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Large reversible magnetocaloric effect in antiferromagnetic Ho2O3 powders
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AbstractGiant magnetocaloric materials are highly promising for technological applications in magnetic refrigeration. Although giant magnetocaloric effects were discovered in first-order magnetic transition materials, it is accompanied by some non-desirable drawbacks, such as important hysteretic phenomena, irreversibility of the effect, or poor mechanical stability, which limits their use in applications. Here, we report the discovery of a giant magnetocaloric effect in commercialized Ho2O3 oxide at low temperature (around 2 K) without hysteresis losses. Ho2O3 is found to exhibit a second-order antiferromagnetic transition with a Néel temperature of 2 K. At an applied magnetic field change of 5 T and below 3.5 K, the maximum value of magnetic entropy change $$(-\Delta {{\rm{S}}}_{M}^{max})$$
(
-
Δ
S
M
max
)
, the refrigerant capacity (RC) were found to be 31.9 J.K−1.kg−1 and 180 J.K−1, respectively.
Springer Science and Business Media LLC
Title: Large reversible magnetocaloric effect in antiferromagnetic Ho2O3 powders
Description:
AbstractGiant magnetocaloric materials are highly promising for technological applications in magnetic refrigeration.
Although giant magnetocaloric effects were discovered in first-order magnetic transition materials, it is accompanied by some non-desirable drawbacks, such as important hysteretic phenomena, irreversibility of the effect, or poor mechanical stability, which limits their use in applications.
Here, we report the discovery of a giant magnetocaloric effect in commercialized Ho2O3 oxide at low temperature (around 2 K) without hysteresis losses.
Ho2O3 is found to exhibit a second-order antiferromagnetic transition with a Néel temperature of 2 K.
At an applied magnetic field change of 5 T and below 3.
5 K, the maximum value of magnetic entropy change $$(-\Delta {{\rm{S}}}_{M}^{max})$$
(
-
Δ
S
M
max
)
, the refrigerant capacity (RC) were found to be 31.
9 J.
K−1.
kg−1 and 180 J.
K−1, respectively.
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