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Evidence of a Large Refrigerant Capacity in Nb-Modified La 1.4 Sr 1.6 Mn 2−x Nb x O 7 (0.0 ≤ x ≤ 0.15) Layered Perovskites.

Authors :
Kumar, Akshay
Kim, Jong Woo
Sharma, Mohit K.
Kumari, Kavita
Vij, Ankush
Koo, Bon Heun
Source :
Magnetochemistry; Apr2024, Vol. 10 Issue 4, p22, 13p
Publication Year :
2024

Abstract

In this work, evidence of isothermal magnetic entropy change ( ∆ S M ) over a broad temperature region is presented in a series of La<subscript>1.4</subscript>Sr<subscript>1.6</subscript>Mn<subscript>2−x</subscript>Nb<subscript>x</subscript>O<subscript>7</subscript> Ruddlesden–Popper compounds with niobium modification (Nb) (0.0 ≤ x ≤ 0.15) at the manganese (Mn) site. The ceramic samples were obtained through a solid-state sintering method in optimized conditions. All compounds predominantly possessed Ruddlesden–Popper phase while a few additional reflections were resolved in Nb-doped compounds which indicates the separation of structural phases. These peaks are assigned to a separate layered perovskite and single perovskite with tetragonal symmetry and hexagonal symmetry, respectively. The microstructure of the pure sample reveals uniform grain morphology but in Nb-doped specimens chiefly three types of grains were found. It was assumed that the inter-connected large particles were of R-P phase which is dominant in both parent and x = 0.05 compounds, while the hexagonal and polygonal morphology of grains in higher concentrations of dopants directly corroborates with the symmetry of single perovskite and additional layered perovskite phases, respectively. The parent compound exhibits a single ∆ S M curve, whereas all Nb-substituted samples display bifurcated ∆ S M curves. This indicated two transition regions with multiple magnetic components, attributed to distinct structural phases. The highest ∆ S M values obtained for components corresponding to the R-P phase are 2.32 Jkg<superscript>−1</superscript>k<superscript>−1</superscript>, 0.75 Jkg<superscript>−1</superscript>k<superscript>−1</superscript>, 0.58 Jkg<superscript>−1</superscript>k<superscript>−1</superscript> and 0.43 Jkg<superscript>−1</superscript>k<superscript>−1</superscript> and for the second component located around room temperature are 0.0 Jkg<superscript>−1</superscript>k<superscript>−1</superscript>, 0.2 Jkg<superscript>−1</superscript>k<superscript>−1</superscript>, 0.28 Jkg<superscript>−1</superscript>k<superscript>−1</superscript> and 0.35 Jkg<superscript>−1</superscript>k<superscript>−1</superscript> for x = 0.0, 0.05, 0.10 and 0.15 compositions, respectively, at 2.5 T. Due to the collective participation of both components the ∆ S M was expanded through a broad temperature range upon Nb doping. [ABSTRACT FROM AUTHOR]

Details

Language :
English
ISSN :
23127481
Volume :
10
Issue :
4
Database :
Complementary Index
Journal :
Magnetochemistry
Publication Type :
Academic Journal
Accession number :
176875793
Full Text :
https://doi.org/10.3390/magnetochemistry10040022