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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Main Authors: U. Chaudhuri, R. Mahendiran
Format: Article
Language:English
Published: AIP Publishing LLC 2021-01-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/9.0000107
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spelling 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
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