2015
DOI: 10.1063/1.4913616
|View full text |Cite
|
Sign up to set email alerts
|

Electrical controlled magnetism in FePt film with the coexistence of two phases

Abstract: A series of FePt films with different magnetic structures are deposited on Pb(Mg1/3Nb2/3)O3–PbTiO3 substrates. By applying an electric field across the piezoelectric single crystal substrate, an magnetoelectric effect is observed in FePt/Pb(Mg1/3Nb2/3)O3–PbTiO3 heterostructure due to the phase transformation between face-centered cubic and face-centered tetragonal phases in the film. Taking advantage of the different coercivity caused by the electric field, the sign of magnetization can be manipulated reversib… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
5
0

Year Published

2016
2016
2023
2023

Publication Types

Select...
7

Relationship

0
7

Authors

Journals

citations
Cited by 9 publications
(5 citation statements)
references
References 28 publications
(37 reference statements)
0
5
0
Order By: Relevance
“…Furthermore, because the maximum deformation magnitude of ferroelectrics is usually below 1%, , the transferrable lattice strain in the attached film is normally limited to be less than 0.5%. The strain induced magnetoelastic energy to the film (∼10 4 J/m 3 ) can only achieve values comparable to the magnetocrystalline anisotropy energy of low K u materials such as Ni, Co, CoFe, ,, the effective H C tunability in large K u materials , is very limited. The achievable lattice strain, H C variation, and sensitivity of H C change to strain level in some typical magnetic materials deposited on ferroelectric substrates ,,,, are summarized in Figure S1.…”
Section: Introductionmentioning
confidence: 99%
“…Furthermore, because the maximum deformation magnitude of ferroelectrics is usually below 1%, , the transferrable lattice strain in the attached film is normally limited to be less than 0.5%. The strain induced magnetoelastic energy to the film (∼10 4 J/m 3 ) can only achieve values comparable to the magnetocrystalline anisotropy energy of low K u materials such as Ni, Co, CoFe, ,, the effective H C tunability in large K u materials , is very limited. The achievable lattice strain, H C variation, and sensitivity of H C change to strain level in some typical magnetic materials deposited on ferroelectric substrates ,,,, are summarized in Figure S1.…”
Section: Introductionmentioning
confidence: 99%
“…Electric field (E-field) modulates magnetism is one of the most energy-efficient pathways toward fast, compact, and light-weight devices. Conventional magnetoelectric (ME) devices based on rigid, planar chips achieve voltage control magnetism by the virtue of a strain-induced inverse magnetostriction effect or interface charge accumulation. For flexible ME devices, the materials will be bent, stretched, or even twisted, and such variable strain conditions are fatal for strain-mediated ME coupling . In contrast, the charge-mediated ME coupling mechanism became a practical approach.…”
mentioning
confidence: 99%
“…The remarkable strain transfer on membranes bonded by SU-8 is attributed to the excellent wettability of the polymer when heated up during the bonding process, which fills the gaps between the PMN-PT and the membrane. Moreover, the observed strain transfer efficiency is higher than that reported on epitaxially grown SrTiO3:Ni 2+ or NdNiO3/SrTiO3 or thin films on PMN-PT substrates [62,63], and similar to epitaxial La0.335Pr0.335Ca0.33MnO3 films [64] with a thickness 10 times lower than the GaAs membranes employed in Ref. [50].…”
Section: 23-nanomembranes Transferred By Polymer-based Bondingmentioning
confidence: 55%