Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics

Pb1-xLaxTi1-xMnxO3 (PLTM100x, x = 0.20, 0.40, 0.50, 0.60, and 0.80) ceramics have been prepared and investigated. X-ray diffractions show all ceramics are crystallized into perovskite structures with tetragonal symmetry for PLTMO20 and orthorhombic symmetry for the other compositions. X-ray photoele...

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Main Authors: Jie Xu, Jin-Feng Wang, Long Jiao, Weijing Ji, Jian Zhou, Zheng-Bin Gu, Y. B. Chen, Shu-Hua Yao, Shan-Tao Zhang, Yan-Feng Chen
Format: Article
Language:English
Published: AIP Publishing LLC 2012-09-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4749254
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author Jie Xu
Jin-Feng Wang
Long Jiao
Weijing Ji
Jian Zhou
Zheng-Bin Gu
Y. B. Chen
Shu-Hua Yao
Shan-Tao Zhang
Yan-Feng Chen
author_facet Jie Xu
Jin-Feng Wang
Long Jiao
Weijing Ji
Jian Zhou
Zheng-Bin Gu
Y. B. Chen
Shu-Hua Yao
Shan-Tao Zhang
Yan-Feng Chen
author_sort Jie Xu
collection DOAJ
description Pb1-xLaxTi1-xMnxO3 (PLTM100x, x = 0.20, 0.40, 0.50, 0.60, and 0.80) ceramics have been prepared and investigated. X-ray diffractions show all ceramics are crystallized into perovskite structures with tetragonal symmetry for PLTMO20 and orthorhombic symmetry for the other compositions. X-ray photoelectron spectroscopy results confirm that the Mn cations in PLTMO20 and PLTMO40 have the valence state of +3, whereas in other compositions, the Mn cations have mixed valences states of +3 and +4. With increasing x from 0.20 to 0.80, the materials change from superparamagnetic to coexisting ferromagnetic and antiferromagnetic magnetic behaviour whereas all compositions persist insulating behaviour, as confirmed by the magnetization-magnetic field (M-H), the temperature dependent magnetization (M-T) and transport measurements. Especially, the PLTMO80 has a large negative magnetoresistance of −41.5% at 10 K with the applied filed of 2 T. By considering the chemical states of Mn cations, these results are attributed to that the coexistence of metallic ferromagnetic and insulating non-ferromagnetic phases.
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spelling doaj.art-01a33e81208a415887126cd04afd37be2022-12-22T03:16:26ZengAIP Publishing LLCAIP Advances2158-32262012-09-0123032156032156-1010.1063/1.4749254056203ADVMagnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramicsJie Xu0Jin-Feng Wang1Long Jiao2Weijing Ji3Jian Zhou4Zheng-Bin Gu5Y. B. Chen6Shu-Hua Yao7Shan-Tao Zhang8Yan-Feng Chen9National Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Physics, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaNational Laboratory of Solid State Microstructure and Department of Materials Science and Engineering, Nanjing University, Nanjing 210093, ChinaPb1-xLaxTi1-xMnxO3 (PLTM100x, x = 0.20, 0.40, 0.50, 0.60, and 0.80) ceramics have been prepared and investigated. X-ray diffractions show all ceramics are crystallized into perovskite structures with tetragonal symmetry for PLTMO20 and orthorhombic symmetry for the other compositions. X-ray photoelectron spectroscopy results confirm that the Mn cations in PLTMO20 and PLTMO40 have the valence state of +3, whereas in other compositions, the Mn cations have mixed valences states of +3 and +4. With increasing x from 0.20 to 0.80, the materials change from superparamagnetic to coexisting ferromagnetic and antiferromagnetic magnetic behaviour whereas all compositions persist insulating behaviour, as confirmed by the magnetization-magnetic field (M-H), the temperature dependent magnetization (M-T) and transport measurements. Especially, the PLTMO80 has a large negative magnetoresistance of −41.5% at 10 K with the applied filed of 2 T. By considering the chemical states of Mn cations, these results are attributed to that the coexistence of metallic ferromagnetic and insulating non-ferromagnetic phases.http://dx.doi.org/10.1063/1.4749254
spellingShingle Jie Xu
Jin-Feng Wang
Long Jiao
Weijing Ji
Jian Zhou
Zheng-Bin Gu
Y. B. Chen
Shu-Hua Yao
Shan-Tao Zhang
Yan-Feng Chen
Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
AIP Advances
title Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
title_full Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
title_fullStr Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
title_full_unstemmed Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
title_short Magnetic and electrical transport properties of Pb1-xLaxTi1-xMnxO3 ceramics
title_sort magnetic and electrical transport properties of pb1 xlaxti1 xmnxo3 ceramics
url http://dx.doi.org/10.1063/1.4749254
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