Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3
The magnetocaloric effect in ferromagnetic single crystal EuTi0.85Nb0.15O3 has been investigated using magnetization and heat capacity measurements. EuTi0.85Nb0.15O3 undergoes a continuous ferromagnetic phase transition at TC = 9.5 K due to the long range ordering of magnetic moments of Eu2+ (4f7)....
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2016-02-01
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Online Access: | http://dx.doi.org/10.1063/1.4940960 |
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doaj-249c8e8b6b5345ebb20718ebfea61e9b2020-11-25T00:40:33ZengAIP Publishing LLCAPL Materials2166-532X2016-02-0142026102026102-710.1063/1.4940960002602APMGiant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3S. Roy0N. Khan1P. Mandal2 Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, India Saha Institute of Nuclear Physics, 1/AF Bidhannagar, Calcutta 700 064, IndiaThe magnetocaloric effect in ferromagnetic single crystal EuTi0.85Nb0.15O3 has been investigated using magnetization and heat capacity measurements. EuTi0.85Nb0.15O3 undergoes a continuous ferromagnetic phase transition at TC = 9.5 K due to the long range ordering of magnetic moments of Eu2+ (4f7). With the application of magnetic field, the spin entropy is strongly suppressed and a giant magnetic entropy change is observed near TC. The values of entropy change ΔSm and adiabatic temperature change ΔTad are as high as 51.3 J kg−1 K−1 and 22 K, respectively, for a field change of 0–9 T. The corresponding magnetic heating/cooling capacity is 700 J kg−1. This compound also shows large magnetocaloric effect even at low magnetic fields. In particular, the values of ΔSm reach 14.7 and 23.8 J kg−1 K−1 for field changes of 0–1 T and 0–2 T, respectively. The low-field giant magnetocaloric effect, together with the absence of thermal and field hysteresis makes EuTi0.85Nb0.15O3 a very promising candidate for low temperature magnetic refrigeration.http://dx.doi.org/10.1063/1.4940960 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
S. Roy N. Khan P. Mandal |
spellingShingle |
S. Roy N. Khan P. Mandal Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 APL Materials |
author_facet |
S. Roy N. Khan P. Mandal |
author_sort |
S. Roy |
title |
Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 |
title_short |
Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 |
title_full |
Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 |
title_fullStr |
Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 |
title_full_unstemmed |
Giant low-field magnetocaloric effect in single-crystalline EuTi0.85Nb0.15O3 |
title_sort |
giant low-field magnetocaloric effect in single-crystalline euti0.85nb0.15o3 |
publisher |
AIP Publishing LLC |
series |
APL Materials |
issn |
2166-532X |
publishDate |
2016-02-01 |
description |
The magnetocaloric effect in ferromagnetic single crystal EuTi0.85Nb0.15O3 has been investigated using magnetization and heat capacity measurements. EuTi0.85Nb0.15O3 undergoes a continuous ferromagnetic phase transition at TC = 9.5 K due to the long range ordering of magnetic moments of Eu2+ (4f7). With the application of magnetic field, the spin entropy is strongly suppressed and a giant magnetic entropy change is observed near TC. The values of entropy change ΔSm and adiabatic temperature change ΔTad are as high as 51.3 J kg−1 K−1 and 22 K, respectively, for a field change of 0–9 T. The corresponding magnetic heating/cooling capacity is 700 J kg−1. This compound also shows large magnetocaloric effect even at low magnetic fields. In particular, the values of ΔSm reach 14.7 and 23.8 J kg−1 K−1 for field changes of 0–1 T and 0–2 T, respectively. The low-field giant magnetocaloric effect, together with the absence of thermal and field hysteresis makes EuTi0.85Nb0.15O3 a very promising candidate for low temperature magnetic refrigeration. |
url |
http://dx.doi.org/10.1063/1.4940960 |
work_keys_str_mv |
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