“…[10][11][12][13] In addition, it is important to explore magnetocaloric materials at the cryogenic temperature, which would be beneficial for hydrogen or helium liquefaction and space science. [5,14] Over the past few decades, attention has mostly been paid to cryogenic magnetocaloric materials with rare-earth based alloys and oxides, such as Gd 3 B 5 O 12 (B = Ga, Fe, Al), [15] RM 2 (R = rare earth elements, M = Al, Ni, Co), [16][17][18] RM (M = Zn, Ga), [19][20][21][22] RMX (M = Fe, Co, X = Al, Mg, C), [23,24] R 2 T 2 X (T = Cu, Ni, Co, X = In, Al, Ga, Sn, and so on), [25] R 60 Co 20 Ni 20 (R = Ho and Er), [26] La 1−x Pr x Fe 12 B 6 , [27] Gd 20 Ho 20 Tm 20 Cu 20 Ni 20 , [28] DyNiGa, [2] dual-phase HoNi/HoNi 2 composite, [29] RNO 3 (N = Al, Fe, Mn, Cr, and so on), [30][31][32][33][34][35][36][37] and R 2 M 2 O 7 . [38][39][40][41][42] In particular, recent studies have demonstrated that the Gd 3+ and Eu 2+ ion-based compounds display great MCE performances due to the large angular momentum of the half-filled 4f shell (4f 7 ) and negligible crystal electrical field (CEF) effect with J = S = 7/2, L = 0, with the representative compounds such as GdFeO 3 , [43] GdScO 3 , [44] GdCrO 3 , [45] GdAlO 3 ,…”