Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics

The dielectric properties of dense ceramics of (6H)-Ba(Ti 0.90Mn0.10)O3 are reported. Single-phase powders were obtained by the mixed oxide route at 1250 °C and ceramics (∼ 87% of the theoretical X-ray density) by sintering in air and flowing O2 at 1400 °C. The hexagonal phase was detected by angle...

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Main Authors: Phoosit N., Sinclair D.C., Phanichphant S.
Format: Conference or Workshop Item
Language:English
Published: 2014
Online Access:http://www.scopus.com/inward/record.url?eid=2-s2.0-34548120161&partnerID=40&md5=bb9a8d445f75785140d9b419ccab47f4
http://cmuir.cmu.ac.th/handle/6653943832/5208
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spelling th-cmuir.6653943832-52082014-08-30T02:56:16Z Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics Phoosit N. Sinclair D.C. Phanichphant S. The dielectric properties of dense ceramics of (6H)-Ba(Ti 0.90Mn0.10)O3 are reported. Single-phase powders were obtained by the mixed oxide route at 1250 °C and ceramics (∼ 87% of the theoretical X-ray density) by sintering in air and flowing O2 at 1400 °C. The hexagonal phase was detected by angle XRD analysis. The lattice parameter was calculated from the XRD data. The phase purity of the powders and ceramics was determined using the index scheme for undoped 6H- BaTiO3, reported in the ICDD file number 82-1175 as space group P63/mmc with lattice parameters of a = 5.72380(70) Å, c = 13.96490(70) Å, V = 396.2 Å3 and refinement data of XRD for BaTi0.90Mn0.10O3. After calcining at 1250 °C it had lattice parameters of a = 5.7235(6) Å, c = 13.9771(15) Å and V = 396.53 Å3, showing very little difference in lattice parameters from the reported values. BaTi0.90Mn 0.10O3 ceramics, after sintering at 1400 °C for 4 hours in air and flowing oxygen, showed lattice parameters of a = 5.7277(4) Å, c = 13.9750(17) Å, V = 396.73 Å3 and a = 5.7176(6) Å, c = 13.9607(5) Å, V = 395.25 Å3, respectively. SEM micrograph of the ceramics microstructure revealed the presence of open porosity with an average grain size between 1 and 3 μn. The conductivity through the grain and grain boundary was analyzed using impedance analysis. The impedance response of the ceramics showed single parallel RC elements with total resistance of 8.124X105 Ωcm at 384 °C, capacitance of ∼4.79 pFcm-1 and permittivity of ∼40-50, quality factor, Q × fr ∼ 13,000-19,000 GHz at ∼6.3GHz. The bulk resistivity and ceramics microstructure influence the loss in the microwave frequency range. © 2007 IEEE. 2014-08-30T02:56:16Z 2014-08-30T02:56:16Z 2007 Conference Paper 1424406102; 9781424406104 10.1109/NEMS.2007.352174 70130 http://www.scopus.com/inward/record.url?eid=2-s2.0-34548120161&partnerID=40&md5=bb9a8d445f75785140d9b419ccab47f4 http://cmuir.cmu.ac.th/handle/6653943832/5208 English
institution Chiang Mai University
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description The dielectric properties of dense ceramics of (6H)-Ba(Ti 0.90Mn0.10)O3 are reported. Single-phase powders were obtained by the mixed oxide route at 1250 °C and ceramics (∼ 87% of the theoretical X-ray density) by sintering in air and flowing O2 at 1400 °C. The hexagonal phase was detected by angle XRD analysis. The lattice parameter was calculated from the XRD data. The phase purity of the powders and ceramics was determined using the index scheme for undoped 6H- BaTiO3, reported in the ICDD file number 82-1175 as space group P63/mmc with lattice parameters of a = 5.72380(70) Å, c = 13.96490(70) Å, V = 396.2 Å3 and refinement data of XRD for BaTi0.90Mn0.10O3. After calcining at 1250 °C it had lattice parameters of a = 5.7235(6) Å, c = 13.9771(15) Å and V = 396.53 Å3, showing very little difference in lattice parameters from the reported values. BaTi0.90Mn 0.10O3 ceramics, after sintering at 1400 °C for 4 hours in air and flowing oxygen, showed lattice parameters of a = 5.7277(4) Å, c = 13.9750(17) Å, V = 396.73 Å3 and a = 5.7176(6) Å, c = 13.9607(5) Å, V = 395.25 Å3, respectively. SEM micrograph of the ceramics microstructure revealed the presence of open porosity with an average grain size between 1 and 3 μn. The conductivity through the grain and grain boundary was analyzed using impedance analysis. The impedance response of the ceramics showed single parallel RC elements with total resistance of 8.124X105 Ωcm at 384 °C, capacitance of ∼4.79 pFcm-1 and permittivity of ∼40-50, quality factor, Q × fr ∼ 13,000-19,000 GHz at ∼6.3GHz. The bulk resistivity and ceramics microstructure influence the loss in the microwave frequency range. © 2007 IEEE.
format Conference or Workshop Item
author Phoosit N.
Sinclair D.C.
Phanichphant S.
spellingShingle Phoosit N.
Sinclair D.C.
Phanichphant S.
Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
author_facet Phoosit N.
Sinclair D.C.
Phanichphant S.
author_sort Phoosit N.
title Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
title_short Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
title_full Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
title_fullStr Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
title_full_unstemmed Electrical conductivity of hexagonal Ba(Ti0.90Mn 0.10)O3 ceramics
title_sort electrical conductivity of hexagonal ba(ti0.90mn 0.10)o3 ceramics
publishDate 2014
url http://www.scopus.com/inward/record.url?eid=2-s2.0-34548120161&partnerID=40&md5=bb9a8d445f75785140d9b419ccab47f4
http://cmuir.cmu.ac.th/handle/6653943832/5208
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