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Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)

The nature of the magnetic transition, critical scaling of magnetization, and magnetocaloric effect in Mn(1+x)Fe(4−x)Si(3) (x = 0 to 1) are studied in detail. Our measurements show no thermal hysteresis across the magnetic transition for the parent compound which is in contrast with the previous rep...

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Autores principales: Singh, Vikram, Bag, Pallab, Rawat, R., Nath, R.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7181668/
https://www.ncbi.nlm.nih.gov/pubmed/32332771
http://dx.doi.org/10.1038/s41598-020-63223-0
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author Singh, Vikram
Bag, Pallab
Rawat, R.
Nath, R.
author_facet Singh, Vikram
Bag, Pallab
Rawat, R.
Nath, R.
author_sort Singh, Vikram
collection PubMed
description The nature of the magnetic transition, critical scaling of magnetization, and magnetocaloric effect in Mn(1+x)Fe(4−x)Si(3) (x = 0 to 1) are studied in detail. Our measurements show no thermal hysteresis across the magnetic transition for the parent compound which is in contrast with the previous report and corroborate the second order nature of the transition. The magnetic transition could be tuned continuously from 328 K to 212 K with Mn substitution at the Fe site. The Mn substitution leads to a linear increase in the unit cell volume and a slight reduction in the effective moment. A detailed critical analysis of the magnetization data for x = 0.0 and 0.2 is performed in the critical regime using the modified Arrott plots, Kouvel-Fisher plot, universal curve scaling, and scaling analysis of magnetocaloric effect. The magnetization isotherms follow modified Arrott plots with critical exponent (β [Formula: see text] 0.308, γ [Formula: see text] 1.448, and δ [Formula: see text] 5.64) for the parent compound (x = 0.0) and (β [Formula: see text] 0.304, γ [Formula: see text] 1.445, and δ [Formula: see text] 5.64) for x = 0.2. The Kouvel-Fisher and universal scaling plots of the magnetization isotherms further confirm the reliability of our critical analysis and values of the exponents. These values of the critical exponents are found to be same for both the parent and doped samples which do not fall under any of the standard universality classes. The exchange interaction decays as J(r) ~ r(−3.41) following the renormalization group theory and the observed critical exponents correspond to lattice dimensionality d = 2, spin dimensionality n = 1, and the range of interaction σ = 1.41. This value of σ(<2) indicates long-range interaction between magnetic spins. A reasonable magnetocaloric effect ΔS(m) [Formula: see text] −6.67 J/Kg-K and −5.84 J/Kg-K for x = 0.0 and 0.2 compounds, respectively, with a huge relative cooling power (RCP ~ 700 J/Kg) for 9 T magnetic field change is observed. The universal scaling of magnetocaloric effect further mimics the second order character of the magnetic transition. The obtained critical exponents from the critical analysis of magnetocaloric effect agree with the values deduced from the magnetic isotherm analysis.
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spelling pubmed-71816682020-04-27 Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3) Singh, Vikram Bag, Pallab Rawat, R. Nath, R. Sci Rep Article The nature of the magnetic transition, critical scaling of magnetization, and magnetocaloric effect in Mn(1+x)Fe(4−x)Si(3) (x = 0 to 1) are studied in detail. Our measurements show no thermal hysteresis across the magnetic transition for the parent compound which is in contrast with the previous report and corroborate the second order nature of the transition. The magnetic transition could be tuned continuously from 328 K to 212 K with Mn substitution at the Fe site. The Mn substitution leads to a linear increase in the unit cell volume and a slight reduction in the effective moment. A detailed critical analysis of the magnetization data for x = 0.0 and 0.2 is performed in the critical regime using the modified Arrott plots, Kouvel-Fisher plot, universal curve scaling, and scaling analysis of magnetocaloric effect. The magnetization isotherms follow modified Arrott plots with critical exponent (β [Formula: see text] 0.308, γ [Formula: see text] 1.448, and δ [Formula: see text] 5.64) for the parent compound (x = 0.0) and (β [Formula: see text] 0.304, γ [Formula: see text] 1.445, and δ [Formula: see text] 5.64) for x = 0.2. The Kouvel-Fisher and universal scaling plots of the magnetization isotherms further confirm the reliability of our critical analysis and values of the exponents. These values of the critical exponents are found to be same for both the parent and doped samples which do not fall under any of the standard universality classes. The exchange interaction decays as J(r) ~ r(−3.41) following the renormalization group theory and the observed critical exponents correspond to lattice dimensionality d = 2, spin dimensionality n = 1, and the range of interaction σ = 1.41. This value of σ(<2) indicates long-range interaction between magnetic spins. A reasonable magnetocaloric effect ΔS(m) [Formula: see text] −6.67 J/Kg-K and −5.84 J/Kg-K for x = 0.0 and 0.2 compounds, respectively, with a huge relative cooling power (RCP ~ 700 J/Kg) for 9 T magnetic field change is observed. The universal scaling of magnetocaloric effect further mimics the second order character of the magnetic transition. The obtained critical exponents from the critical analysis of magnetocaloric effect agree with the values deduced from the magnetic isotherm analysis. Nature Publishing Group UK 2020-04-24 /pmc/articles/PMC7181668/ /pubmed/32332771 http://dx.doi.org/10.1038/s41598-020-63223-0 Text en © The Author(s) 2020 Open Access This article is licensed under a Creative Commons Attribution 4.0 International License, which permits use, sharing, adaptation, distribution and reproduction in any medium or format, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in a credit line to the material. If material is not included in the article’s Creative Commons license and your intended use is not permitted by statutory regulation or exceeds the permitted use, you will need to obtain permission directly from the copyright holder. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/.
spellingShingle Article
Singh, Vikram
Bag, Pallab
Rawat, R.
Nath, R.
Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title_full Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title_fullStr Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title_full_unstemmed Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title_short Critical behavior and magnetocaloric effect across the magnetic transition in Mn(1+x)Fe(4−x)Si(3)
title_sort critical behavior and magnetocaloric effect across the magnetic transition in mn(1+x)fe(4−x)si(3)
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7181668/
https://www.ncbi.nlm.nih.gov/pubmed/32332771
http://dx.doi.org/10.1038/s41598-020-63223-0
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