Beongki Cho1,Songhee Han2
GIST1,Mokpo National Maritime University2
Beongki Cho1,Songhee Han2
GIST1,Mokpo National Maritime University2
The RB<sub>4</sub> (R = Gd, Tb, Dy, Ho, and Tm) compound presents an intriguing system with simultaneous magnetic ordering and geometrical frustration, leading to a strong interaction within the matarial. The interaction manifests in consecutive magnetic transitions at temperatures <i>T</i> = <i>T</i><sub>N1</sub> and <i>T</i><sub>N2</sub> (where <i>T</i><sub>N1</sub> > <i>T</i><sub>N2</sub>) and results in a highly anisotropic magnetic configuration when in an ordered state. In this study, we systematically investigate the anisotropic entropy chnage (ΔS<sub>AN</sub>) of single crystals of RB<sub>4</sub> (R = Dy, Ho, and Tm). Our findings reveal distinct behavior: the negative entropy change above <i>T</i><sub>N1</sub> follows conventional field-dependence, while a positive entropy change below <i>T</i><sub>N1</sub> follows anomalous field-dependence. Notably, ErB<sub>4</sub> (<i>T</i><sub>N1</sub> = 15.5 K) and TmB<sub>4</sub> (<i>T</i><sub>N1</sub> = 11.7 K) demonstrate ΙΔS<sub>AN</sub>Ι values of ≈ 11.6 J/(K kg) and 10.2 J/(K kg), respectively, at <i>T</i> > <i>T</i><sub>N1</sub> and for <i>H</i> = 50 kOe, accompanied by relative cooling power (RCP) values of ≈ 237.1 J/kg and 225.9 J/kg. Interestingly, DyB<sub>4</sub> (<i>T</i><sub>N1</sub> = 20.5 K) exchibits a significant ΙΔS<sub>AN</sub>Ι value of 18.8 J/(K kg) near <i>T</i> = <i>T</i><sub>N2</sub> (= 13.0 K) and an RCP value of ≈ 208.39 J/kg for <i>H</i> = 50 kOe. These ΙΔS<sub>AN</sub>Ι and RCP values demonstrate the potential of these comounds for applications in refrigeration using rotational magnetocaloric effect (RMCE). Additionally, HoB<sub>4</sub>, ErB<sub>4</sub> and TmB<sub>4</sub> exchibit also promising behavior for RMCE even at temperatures of <i>T</i> < <i>T</i><sub>N1 </sub>and particularly during low-field cooling (<i>H</i> < 50 kOe). This work highlights the suitability of RB<sub>4</sub> compounds as effective materials for RMCE cooling, covering a broad temperature range above and below the antiferromagnetic Néel temperature. Specifically, the anisotropic entropy change observed in DyB<sub>4</sub> near <i>T</i>= <i>T</i><sub>N2</sub> holds considerable potential for RMCE applications, such as hydrogen liquefaction due to its occurrence which a limited temperture range, accompanied by large ΙΔS<sub>AN</sub>Ι and RCP values.