posted on 2017-02-15, 16:03authored byPiotr Konieczny, Łukasz Michalski, Robert Podgajny, Szymon Chorazy, Robert Pełka, Dominik Czernia, Szymon Buda, Jacek Mlynarski, Barbara Sieklucka, Tadeusz Wasiutyński
The rotating magnetocaloric
effect (RMCE) is a new issue in the field of magnetic refrigeration.
We have explored this subject on the two-dimensional (2D) enantiopure
{[MnII(R-mpm)2]2[NbIV(CN)8]}·4H2O (where mpm = α-methyl-2-pyridinemethanol)
coordination ferrimagnet. In this study, the magnetic and magnetocaloric
properties of single crystals were investigated along the bc//H easy plane and the a*//H hard axis. The observed small easy plane anisotropy
is due to the dipole–dipole interactions. For fields higher
than 0.5 T, no significant difference in the magnetocaloric effect
between both geometries was noticed. The maximal magnetic entropy
change for conventional effect was observed at 32 K and the magnetic
field change μ0ΔH = 5.0 T
attaining the value of ∼5 J mol–1 K–1. The obtained maximal value of −ΔSm is comparable to previously reported results for polycrystalline
octacyanidoniobate-based bimetallic coordination polymers. A substantial
anisotropy of magnetocaloric effect between the easy plane and hard
axis appears in low fields. This includes the presence of inverse
magnetocaloric effect only for the a*//H direction. The difference between both geometries was used to study
the rotating magnetocaloric effect. We show that the inverse part
of magnetocaloric effect can be used to enhance the rotating magnetic
entropy change up to 51%. This finding is of key importance for searching
efficient materials for RMCE.