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Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from Density Functional Calculations
[Image: see text] Giant magnetoelectric coupling is a very rare phenomenon that has gained much attention in the past few decades due to fundamental interest as well as practical applications. Here, we have successfully achieved giant magnetoelectric coupling in PbTi(1–x)V(x)O(3) (x = 0–1) using a s...
Autores principales: | , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2019
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6796892/ https://www.ncbi.nlm.nih.gov/pubmed/31646219 http://dx.doi.org/10.1021/acsomega.9b01176 |
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author | Patra, Lokanath Vidya, Ravindran Fjellvåg, Helmer Ravindran, Ponniah |
author_facet | Patra, Lokanath Vidya, Ravindran Fjellvåg, Helmer Ravindran, Ponniah |
author_sort | Patra, Lokanath |
collection | PubMed |
description | [Image: see text] Giant magnetoelectric coupling is a very rare phenomenon that has gained much attention in the past few decades due to fundamental interest as well as practical applications. Here, we have successfully achieved giant magnetoelectric coupling in PbTi(1–x)V(x)O(3) (x = 0–1) using a series of generalized gradient-corrected GGA (generalized gradient approximation), including on-site Coulomb repulsion (U)-corrected spin-polarized calculations based on accurate density functional theory. Our total energy calculations show that PbTi(1–x)V(x)O(3) stabilizes in C-type antiferromagnetic ground state for x > 0.123. With the substitution of V into PbTiO(3), the tetragonal distortion is highly enhanced accompanied by a linear increase in polarization. In addition, our band structure analysis shows that for lower x values, the tendency to form two-dimensional magnetism of PbTi(1–x)V(x)O(3) decreases. The orbital magnetic polarization was calculated with self-consistent field method by including orbital polarization correction in the calculation as well as from the computed X-ray magnetic dichroism spectra. A nonmagnetic metallic ground state is observed for the paraelectric phase for V concentration (x) = 1 competing with a volume change of 10% showing a large magnetovolume effect. Our orbital-projected density of states as well as orbital ordering analysis suggest that the orbital ordering plays a major role in the magnetic-to-nonmagnetic transition when going from ferroelectric to paraelectric phase. The calculated magnetic anisotropic energy shows that the direction [110] is the easy axis of magnetization for x = 1 composition. The partial polarization analysis shows that the Ti/V–O hybridization majorly contributes to the total electrical polarization. The present study adds a new series of compounds to the magnetoelectric family with rarely existing giant coupling between electric- and magnetic-order parameters. These results show that such kind of materials can be used for novel practical applications where one can change the magnetic properties drastically (magnetic to nonmagnetic, as shown here) with external electric field and vice versa. |
format | Online Article Text |
id | pubmed-6796892 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2019 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-67968922019-10-23 Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from Density Functional Calculations Patra, Lokanath Vidya, Ravindran Fjellvåg, Helmer Ravindran, Ponniah ACS Omega [Image: see text] Giant magnetoelectric coupling is a very rare phenomenon that has gained much attention in the past few decades due to fundamental interest as well as practical applications. Here, we have successfully achieved giant magnetoelectric coupling in PbTi(1–x)V(x)O(3) (x = 0–1) using a series of generalized gradient-corrected GGA (generalized gradient approximation), including on-site Coulomb repulsion (U)-corrected spin-polarized calculations based on accurate density functional theory. Our total energy calculations show that PbTi(1–x)V(x)O(3) stabilizes in C-type antiferromagnetic ground state for x > 0.123. With the substitution of V into PbTiO(3), the tetragonal distortion is highly enhanced accompanied by a linear increase in polarization. In addition, our band structure analysis shows that for lower x values, the tendency to form two-dimensional magnetism of PbTi(1–x)V(x)O(3) decreases. The orbital magnetic polarization was calculated with self-consistent field method by including orbital polarization correction in the calculation as well as from the computed X-ray magnetic dichroism spectra. A nonmagnetic metallic ground state is observed for the paraelectric phase for V concentration (x) = 1 competing with a volume change of 10% showing a large magnetovolume effect. Our orbital-projected density of states as well as orbital ordering analysis suggest that the orbital ordering plays a major role in the magnetic-to-nonmagnetic transition when going from ferroelectric to paraelectric phase. The calculated magnetic anisotropic energy shows that the direction [110] is the easy axis of magnetization for x = 1 composition. The partial polarization analysis shows that the Ti/V–O hybridization majorly contributes to the total electrical polarization. The present study adds a new series of compounds to the magnetoelectric family with rarely existing giant coupling between electric- and magnetic-order parameters. These results show that such kind of materials can be used for novel practical applications where one can change the magnetic properties drastically (magnetic to nonmagnetic, as shown here) with external electric field and vice versa. American Chemical Society 2019-09-30 /pmc/articles/PMC6796892/ /pubmed/31646219 http://dx.doi.org/10.1021/acsomega.9b01176 Text en Copyright © 2019 American Chemical Society This is an open access article published under an ACS AuthorChoice License (http://pubs.acs.org/page/policy/authorchoice_termsofuse.html) , which permits copying and redistribution of the article or any adaptations for non-commercial purposes. |
spellingShingle | Patra, Lokanath Vidya, Ravindran Fjellvåg, Helmer Ravindran, Ponniah Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from Density Functional Calculations |
title | Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from
Density Functional Calculations |
title_full | Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from
Density Functional Calculations |
title_fullStr | Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from
Density Functional Calculations |
title_full_unstemmed | Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from
Density Functional Calculations |
title_short | Giant Magnetoelectric Coupling in Multiferroic PbTi(1–x)V(x)O(3) from
Density Functional Calculations |
title_sort | giant magnetoelectric coupling in multiferroic pbti(1–x)v(x)o(3) from
density functional calculations |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6796892/ https://www.ncbi.nlm.nih.gov/pubmed/31646219 http://dx.doi.org/10.1021/acsomega.9b01176 |
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