Large low-field magnetic refrigeration in ferromagnetic insulator 
<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:msub><mml:mi mathvariant="bold">EuTi</mml:mi><mml:mrow><mml:mn>0.9</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="bold">V</mml:mi><mml:mrow><mml:mn>0.1</mml:mn></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="bold">O</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:mrow></mml:math>

Roy, Shubhankar; Das, Moumita; Mandal, P.

doi:10.1103/physrevmaterials.2.064412

Cited by 5 publications

(2 citation statements)

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“…A large number of studies revealed that B-site doping is a crucial mean to affect the magnetic properties of ETO. [10][11][12][13][14][15][16] The Nb-doped ETO presents the FM state and the value of maximal magnetic entropy (∆S max M ) reaches 14.7 J•kg −1 •K −1 for the single crystal EuTi 0.85 Nb 0.15 O 3 under a magnetic field in a range of 0 kOe-10 kOe. [13] Roy et al [14] discovered that EuTi 0.9 V 0.1 O 3 has a large ∆S max M of 20 J•kg −1 •K −1 when the magnetic field changes from 0 kOe to 20 kOe.…”

Section: Introductionmentioning

confidence: 99%

“…[10][11][12][13][14][15][16] The Nb-doped ETO presents the FM state and the value of maximal magnetic entropy (∆S max M ) reaches 14.7 J•kg −1 •K −1 for the single crystal EuTi 0.85 Nb 0.15 O 3 under a magnetic field in a range of 0 kOe-10 kOe. [13] Roy et al [14] discovered that EuTi 0.9 V 0.1 O 3 has a large ∆S max M of 20 J•kg −1 •K −1 when the magnetic field changes from 0 kOe to 20 kOe. The EuTi 1−x Al x O 3 compounds at 0.10 ≤ x ≤ 0.50 display the FM insulation behaviors.…”

Section: Introductionmentioning

confidence: 99%

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Improvement of the low-field-induced magnetocaloric effect in EuTiO₃ compounds*

Zeng¹,

Jiang²,

Yang³

et al. 2020

Chinese Phys. B

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The magnetocaloric effect of Mn, Ni, and Mn–Ni-doped EuTiO3 compounds are studied in the near-liquid-helium-temperature range. The Eu(Ti0.9375Mn0.0625)O3, Eu(Ti0.975Ni0.025)O3, and Eu(Ti0.9125Mn0.0625Ni0.025)O3 are prepared by the sol–gel method. The Eu(Ti0.9375Mn0.0625)O3 and Eu(Ti0.9125Mn0.0625Ni0.025)O3 exhibit ferromagnetism with second-order phase transition, and the Eu(Ti0.975Ni0.025)O3 displays antiferromagnetic behavior. Under the magnetic field change of 10 kOe (1 Oe = 79.5775 A⋅m−1), the values of magnetic entropy change are 8.8 J⋅kg−1⋅K−1, 12 J⋅kg−1⋅K−1, and 10.9 J⋅kg−1⋅K−1 for Eu(Ti0.9375Mn0.0625)O3, Eu(Ti0.975Ni0.025)O3, and Eu(Ti0.9125Mn0.0625Ni0.025)O3, respectively. The co-substitution of Mn and Ni can not only improve the magnetic entropy change, but also widen the refrigeration temperature window, which greatly enhances the magnetic refrigeration capacity. Under the magnetic field change of 10 kOe, the refrigerant capacity value of Eu(Ti0.9125Mn0.0625Ni0.025)O3 is 62.6 J⋅kg−1 more than twice that of EuTiO3 (27 J⋅kg−1), indicating that multi-component substitution can lead to better magnetocaloric performance.

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