High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20)
We report the magnetization, magnetic field dependence of direct current magnetoresistance (dc MR) and alternating current magnetoresistance (ac MR) in La1-xSrxMnO3 (x = 0.12, 0.18, and 0.20) in the frequency range f= 30 MHz to 3000 MHz, at room temperature. The ac MR is negative in all three compos...
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doaj-a2c4324974be47a5ab87991d1bc428102021-02-02T21:32:46ZengAIP Publishing LLCAIP Advances2158-32262021-01-01111015345015345-410.1063/9.0000107High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20)U. Chaudhuri0R. Mahendiran1Physics Department, 2 Science Drive 3, National University of Singapore, Singapore 117551, Republic of SingaporePhysics Department, 2 Science Drive 3, National University of Singapore, Singapore 117551, Republic of SingaporeWe report the magnetization, magnetic field dependence of direct current magnetoresistance (dc MR) and alternating current magnetoresistance (ac MR) in La1-xSrxMnO3 (x = 0.12, 0.18, and 0.20) in the frequency range f= 30 MHz to 3000 MHz, at room temperature. The ac MR is negative in all three compositions and shows a dramatic increase in magnitude compared to the dc MR when f = 30 MHz and in a magnetic field H = ±3 kOe. With increasing frequency of current, the sign of ac MR at 3 kOe progressively changes from negative to positive in all these samples which is initiated by appearance of two peaks at H = ±Hr. Line shape analysis of the data indicate that Hr increases linearly with f in x = 0.12 and 0.18. We attribute the two peak behavior at high frequencies to electron paramagnetic resonance in x = 0.12 and 0.18 samples. From the analysis, we obtain the gyromagnetic ratio γ/2π = 2.428 MHz/Oe and 2.690 MHz/Oe for x = 0.18 and 0.12 respectively. The smaller value of γ/2π in x = 0.18 possibly reflects short-range correlations among Mn-spins in the paramagnetic state.http://dx.doi.org/10.1063/9.0000107 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
U. Chaudhuri R. Mahendiran |
spellingShingle |
U. Chaudhuri R. Mahendiran High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) AIP Advances |
author_facet |
U. Chaudhuri R. Mahendiran |
author_sort |
U. Chaudhuri |
title |
High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) |
title_short |
High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) |
title_full |
High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) |
title_fullStr |
High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) |
title_full_unstemmed |
High-frequency magnetotransport in La1-xSrxMnO3 (x = 0.12-0.20) |
title_sort |
high-frequency magnetotransport in la1-xsrxmno3 (x = 0.12-0.20) |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2021-01-01 |
description |
We report the magnetization, magnetic field dependence of direct current magnetoresistance (dc MR) and alternating current magnetoresistance (ac MR) in La1-xSrxMnO3 (x = 0.12, 0.18, and 0.20) in the frequency range f= 30 MHz to 3000 MHz, at room temperature. The ac MR is negative in all three compositions and shows a dramatic increase in magnitude compared to the dc MR when f = 30 MHz and in a magnetic field H = ±3 kOe. With increasing frequency of current, the sign of ac MR at 3 kOe progressively changes from negative to positive in all these samples which is initiated by appearance of two peaks at H = ±Hr. Line shape analysis of the data indicate that Hr increases linearly with f in x = 0.12 and 0.18. We attribute the two peak behavior at high frequencies to electron paramagnetic resonance in x = 0.12 and 0.18 samples. From the analysis, we obtain the gyromagnetic ratio γ/2π = 2.428 MHz/Oe and 2.690 MHz/Oe for x = 0.18 and 0.12 respectively. The smaller value of γ/2π in x = 0.18 possibly reflects short-range correlations among Mn-spins in the paramagnetic state. |
url |
http://dx.doi.org/10.1063/9.0000107 |
work_keys_str_mv |
AT uchaudhuri highfrequencymagnetotransportinla1xsrxmno3x012020 AT rmahendiran highfrequencymagnetotransportinla1xsrxmno3x012020 |
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1724291297546600448 |