Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics

Ferroelectric varactors should have high tunability at low permittivity and a working electric field to obtain better impedance matching and stable tunability. In this work, (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2−x</sub>Ti<sub...

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Main Authors: Bo Wang, Le Zhao, Xiuhuai Jia, Pan Yang, Shihui Yu
Format: Article
Language:English
Published: MDPI AG 2023-07-01
Series:Materials
Subjects:
Online Access:https://www.mdpi.com/1996-1944/16/15/5226
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author Bo Wang
Le Zhao
Xiuhuai Jia
Pan Yang
Shihui Yu
author_facet Bo Wang
Le Zhao
Xiuhuai Jia
Pan Yang
Shihui Yu
author_sort Bo Wang
collection DOAJ
description Ferroelectric varactors should have high tunability at low permittivity and a working electric field to obtain better impedance matching and stable tunability. In this work, (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2−x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> (abbreviated as BCSZT100x, x = 0.05, 0.10, 0.15 and 0.20, respectively) are prepared to achieve high tunability at low permittivity and a working electric field. The tunable mechanisms are investigated based on crystal structure, micro-morphology and the permittivity-temperature spectrum. The results show that the shrink of oxygen octahedron and weaker interaction force between Sn<sup>4+</sup> and O<sup>2−</sup> make BCSZT5 ceramic have a higher tunability value of 26.55% at low permittivity (1913) and a working electric field (7.3 kV/cm). The tunability value of BCSZT5 ceramic increases by 58%, while its permittivity decreases by 25%, compared with x = 0. Those advantages make BCSZT5 ceramic have substantial application prospects in varactors.
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spelling doaj.art-e05de796153243468b6269f793d97a132023-11-18T23:10:29ZengMDPI AGMaterials1996-19442023-07-011615522610.3390/ma16155226Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> CeramicsBo Wang0Le Zhao1Xiuhuai Jia2Pan Yang3Shihui Yu4Department of Electrical Engineering and Automation, Luoyang Institute of Science and Technology, Luoyang 471023, ChinaSchool of Microelectronics, Tianjin University, Tianjin 300072, ChinaSchool of Microelectronics, Tianjin University, Tianjin 300072, ChinaDepartment of Electrical Engineering and Automation, Luoyang Institute of Science and Technology, Luoyang 471023, ChinaDepartment of Electrical Engineering and Automation, Luoyang Institute of Science and Technology, Luoyang 471023, ChinaFerroelectric varactors should have high tunability at low permittivity and a working electric field to obtain better impedance matching and stable tunability. In this work, (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2−x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> (abbreviated as BCSZT100x, x = 0.05, 0.10, 0.15 and 0.20, respectively) are prepared to achieve high tunability at low permittivity and a working electric field. The tunable mechanisms are investigated based on crystal structure, micro-morphology and the permittivity-temperature spectrum. The results show that the shrink of oxygen octahedron and weaker interaction force between Sn<sup>4+</sup> and O<sup>2−</sup> make BCSZT5 ceramic have a higher tunability value of 26.55% at low permittivity (1913) and a working electric field (7.3 kV/cm). The tunability value of BCSZT5 ceramic increases by 58%, while its permittivity decreases by 25%, compared with x = 0. Those advantages make BCSZT5 ceramic have substantial application prospects in varactors.https://www.mdpi.com/1996-1944/16/15/5226ferroelectric varactorspermittivityimpedance matchingoxygen octahedron
spellingShingle Bo Wang
Le Zhao
Xiuhuai Jia
Pan Yang
Shihui Yu
Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
Materials
ferroelectric varactors
permittivity
impedance matching
oxygen octahedron
title Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
title_full Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
title_fullStr Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
title_full_unstemmed Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
title_short Enhanced Tunability Achieving at Low Permittivity and Electric Field in (Ba<sub>0.91</sub>Ca<sub>0.09</sub>)(Sn<sub>x</sub>Zr<sub>0.2</sub><sub>−</sub><sub>x</sub>Ti<sub>0.8</sub>)O<sub>3</sub>-2 mol% CuO-1 mol% Li<sub>2</sub>CO<sub>3</sub> Ceramics
title_sort enhanced tunability achieving at low permittivity and electric field in ba sub 0 91 sub ca sub 0 09 sub sn sub x sub zr sub 0 2 sub sub sub sub x sub ti sub 0 8 sub o sub 3 sub 2 mol cuo 1 mol li sub 2 sub co sub 3 sub ceramics
topic ferroelectric varactors
permittivity
impedance matching
oxygen octahedron
url https://www.mdpi.com/1996-1944/16/15/5226
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