TY - JOUR
T1 - Al substitution effect on magnetic properties of magnetocaloric material HoB2
AU - Iwasaki, Suguru
AU - Yamamoto, Takafumi D.
AU - Baptista de Castro, Pedro
AU - Terashima, Kensei
AU - Takeya, Hiroyuki
AU - Takano, Yoshihiko
N1 - Publisher Copyright:
© 2021
PY - 2022/2/1
Y1 - 2022/2/1
N2 - We investigate the Al substitution effect for HoB2 to tune the Curie temperature (TC). The HoB2−xAlx samples with nominal x (xnom) of 0, 0.1, 0.3, and 0.5 are characterized by powder X-ray diffraction measurements, EDS analysis and magnetization measurements. The HoB2−xAlx samples with xnom of 0.1, 0.3, and 0.5 show two ferromagnetic transitions at TC1 of ∼15 K and TC2 of >32 K. The TC1 is identical to the TC of HoB2 and does not change with Al substitution. The TC2 is similar to the TC of HoAl2 and varies with Al content. In an EDS analysis, the inhomogeneous elemental distribution is observed in Al-substituted HoB2, where the Al-rich regions exist. Our results suggest that the Al added to HoB2 does not form a solid solution, but rather leads to the phase segregation into stoichiometric HoB2 and B-substituted HoAl2. The xnom = 0.5 sample exhibits the maximum |ΔSM(μ0H:5 T→0 T)| of 32.1 J kg K−1 at TC1 and a small kink of |ΔSM| at TC2. Because the |ΔSM| exhibits a maximum at TC1, stoichiometric HoB2 mainly contributes to the maximum of |ΔSM|.
AB - We investigate the Al substitution effect for HoB2 to tune the Curie temperature (TC). The HoB2−xAlx samples with nominal x (xnom) of 0, 0.1, 0.3, and 0.5 are characterized by powder X-ray diffraction measurements, EDS analysis and magnetization measurements. The HoB2−xAlx samples with xnom of 0.1, 0.3, and 0.5 show two ferromagnetic transitions at TC1 of ∼15 K and TC2 of >32 K. The TC1 is identical to the TC of HoB2 and does not change with Al substitution. The TC2 is similar to the TC of HoAl2 and varies with Al content. In an EDS analysis, the inhomogeneous elemental distribution is observed in Al-substituted HoB2, where the Al-rich regions exist. Our results suggest that the Al added to HoB2 does not form a solid solution, but rather leads to the phase segregation into stoichiometric HoB2 and B-substituted HoAl2. The xnom = 0.5 sample exhibits the maximum |ΔSM(μ0H:5 T→0 T)| of 32.1 J kg K−1 at TC1 and a small kink of |ΔSM| at TC2. Because the |ΔSM| exhibits a maximum at TC1, stoichiometric HoB2 mainly contributes to the maximum of |ΔSM|.
KW - Al substitution
KW - HoB
KW - Magnetic refrigeration
UR - http://www.scopus.com/inward/record.url?scp=85120627041&partnerID=8YFLogxK
U2 - 10.1016/j.ssc.2021.114616
DO - 10.1016/j.ssc.2021.114616
M3 - Article
AN - SCOPUS:85120627041
SN - 0038-1098
VL - 342
JO - Solid State Communications
JF - Solid State Communications
M1 - 114616
ER -