High‐temperature dielectric properties and impedance spectroscopy of PbHf1−x Snx O3 ceramics

PbHf1−x Snx O3 (PSH) ceramics were synthesised by a conventional solid‐state reaction method. Dielectric properties were investigated in the temperature range of 20–650°C. As the Sn4+ content goes up, the phase transition temperatures of an antiferroelectric (AFE1) to another intermediate antiferroe...

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Published inIET Nanodielectrics Vol. 3; no. 4; pp. 131 - 137
Main Authors Liu, Zhi‐Gang, Ge, Peng‐Zu, Tang, Hui, Tang, Xin‐Gui, Zeng, Si‐Ming, Jiang, Yan‐Ping, Tang, Zhen‐Hua, Liu, Qiu‐Xiang
Format Journal Article
LanguageEnglish
Published Beijing The Institution of Engineering and Technology 01.12.2020
John Wiley & Sons, Inc
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Abstract PbHf1−x Snx O3 (PSH) ceramics were synthesised by a conventional solid‐state reaction method. Dielectric properties were investigated in the temperature range of 20–650°C. As the Sn4+ content goes up, the phase transition temperatures of an antiferroelectric (AFE1) to another intermediate antiferroelectric (AFE2) phase and AFE2 to the paraelectric (PE) phase decrease gradually. When x ≥0.1 for PSH ceramics, the ferroelectric (FE) phase appears around 225°C, and phase transition temperature from FE phase to PE phase goes up with the increasing concentration of Sn4+. Moreover, high‐temperature dielectric relaxation (HTDR) phenomenon can be seen from all samples. Mechanism of HTDR was discussed from impedance spectroscopy and conductivity for PSH ceramics. It was found that three dielectric responses were observed in complex impedance plots and HTDR was involved with the movement of oxygen vacancies. Activation energy calculated from dielectric data suggested that the HTDR was governed by the hopping conduction process.
AbstractList PbHf1−x Snx O3 (PSH) ceramics were synthesised by a conventional solid‐state reaction method. Dielectric properties were investigated in the temperature range of 20–650°C. As the Sn4+ content goes up, the phase transition temperatures of an antiferroelectric (AFE1) to another intermediate antiferroelectric (AFE2) phase and AFE2 to the paraelectric (PE) phase decrease gradually. When x ≥0.1 for PSH ceramics, the ferroelectric (FE) phase appears around 225°C, and phase transition temperature from FE phase to PE phase goes up with the increasing concentration of Sn4+. Moreover, high‐temperature dielectric relaxation (HTDR) phenomenon can be seen from all samples. Mechanism of HTDR was discussed from impedance spectroscopy and conductivity for PSH ceramics. It was found that three dielectric responses were observed in complex impedance plots and HTDR was involved with the movement of oxygen vacancies. Activation energy calculated from dielectric data suggested that the HTDR was governed by the hopping conduction process.
Author Tang, Hui
Liu, Zhi‐Gang
Liu, Qiu‐Xiang
Tang, Xin‐Gui
Ge, Peng‐Zu
Jiang, Yan‐Ping
Tang, Zhen‐Hua
Zeng, Si‐Ming
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  fullname: Ge, Peng‐Zu
  organization: Guangzhou Higher Education Mega Centre
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  fullname: Tang, Hui
  organization: Guangzhou Higher Education Mega Centre
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  givenname: Xin‐Gui
  surname: Tang
  fullname: Tang, Xin‐Gui
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  surname: Liu
  fullname: Liu, Qiu‐Xiang
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Snippet PbHf1−x Snx O3 (PSH) ceramics were synthesised by a conventional solid‐state reaction method. Dielectric properties were investigated in the temperature range...
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StartPage 131
SubjectTerms activation energy
antiferroelectric materials
Antiferroelectricity
Ceramics
Chemical synthesis
complex impedance plots
Conduction heating
conventional solid‐state reaction method
Dielectric properties
Dielectric relaxation
FE phase
ferroelectric ceramics
ferroelectric phase
ferroelectric transitions
high‐temperature dielectric relaxation
Hopping conduction
Impedance spectroscopy
intermediate antiferroelectric phase
lead compounds
oxygen vacancies
paraelectric phase
PbHf1‐x Snx O3
PE phase
phase transition temperature
Phase transitions
PSH ceramics
Single crystals
Spectrum analysis
Temperature
temperature 20.0 degC to 650.0 degC
Transition temperature
vacancies (crystal)
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Title High‐temperature dielectric properties and impedance spectroscopy of PbHf1−x Snx O3 ceramics
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