Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics

Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) ceramics were prepared by using conventional solid-state route. The microwave dielectric properties of the samples were investigated as a function of measured frequency and the Ca content. A pure perovskite structure was obtained for samples with -0.02 ≤ x ≤ 0.02,...

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Main Authors: M. J. Abu, M. F. Ab. Rahman, R.A. Zaman, M. Ahmadipour, J. J. Mohamed, M. F. ain, Z. A. Ahmad
Format: Book Section
Published: Elsevier 2016
Online Access:http://discol.umk.edu.my/id/eprint/8613/
http://www.sciencedirect.com/science/article/pii/S1876619616001832
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spelling my.umk.eprints.86132022-05-23T10:38:27Z http://discol.umk.edu.my/id/eprint/8613/ Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics M. J. Abu M. F. Ab. Rahman R.A. Zaman M. Ahmadipour J. J. Mohamed M. F. ain Z. A. Ahmad Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) ceramics were prepared by using conventional solid-state route. The microwave dielectric properties of the samples were investigated as a function of measured frequency and the Ca content. A pure perovskite structure was obtained for samples with -0.02 ≤ x ≤ 0.02, whereas small amount of CuO and CaTiO3 appeared in the samples with x = -0.04 and 0.04, respectively, indicated that the solubility limit of Ca atom in CCTO lattice was reached for this system. Adjusting of Ca content showed a little influence on the microstructure of the ceramics. The sample with x = 0 exhibited good microwave dielectric permittivity (ɛ’ ∼ 85), which nearly constant at a broad frequency range of 1 – 35 GHz, then abruptly dropped to ∼70 at 50 GHz. The other samples showed a strongly frequency dependence of dielectric permittivity from ∼100 (at 1 GHz) to ∼10 (at 50 GHz). The dielectric loss (tan-δ) for nonstoichiometry CCTO samples is relatively higher at least an order of magnitude and displays strong frequency dependence as compared with the x = 0 sample. The existence of vacancy (oxygen and Ca) and Ca/Cu disorder are the main factor affecting ɛ’ and tan-δ values of the ceramics. Elsevier 2016 Book Section NonPeerReviewed M. J. Abu and M. F. Ab. Rahman and R.A. Zaman and M. Ahmadipour and J. J. Mohamed and M. F. ain and Z. A. Ahmad (2016) Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics. In: 5th International Conference on Recent Advances in Materials, Minerals and Environment (RAMM) & 2nd International Postgraduate Conference on Materials, Mineral and Polymer (MAMIP). Elsevier, pp. 929-934. http://www.sciencedirect.com/science/article/pii/S1876619616001832
institution Universiti Malaysia Kelantan
building Perpustakaan Universiti Malaysia Kelantan
collection Institutional Repository
continent Asia
country Malaysia
content_provider Universiti Malaysia Kelantan
content_source UMK Institutional Repository
url_provider http://umkeprints.umk.edu.my/
description Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) ceramics were prepared by using conventional solid-state route. The microwave dielectric properties of the samples were investigated as a function of measured frequency and the Ca content. A pure perovskite structure was obtained for samples with -0.02 ≤ x ≤ 0.02, whereas small amount of CuO and CaTiO3 appeared in the samples with x = -0.04 and 0.04, respectively, indicated that the solubility limit of Ca atom in CCTO lattice was reached for this system. Adjusting of Ca content showed a little influence on the microstructure of the ceramics. The sample with x = 0 exhibited good microwave dielectric permittivity (ɛ’ ∼ 85), which nearly constant at a broad frequency range of 1 – 35 GHz, then abruptly dropped to ∼70 at 50 GHz. The other samples showed a strongly frequency dependence of dielectric permittivity from ∼100 (at 1 GHz) to ∼10 (at 50 GHz). The dielectric loss (tan-δ) for nonstoichiometry CCTO samples is relatively higher at least an order of magnitude and displays strong frequency dependence as compared with the x = 0 sample. The existence of vacancy (oxygen and Ca) and Ca/Cu disorder are the main factor affecting ɛ’ and tan-δ values of the ceramics.
format Book Section
author M. J. Abu
M. F. Ab. Rahman
R.A. Zaman
M. Ahmadipour
J. J. Mohamed
M. F. ain
Z. A. Ahmad
spellingShingle M. J. Abu
M. F. Ab. Rahman
R.A. Zaman
M. Ahmadipour
J. J. Mohamed
M. F. ain
Z. A. Ahmad
Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
author_facet M. J. Abu
M. F. Ab. Rahman
R.A. Zaman
M. Ahmadipour
J. J. Mohamed
M. F. ain
Z. A. Ahmad
author_sort M. J. Abu
title Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
title_short Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
title_full Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
title_fullStr Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
title_full_unstemmed Microwave Dielectric Properties of Ca1+xCu3Ti4O12+x (-0.04 ≤ x ≤ 0.04) Ceramics
title_sort microwave dielectric properties of ca1+xcu3ti4o12+x (-0.04 ≤ x ≤ 0.04) ceramics
publisher Elsevier
publishDate 2016
url http://discol.umk.edu.my/id/eprint/8613/
http://www.sciencedirect.com/science/article/pii/S1876619616001832
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