polarization ◽

Metamagnetic Transition ◽

Ferromagnetic Component ◽

Antiferromagnetic Structure ◽

Field Control ◽

Ferromagnetic Magnetization

Abstract All the magnetoelectric properties of scheelite-type DyCrO4 are characterized by temperature- and field-dependent magnetization, specific heat, permittivity, electric polarization, and neutron diffraction measurements. Upon application of a magnetic field within ±3 T, the nonpolar collinear antiferromagnetic structure leads to a large linear magnetoelectric effect with a considerable coupling coefficient. An applied electric field can induce the converse linear magnetoelectric effect, realizing magnetic field control of ferroelectricity and electric field control of magnetism. Furthermore, a higher magnetic field (>3 T) can cause a metamagnetic transition from the initially collinear antiferromagnetic structure to a canted structure, generating a large ferromagnetic magnetization up to 7.0 μB f.u.−1. Moreover, the new spin structure can break the space inversion symmetry, yielding ferroelectric polarization, which leads to coupling of ferromagnetism and ferroelectricity with a large ferromagnetic component.

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Relationship Between In-Situ Electric Field and External Magnetic Field Strength in Human Models-Rational of IEEE C95.6 Standard Revisited

2018 International Symposium on Electromagnetic Compatibility (EMC EUROPE) ◽

10.1109/emceurope.2018.8485010 ◽

2018 ◽

Author(s):

Katsuaki Aga ◽

Akimasa Hirata ◽

Ilkka Laakso

Keyword(s):

Magnetic Field ◽

External Magnetic Field ◽

Field Strength ◽

Electric Field ◽

Magnetic Field Strength ◽

Human Models ◽

External Magnetic Field Strength

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Magnetization switching in ferromagnets by adsorbed chiral molecules without current or external magnetic field

Nature Communications ◽

10.1038/ncomms14567 ◽

2017 ◽

Vol 8 (1) ◽

Cited By ~ 52

Author(s):

Oren Ben Dor ◽

Shira Yochelis ◽

Anna Radko ◽

Kiran Vankayala ◽

Eyal Capua ◽

...

Keyword(s):

Magnetic Field ◽

External Magnetic Field ◽

Chiral Molecules ◽

Magnetization Switching

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Electrostatic ion-cyclotron instability caused by a nonuniform electric field perpendicular to the external magnetic field

The Physics of Fluids ◽

10.1063/1.865096 ◽

1985 ◽

Vol 28 (3) ◽

pp. 761 ◽

Cited By ~ 106

Author(s):

G. Ganguli ◽

Y. C. Lee ◽

P. Palmadesso

Keyword(s):

Magnetic Field ◽

External Magnetic Field ◽

Electric Field ◽

Nonuniform Electric Field ◽

Cyclotron Instability ◽

Ion Cyclotron

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Electric Field-Induced Magnetization Reversal of Multiferroic Nanomagnet

Magnetic Materials and Magnetic Levitation ◽

10.5772/intechopen.91231 ◽

2021 ◽

Author(s):

Jiahao Liu ◽

Liang Fang

Keyword(s):

Magnetic Field ◽

Integrated Circuits ◽

Electric Field ◽

Magnetization Reversal ◽

Logic Gate ◽

Electronic Systems ◽

Spintronic Devices ◽

Nanomagnetic Logic ◽

Field Control ◽

Application Potential

Using the inverse piezoelectric effect and inverse magnetostrictive effect in a multiferroic heterojunction, an electric field is able to control the magnetization switching of a uniaxial nanomagnet. Compared with traditional spintronic devices based on magnetic field, multiferroic nanomagnet devices have the advantages of ultra-low consumption and high radiation resistance, showing great application potential in modern high-integrated circuits and military electronic systems. However, the difficulties of electric field control of complete magnetization reversal of the nanomagnet and nanomagnet arrays in a nanomagnetic logic gate still restrict the developments of multiferroic nanomagnet device. In this chapter, the uniaxial nanomagnets in multiferroic heterojunctions are mainly discussed. The two core problems of the electric field control of nanomagnets and nanomagnetic logic gate are well solved.

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Trade-oﬀ in perpendicular electric ﬁeld control using negatively biased emissive end-electrodes

Plasma Sources Science and Technology ◽

10.1088/1361-6595/ac4847 ◽

2022 ◽

Author(s):

Baptiste Trotabas ◽

Renaud Gueroult

Keyword(s):

Magnetic Field ◽

Electric Field ◽

Thermionic Emission ◽

Potential Drop ◽

Plasma Potential ◽

Magnetized Plasma ◽

Trade Off ◽

Sheath Edge ◽

Field Control ◽

Field Lines

Abstract The beneﬁts of thermionic emission from negatively biased electrodes for perpendicular electric ﬁeld control in a magnetized plasma are examined through its combined eﬀects on the sheath and on the plasma potential variation along magnetic ﬁeld lines. By increasing the radial current ﬂowing through the plasma thermionic emission is conﬁrmed to improve control over the plasma potential at the sheath edge compared to the case of a cold electrode. Conversely, thermionic emission is shown to be responsible for an increase of the plasma potential drop along magnetic ﬁeld lines in the quasi-neutral plasma. These results suggest that there exists a trade-oﬀ between electric ﬁeld longitudinal uniformity and amplitude when using negatively biased emissive electrodes to control the perpendicular electric ﬁeld in a magnetized plasma.

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