Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample
We have investigated the structural and magnetization properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample, synthesized using the sol–gel method. The Rietveld refinement of the X-ray diffraction pattern of the nanocrystalline sample (recorded at room temperature) confirmed the formation of t...
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doaj-effb98e4d5214ebd9b24805454ac1f602021-02-02T21:32:45ZengAIP Publishing LLCAIP Advances2158-32262021-01-01111015239015239-510.1063/9.0000088Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sampleMeenak shi0Priyanka Bisht1Amit Kumar2Rabindra Nath Mahato3School of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, IndiaSchool of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, IndiaSchool of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, IndiaSchool of Physical Sciences, Jawaharlal Nehru University, New Delhi 110067, IndiaWe have investigated the structural and magnetization properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample, synthesized using the sol–gel method. The Rietveld refinement of the X-ray diffraction pattern of the nanocrystalline sample (recorded at room temperature) confirmed the formation of the orthorhombic crystal structure with Pnma space group. The temperature dependent magnetization M(T) measurements suggested that the present sample undergoes a paramagnetic to ferromagnetic phase transition and the Curie temperature was found to be ∼ 126 K. The positive slopes observed from the Arrott plots for the present sample indicate the second order of magnetic phase transition, as per the Banerjee’s criterion. The maximum value of magnetic entropy change |ΔSMmax| and relative cooling power (RCP) were found to be ∼ 2.2 J kg-1K-1 and 261 Jkg-1 for a magnetic field change of 5 T. The phenomenological universal curve was constructed for the present sample and ΔSM curves were found to collapse into one, and the universal curve confirmed the second order of magnetic phase transition. The relatively large values of |ΔSM| and RCP make the present nanocrystalline compound promising for the magnetic refrigeration technology.http://dx.doi.org/10.1063/9.0000088 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Meenak shi Priyanka Bisht Amit Kumar Rabindra Nath Mahato |
spellingShingle |
Meenak shi Priyanka Bisht Amit Kumar Rabindra Nath Mahato Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample AIP Advances |
author_facet |
Meenak shi Priyanka Bisht Amit Kumar Rabindra Nath Mahato |
author_sort |
Meenak shi |
title |
Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample |
title_short |
Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample |
title_full |
Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample |
title_fullStr |
Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample |
title_full_unstemmed |
Magnetic and magnetocaloric properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample |
title_sort |
magnetic and magnetocaloric properties of the nanocrystalline pr0.7ba0.2ca0.1mno3 sample |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2021-01-01 |
description |
We have investigated the structural and magnetization properties of the nanocrystalline Pr0.7Ba0.2Ca0.1MnO3 sample, synthesized using the sol–gel method. The Rietveld refinement of the X-ray diffraction pattern of the nanocrystalline sample (recorded at room temperature) confirmed the formation of the orthorhombic crystal structure with Pnma space group. The temperature dependent magnetization M(T) measurements suggested that the present sample undergoes a paramagnetic to ferromagnetic phase transition and the Curie temperature was found to be ∼ 126 K. The positive slopes observed from the Arrott plots for the present sample indicate the second order of magnetic phase transition, as per the Banerjee’s criterion. The maximum value of magnetic entropy change |ΔSMmax| and relative cooling power (RCP) were found to be ∼ 2.2 J kg-1K-1 and 261 Jkg-1 for a magnetic field change of 5 T. The phenomenological universal curve was constructed for the present sample and ΔSM curves were found to collapse into one, and the universal curve confirmed the second order of magnetic phase transition. The relatively large values of |ΔSM| and RCP make the present nanocrystalline compound promising for the magnetic refrigeration technology. |
url |
http://dx.doi.org/10.1063/9.0000088 |
work_keys_str_mv |
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