2021
DOI: 10.1002/adfm.202107135
|View full text |Cite
|
Sign up to set email alerts
|

Engineering of Ferroic Orders in Thin Films by Anionic Substitution

Abstract: Multiferroics are a unique class of materials where magnetic and ferroelectric orders coexist. The research on multiferroics contributes significantly to the fundamental understanding of the strong correlations between different material degrees of freedom and provides an energy‐efficient route toward the electrical control of magnetism. While multiple ABO3 oxide perovskites are identified as being multiferroic, their magnetoelectric coupling strength is often weak, necessitating the material search in differe… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

1
6
0
1

Year Published

2022
2022
2024
2024

Publication Types

Select...
10

Relationship

1
9

Authors

Journals

citations
Cited by 12 publications
(8 citation statements)
references
References 61 publications
1
6
0
1
Order By: Relevance
“…With these Hubbard-U parameters, we obtained an equilibrium lattice parameter for cubic BSO, a = 4.118 Å (SNO: 4.044 Å), comparable to our DFT relaxed lattice parameter of 4.178 Å (SNO: 4.061 Å), and in excellent agreement with the experiment, 4.115 Å (SNO: 4.020 Å). The BSO band gap increases from 0.4 eV (DFT) to 3.6 eV (ACBN0), closer to the experimental band gap of 3.1 eV, while SNO remains non-magnetic metal, consistent with previous theory and experiment . We built different (BSO) N /(SNO) M heterostructures ( N , M refer to the number of cubic unit cells in each stack): (BSO)­4/(SNO)­2, (BSO)­4/(SNO)­4, (BSO)­6/(SNO)­6, (BSO)­7/(SNO)­7, and (BSO)­8/(SNO)­8.…”
Section: Methodssupporting
confidence: 84%
“…With these Hubbard-U parameters, we obtained an equilibrium lattice parameter for cubic BSO, a = 4.118 Å (SNO: 4.044 Å), comparable to our DFT relaxed lattice parameter of 4.178 Å (SNO: 4.061 Å), and in excellent agreement with the experiment, 4.115 Å (SNO: 4.020 Å). The BSO band gap increases from 0.4 eV (DFT) to 3.6 eV (ACBN0), closer to the experimental band gap of 3.1 eV, while SNO remains non-magnetic metal, consistent with previous theory and experiment . We built different (BSO) N /(SNO) M heterostructures ( N , M refer to the number of cubic unit cells in each stack): (BSO)­4/(SNO)­2, (BSO)­4/(SNO)­4, (BSO)­6/(SNO)­6, (BSO)­7/(SNO)­7, and (BSO)­8/(SNO)­8.…”
Section: Methodssupporting
confidence: 84%
“…8(a). This procedure is well-known to explain the source of the displacive phase transitions as in the case of ferroelectric perovskite oxide BaTiO 3 , 67 the strain-induced multiferroic state in the NaMnF 3 fluoride, 68,69 and the polar response in the Sr(Nb,Ta)O 2 N 70,71 oxynitrides. Fig.…”
Section: Resultsmentioning
confidence: 99%
“…Multiferroics have been intensively studied since the discovery of room-temperature multiferroic BiFeO 3 ( 53 ) and type II multiferroic TbMnO 3 ( 54 ). Nowadays, electric-field control of magnetism has become a key to realize ultralow-power logic memory devices in recently developed device architectures ( 55 , 56 ). One priority for the scientific community is to broaden the set of materials that exhibit multiferroic and ME behavior at room temperature.…”
Section: Discussionmentioning
confidence: 99%