Ferroelectricity of stress-free and strained pure SrTi O3 revealed by ab initio calculations with hybrid and density functionals

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Abstract

The properties of stress-free and biaxially strained stoichiometric SrTiO3 in the absence and presence of antiferrodistortive (AFD) distortion were calculated ab initio. To obtain reliable results, multiple exchange correlation (XC) functionals, including the Heyd-Scuseria-Ernzerhof (HSE) hybrid functional, were used. HSE was the primary XC functional, while another functional provided a good lower bound of ferroelectricity (FE). The reliability of the calculations was further reinforced by the calculations of the strain and AFD dependence. In contrast with previous works, we show that the ferroelectric phase (C4v1, C4v10) is more stable in the absence of quantum and thermal fluctuations than the paraelectric phase (Oh1, D4h18), even for the stress-free case, and clarify the properties of these FE phases. The energy gain of stress-free FE, in comparison with the thermal and quantum fluctuation energy, indicates that a paraelectric phase emerges at room temperature by thermal fluctuations, but is near 0 K marginally close to the FE phase, which aligns with the experimental incipient FE. This implies that the paraelectricity of stress-free SrTiO3 in experiments contains incoherent atomic-scale FE regions. These results are consistent with the FE microregions (FMR), signatures of polar disorders, and the emergence of FE in SrTiO3 due to impurities and defects. The value of spontaneous polarization PS could reach 10μC/cm2 in the absence of fluctuations, even for the stress-free case. In view of the earlier theory of the carrier layer at polar discontinuities, the present results may explain the conduction at the interfaces of the LaAlO3/SrTiO3. In addition, an "enhancement of FE due to symmetry constriction" is proposed as an additional mechanism to the strain-enhanced FE in the epitaxial effect. For large compressive strain, e.g., 2%, the Perdew-Burke-Ernzerhof density functional for solids (PBEsol) yielded properties with PS>20μC/cm2, agreeing with HSE, and therefore is usable as a practical substitute of HSE for SrTiO3.

Original languageEnglish
Article number064107
JournalPhysical Review B
Volume99
Issue number6
DOIs
Publication statusPublished - Feb 19 2019

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Ferroelectricity
ferroelectricity
functionals
Ferroelectric materials
constrictions
discontinuity
signatures
strontium titanium oxide
disorders
Impurities
substitutes
Polarization
conduction

All Science Journal Classification (ASJC) codes

  • Electronic, Optical and Magnetic Materials
  • Condensed Matter Physics

Cite this

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title = "Ferroelectricity of stress-free and strained pure SrTi O3 revealed by ab initio calculations with hybrid and density functionals",
abstract = "The properties of stress-free and biaxially strained stoichiometric SrTiO3 in the absence and presence of antiferrodistortive (AFD) distortion were calculated ab initio. To obtain reliable results, multiple exchange correlation (XC) functionals, including the Heyd-Scuseria-Ernzerhof (HSE) hybrid functional, were used. HSE was the primary XC functional, while another functional provided a good lower bound of ferroelectricity (FE). The reliability of the calculations was further reinforced by the calculations of the strain and AFD dependence. In contrast with previous works, we show that the ferroelectric phase (C4v1, C4v10) is more stable in the absence of quantum and thermal fluctuations than the paraelectric phase (Oh1, D4h18), even for the stress-free case, and clarify the properties of these FE phases. The energy gain of stress-free FE, in comparison with the thermal and quantum fluctuation energy, indicates that a paraelectric phase emerges at room temperature by thermal fluctuations, but is near 0 K marginally close to the FE phase, which aligns with the experimental incipient FE. This implies that the paraelectricity of stress-free SrTiO3 in experiments contains incoherent atomic-scale FE regions. These results are consistent with the FE microregions (FMR), signatures of polar disorders, and the emergence of FE in SrTiO3 due to impurities and defects. The value of spontaneous polarization PS could reach 10μC/cm2 in the absence of fluctuations, even for the stress-free case. In view of the earlier theory of the carrier layer at polar discontinuities, the present results may explain the conduction at the interfaces of the LaAlO3/SrTiO3. In addition, an {"}enhancement of FE due to symmetry constriction{"} is proposed as an additional mechanism to the strain-enhanced FE in the epitaxial effect. For large compressive strain, e.g., 2{\%}, the Perdew-Burke-Ernzerhof density functional for solids (PBEsol) yielded properties with PS>20μC/cm2, agreeing with HSE, and therefore is usable as a practical substitute of HSE for SrTiO3.",
author = "Yukio Watanabe",
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AU - Watanabe, Yukio

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N2 - The properties of stress-free and biaxially strained stoichiometric SrTiO3 in the absence and presence of antiferrodistortive (AFD) distortion were calculated ab initio. To obtain reliable results, multiple exchange correlation (XC) functionals, including the Heyd-Scuseria-Ernzerhof (HSE) hybrid functional, were used. HSE was the primary XC functional, while another functional provided a good lower bound of ferroelectricity (FE). The reliability of the calculations was further reinforced by the calculations of the strain and AFD dependence. In contrast with previous works, we show that the ferroelectric phase (C4v1, C4v10) is more stable in the absence of quantum and thermal fluctuations than the paraelectric phase (Oh1, D4h18), even for the stress-free case, and clarify the properties of these FE phases. The energy gain of stress-free FE, in comparison with the thermal and quantum fluctuation energy, indicates that a paraelectric phase emerges at room temperature by thermal fluctuations, but is near 0 K marginally close to the FE phase, which aligns with the experimental incipient FE. This implies that the paraelectricity of stress-free SrTiO3 in experiments contains incoherent atomic-scale FE regions. These results are consistent with the FE microregions (FMR), signatures of polar disorders, and the emergence of FE in SrTiO3 due to impurities and defects. The value of spontaneous polarization PS could reach 10μC/cm2 in the absence of fluctuations, even for the stress-free case. In view of the earlier theory of the carrier layer at polar discontinuities, the present results may explain the conduction at the interfaces of the LaAlO3/SrTiO3. In addition, an "enhancement of FE due to symmetry constriction" is proposed as an additional mechanism to the strain-enhanced FE in the epitaxial effect. For large compressive strain, e.g., 2%, the Perdew-Burke-Ernzerhof density functional for solids (PBEsol) yielded properties with PS>20μC/cm2, agreeing with HSE, and therefore is usable as a practical substitute of HSE for SrTiO3.

AB - The properties of stress-free and biaxially strained stoichiometric SrTiO3 in the absence and presence of antiferrodistortive (AFD) distortion were calculated ab initio. To obtain reliable results, multiple exchange correlation (XC) functionals, including the Heyd-Scuseria-Ernzerhof (HSE) hybrid functional, were used. HSE was the primary XC functional, while another functional provided a good lower bound of ferroelectricity (FE). The reliability of the calculations was further reinforced by the calculations of the strain and AFD dependence. In contrast with previous works, we show that the ferroelectric phase (C4v1, C4v10) is more stable in the absence of quantum and thermal fluctuations than the paraelectric phase (Oh1, D4h18), even for the stress-free case, and clarify the properties of these FE phases. The energy gain of stress-free FE, in comparison with the thermal and quantum fluctuation energy, indicates that a paraelectric phase emerges at room temperature by thermal fluctuations, but is near 0 K marginally close to the FE phase, which aligns with the experimental incipient FE. This implies that the paraelectricity of stress-free SrTiO3 in experiments contains incoherent atomic-scale FE regions. These results are consistent with the FE microregions (FMR), signatures of polar disorders, and the emergence of FE in SrTiO3 due to impurities and defects. The value of spontaneous polarization PS could reach 10μC/cm2 in the absence of fluctuations, even for the stress-free case. In view of the earlier theory of the carrier layer at polar discontinuities, the present results may explain the conduction at the interfaces of the LaAlO3/SrTiO3. In addition, an "enhancement of FE due to symmetry constriction" is proposed as an additional mechanism to the strain-enhanced FE in the epitaxial effect. For large compressive strain, e.g., 2%, the Perdew-Burke-Ernzerhof density functional for solids (PBEsol) yielded properties with PS>20μC/cm2, agreeing with HSE, and therefore is usable as a practical substitute of HSE for SrTiO3.

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