High-pressure structural change in the ferroelectric layered perovskite Sr2Nb2O7

The structural changes of sintered powder samples of perovskite-slab layered polycrystalline Sr2Nb2O7 (SNO) ferroelectric compound subjected to high pressures are here investigated. The samples were prepared using a solid-state reaction in the presence (SNOE) or absence (SNO) of an applied electric...

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Veröffentlicht in:Physical review. B 2019-08, Vol.100 (5), p.1
Hauptverfasser: Alanis, Javier, Ojeda-Galván, Hiram Joazet, Rodríguez-Aranda, M C, Rodríguez, A G, García, Harumi Moreno, Íñiguez, Jorge, Mendoza, María Eugenia, Navarro-Contreras, Hugo R
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container_issue 5
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container_title Physical review. B
container_volume 100
creator Alanis, Javier
Ojeda-Galván, Hiram Joazet
Rodríguez-Aranda, M C
Rodríguez, A G
García, Harumi Moreno
Íñiguez, Jorge
Mendoza, María Eugenia
Navarro-Contreras, Hugo R
description The structural changes of sintered powder samples of perovskite-slab layered polycrystalline Sr2Nb2O7 (SNO) ferroelectric compound subjected to high pressures are here investigated. The samples were prepared using a solid-state reaction in the presence (SNOE) or absence (SNO) of an applied electric field. Density functional theory (DFT) calculations including hydrostatic pressure indicate that SNO's ferroelectricity remains up to 25 GPa in the structure of space group Cmc21 derived from the condensation of one zone-center soft phonon. The predicted DFT theoretical structural changes are discussed and compared with the results of the experimental Raman spectra as a function of pressure. The pressure-dependent spectra were recorded from atmospheric pressure up to 11.5 and 13.5 GPa for SNOE and SNO, respectively. Both samples underwent a pressure induced phase transition from an incommensurate to a commensurate state at room temperature, SNO at Pi−c=6.5±0.2 GPa, and SNOE at Pi−c=6.9±0.3 GPa. The DFT calculations enable the identification of the change in phase to the orthorhombic structure with the space group Cmc21. The experimental values for Pi−c are in reasonably good agreement with the theoretical predicted value of ∼7.3 GPa. After the critical pressures, the number of observable phonons decreases, that is, when the compound adopts a higher symmetry structure, several phonons vanish abruptly in both the SNO and SNOE samples, as expected. The Raman spectra for both samples show hysteresis effects, that is, after the pressure is removed, a few extra lines remain visible, as well as many relative intensity changes and broadenings for some phonon bands. The bulk moduli of the Sr2Nb2O7 before and after Pi−c are calculated resulting in 117.0 and 147.8 GPa, respectively. The Grüneisen parameters of the phonons observed are finally calculated and discussed.
doi_str_mv 10.1103/PhysRevB.100.054110
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The samples were prepared using a solid-state reaction in the presence (SNOE) or absence (SNO) of an applied electric field. Density functional theory (DFT) calculations including hydrostatic pressure indicate that SNO's ferroelectricity remains up to 25 GPa in the structure of space group Cmc21 derived from the condensation of one zone-center soft phonon. The predicted DFT theoretical structural changes are discussed and compared with the results of the experimental Raman spectra as a function of pressure. The pressure-dependent spectra were recorded from atmospheric pressure up to 11.5 and 13.5 GPa for SNOE and SNO, respectively. Both samples underwent a pressure induced phase transition from an incommensurate to a commensurate state at room temperature, SNO at Pi−c=6.5±0.2 GPa, and SNOE at Pi−c=6.9±0.3 GPa. The DFT calculations enable the identification of the change in phase to the orthorhombic structure with the space group Cmc21. The experimental values for Pi−c are in reasonably good agreement with the theoretical predicted value of ∼7.3 GPa. After the critical pressures, the number of observable phonons decreases, that is, when the compound adopts a higher symmetry structure, several phonons vanish abruptly in both the SNO and SNOE samples, as expected. The Raman spectra for both samples show hysteresis effects, that is, after the pressure is removed, a few extra lines remain visible, as well as many relative intensity changes and broadenings for some phonon bands. The bulk moduli of the Sr2Nb2O7 before and after Pi−c are calculated resulting in 117.0 and 147.8 GPa, respectively. 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B</title><description>The structural changes of sintered powder samples of perovskite-slab layered polycrystalline Sr2Nb2O7 (SNO) ferroelectric compound subjected to high pressures are here investigated. The samples were prepared using a solid-state reaction in the presence (SNOE) or absence (SNO) of an applied electric field. Density functional theory (DFT) calculations including hydrostatic pressure indicate that SNO's ferroelectricity remains up to 25 GPa in the structure of space group Cmc21 derived from the condensation of one zone-center soft phonon. The predicted DFT theoretical structural changes are discussed and compared with the results of the experimental Raman spectra as a function of pressure. The pressure-dependent spectra were recorded from atmospheric pressure up to 11.5 and 13.5 GPa for SNOE and SNO, respectively. 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subjects Density functional theory
Electric fields
Ferroelectric materials
Ferroelectricity
Gruneisen parameter
Hydrostatic pressure
Mathematical analysis
Perovskites
Phase transitions
Phonons
Pressure dependence
Raman spectra
Sintering (powder metallurgy)
title High-pressure structural change in the ferroelectric layered perovskite Sr2Nb2O7
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