Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications
The magnetic and transport properties of La2/3Ba 1/3(Mn1-xAlx)O3 (x50.0, 0.1, 0.2, 0.3 and 0.4) compounds, prepared by the solid state reaction, have been investigated. Samples show a metal-insulator transition excluding the sample x=0.0. With increased Al doping, the metal- insulator transition tem...
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2009
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2-s2.0-70149083068 Abdullah H.; Halim S.A.; Lim K.P.; Jannah A.N. Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications 2009 Materials Research Innovations 13 3 10.1179/143307509X441630 https://www.scopus.com/inward/record.uri?eid=2-s2.0-70149083068&doi=10.1179%2f143307509X441630&partnerID=40&md5=f52779fdd571e77f1d274dcda0bfb400 The magnetic and transport properties of La2/3Ba 1/3(Mn1-xAlx)O3 (x50.0, 0.1, 0.2, 0.3 and 0.4) compounds, prepared by the solid state reaction, have been investigated. Samples show a metal-insulator transition excluding the sample x=0.0. With increased Al doping, the metal- insulator transition temperature Tp is shifted to lower temperatures. Grain size reduction leads to a larger resistivity and a decrease in Tp. Upon analysing the data using several theoretical models, it was found that the metallic (ferromagnetic) part of the resistivity ρ (below Tp) fits well with the equation ρ=ρ0+ρ2T2, where ρ0 is due to the importance of grain/domain boundary effects, and a second term ρ2T2 might be attributed to the electron-electron scattering. The microstructure results indicate that the porosity of the samples increased when the concentration increased. The magnetoresistance (MR) is defined as %MR5100×[ρ(H, T)-ρ(0, T)]/ρ(0, T)], where ρ(H, T) and ρ(0, T) are the resistivities at temperature T, with an applied magnetic field H and zero applied magnetic field respectively. All samples show low-field magnetoresistance and high-field magnetoresistance regions. The highest percentage of LFMR at a temperature of 100 K is ∼210% MR/Tesla, measured for the sample x=0.2. For x=0.3, the sample reveals the highest colossal magnetoresistance value among other doped compounds with 27.27% at 100 K. © W. S. Maney & Son Ltd. 2009. 14328917 English Conference paper All Open Access; Green Open Access |
author |
Abdullah H.; Halim S.A.; Lim K.P.; Jannah A.N. |
spellingShingle |
Abdullah H.; Halim S.A.; Lim K.P.; Jannah A.N. Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
author_facet |
Abdullah H.; Halim S.A.; Lim K.P.; Jannah A.N. |
author_sort |
Abdullah H.; Halim S.A.; Lim K.P.; Jannah A.N. |
title |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
title_short |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
title_full |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
title_fullStr |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
title_full_unstemmed |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
title_sort |
Magneto-transport studies on La2/3Ba1/3(Mn 1-xAlx)O3 for low field sensing applications |
publishDate |
2009 |
container_title |
Materials Research Innovations |
container_volume |
13 |
container_issue |
3 |
doi_str_mv |
10.1179/143307509X441630 |
url |
https://www.scopus.com/inward/record.uri?eid=2-s2.0-70149083068&doi=10.1179%2f143307509X441630&partnerID=40&md5=f52779fdd571e77f1d274dcda0bfb400 |
description |
The magnetic and transport properties of La2/3Ba 1/3(Mn1-xAlx)O3 (x50.0, 0.1, 0.2, 0.3 and 0.4) compounds, prepared by the solid state reaction, have been investigated. Samples show a metal-insulator transition excluding the sample x=0.0. With increased Al doping, the metal- insulator transition temperature Tp is shifted to lower temperatures. Grain size reduction leads to a larger resistivity and a decrease in Tp. Upon analysing the data using several theoretical models, it was found that the metallic (ferromagnetic) part of the resistivity ρ (below Tp) fits well with the equation ρ=ρ0+ρ2T2, where ρ0 is due to the importance of grain/domain boundary effects, and a second term ρ2T2 might be attributed to the electron-electron scattering. The microstructure results indicate that the porosity of the samples increased when the concentration increased. The magnetoresistance (MR) is defined as %MR5100×[ρ(H, T)-ρ(0, T)]/ρ(0, T)], where ρ(H, T) and ρ(0, T) are the resistivities at temperature T, with an applied magnetic field H and zero applied magnetic field respectively. All samples show low-field magnetoresistance and high-field magnetoresistance regions. The highest percentage of LFMR at a temperature of 100 K is ∼210% MR/Tesla, measured for the sample x=0.2. For x=0.3, the sample reveals the highest colossal magnetoresistance value among other doped compounds with 27.27% at 100 K. © W. S. Maney & Son Ltd. 2009. |
publisher |
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issn |
14328917 |
language |
English |
format |
Conference paper |
accesstype |
All Open Access; Green Open Access |
record_format |
scopus |
collection |
Scopus |
_version_ |
1809677788821585920 |