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Page 8 of 37                            Ye et al. J Mater Inf 2023;3:15  https://dx.doi.org/10.20517/jmi.2023.08

               The molar Gibbs energies of Fe Tb , Fe Tb , Fe Tb, Fe Dy , Fe Dy , Fe Dy, Fe Er , Fe Er , Fe Er, Fe Lu ,
                                                                                                     23
                                                                                         23
                                              2
                                          17
                                                                                            6
                                                                                     2
                                                                                                        6
                                                                                               3
                                                 23
                                                                         6
                                                                     23
                                                                                  17
                                                                            3
                                                        3
                                                     6
                                                                  2
                                                              17
               Fe Lu, Fe Y , Fe Y, and Fe Y can be expressed based on the Neumann-Kopp rule as:
                 3
                       23 6
                                     2
                             3
               in which b and q represent the stoichiometric numbers, J and K represent the optimized parameters.
               -                and                  , as shown in Equation (6) and Equation (7), are the magnetic contribution to
               the molar Gibbs energy, and the formula is expressed by Equation (3). T  and β  of the Fe-RE intermetallic
                                                                             C
                                                                                   0
               compounds used in the present work can be found in Tables 1-5, respectively.
               Thermodynamic calculation
               The parameters of all stable phases in the Fe-RE (RE = Tb, Dy, Er, Lu, and Y) binary systems were
               optimized using the PARROT module of Thermo-Calc software  considering the experimental
                                                                           [136]
               information (e.g., phase equilibria, enthalpy of mixing, enthalpy of formation, and heat capacity) reported
               in the literature. As for the Fe-RE binary systems, the experimental data are relatively limited because of the
               experimental difficulties. However, the systematic trends were observed for the thermodynamic
               characteristics of the RE-B , RE-Mn [137,138] , and RE-Ni  binary systems with the increasing of RE atomic
                                                              [139]
                                      [24]
               numbers. The Fe-RE binary systems also show a similar systematic trend, which was considered in the
               present calculations. For example, because the experimental enthalpy of mixing of liquid Fe-Er alloys was
               not  reported  in  the  literature,  which  was  estimated  by  Konar  et al.   using  the  formula
                                                                                     [19]
               [ΔH mix,Fe − Er  = ΔH mix,Fe − Dy  + 0.5(ΔH mix,Fe − Lu  − ΔH mix,Fe − Dy )], where ΔH mix,Fe − Lu  and ΔH mix,Fe − Dy  were obtained from
               the measured experimental results .
                                            [98]
               The thermodynamic parameters were optimized finally, as shown in Tables 1-5, respectively. The enthalpy
               of formation (including the reported experimental results and the calculated results by the CALPHAD
               method and first-principles calculation) and the crystal structure data of the Fe-RE intermetallic
               compounds are shown in the Supplementary Materials.
               CALCULATED RESULTS
               Fe-Tb and Fe-Dy
               Thermodynamic parameters of liquid phase and Fe Tb and Fe Dy were assessed in consideration of the
                                                            2
                                                                      2
               experimental results  and the calculations . In this work, the calculated Fe-Tb binary system is compared
                                [101]
                                                    [27]
               with the measured data [92,93,95]  and the calculations , as shown in Figure 1. The temperatures of invariant
                                                          [104]
               reactions in the Fe-Tb binary system are calculated as listed in Table 6. The present calculations agree with
               the reported calculations [27,104] , and the optimized parameters are shown in Table 1.
               The presently calculated enthalpy of mixing and partial enthalpy of mixing in liquid Fe-Tb alloys at 1,833 K
               are accordant well with the calculations , as shown in Figure 2 and Figure 3. The enthalpies of formation
                                                 [27]
               of the Fe-Tb intermetallic compounds are calculated at 298 K in Figure 4, which is in good accordance with
               the calculations [19,27,104,140]  and the experimental data [54,102] . The presently calculated enthalpy of formation of
               Fe Tb is -9.005 kJ/mol-atom. As presented in Figure 5, the calculated thermodynamic properties [e.g., heat
                 2
               capacity, the entropy of formation, and enthalpy difference                  of Fe Tb] are in accordance with the
               data  and show no artificial break point at 120 K in the heat capacity curve.
                   [101]
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