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Hu et al. J Mater Inf 2023;3:1 I http://dx.doi.org/10.20517/jmi.2022.28 Page 5 of 15

Table 1. Properties of binary systems explored by experiments

A B (eV/atom) (Å) (amu, g/mol) / / / Glass type Condition1 Condition2 Condition3
Ag Ca 2.95 1.44 107.87 0.6237 1.3681 0.372 ribbon 0 0 1
Si Ag 4.63 1.1 28.085 0.6371 1.3091 3.841 ribbon 0 0 0
Al Ca 3.39 1.4 26.982 0.5428 1.4071 1.485 bulk 0 0 1
Cu Al 3.49 1.26 63.546 0.9713 1.1111 0.425 ribbon 0 0 1
Zr Al 6.25 1.58 91.224 0.5424 0.8861 0.296 film 1 1 1
Ge Au 3.85 1.14 72.63 0.9896 1.2544 2.712 ribbon 0 0 0
Hf Au 6.44 1.58 178.49 0.5916 0.9051 1.104 ribbon 1 0 1
Si Au 4.63 1.1 28.085 0.8229 1.3 7.013 ribbon 0 0 0
Au Sn 3.81 1.43 196.97 0.8241 1.0839 0.603 ribbon 0 0 1
Zr Au 6.25 1.58 91.224 0.6096 0.9051 2.159 ribbon 1 0 1
B Co 5.81 0.88 10.81 0.7556 1.4205 5.452 ribbon 0 0 0
B Fe 5.81 0.88 10.81 0.7367 1.4205 5.166 ribbon 0 0 0
B Ni 5.81 0.88 10.81 0.7642 1.4318 5.430 ribbon 0 0 0
Ti Be 4.85 1.42 47.867 0.6845 0.8169 0.188 ribbon 1 1 1
Zr Be 6.25 1.58 91.224 0.5312 0.7342 0.099 ribbon 1 1 1
Ca Mg 1.84 1.97 40.078 0.8207 0.8122 0.606 ribbon 1 1 1
Ca Zn 1.84 1.97 40.078 0.7337 0.7056 1.631 ribbon 1 0 1
Hf Co 6.44 1.58 178.49 0.6817 0.7911 0.330 ribbon 1 1 1
Co P 4.39 1.25 58.933 0.7813 0.848 0.526 ribbon 1 1 0
Ti Co 4.85 1.42 47.867 0.9052 0.8803 1.231 bulk 1 0 1
Zr Co 6.25 1.58 91.224 0.7024 0.7911 0.646 ribbon 1 1 1
Hf Cu 6.44 1.58 178.49 0.5419 0.7975 0.356 bulk 1 1 1
Cu Mg 3.49 1.26 63.546 0.4327 1.2698 0.382 ribbon 0 0 1
Ti Cu 4.85 1.42 47.867 0.7196 0.8873 1.328 ribbon 1 0 1
Y Cu 4.37 1.8 88.906 0.7986 0.7 0.715 ribbon 1 1 1
Zr Cu 6.25 1.58 91.224 0.5584 0.7975 0.697 bulk 1 1 1
Hf Fe 6.44 1.58 178.49 0.6646 0.7911 0.313 film 1 1 1
Fe P 4.28 1.25 55.845 0.8014 0.848 0.555 ribbon 1 1 0
Si Fe 4.63 1.1 28.085 0.9244 1.1364 1.988 film 0 0 0
Fe Sn 4.28 1.25 55.845 0.7336 1.24 2.126 film 0 0 1
Zr Fe 6.25 1.58 91.224 0.6848 0.7911 0.612 ribbon 1 1 1
Hf Ge 6.44 1.58 178.49 0.5978 0.7215 0.407 ribbon 1 1 0
Pd Ge 3.89 1.4 106.42 0.9897 0.8143 0.682 ribbon 1 1 0
Pt Ge 5.84 1.39 195.08 0.6592 0.8201 0.372 ribbon 1 1 0
Zr Ge 6.25 1.58 91.224 0.616 0.7215 0.796 ribbon 1 1 0
Hf Ni 6.44 1.58 178.49 0.6894 0.7975 0.329 ribbon 1 1 1
Hf Si 6.44 1.58 178.49 0.7189 0.6962 0.157 ribbon 1 1 0
Ni Mg 4.44 1.26 58.693 0.3401 1.2698 0.414 ribbon 0 0 1
Y Mg 4.37 1.8 88.906 0.3455 0.8889 0.273 ribbon 1 1 1
Mg Zn 1.51 1.6 24.305 0.894 0.8687 2.690 ribbon 1 0 1
Zr Mg 6.25 1.58 91.224 0.2416 1.0127 0.266 ribbon 0 0 1
Si Mn 4.63 1.1 28.085 0.6307 1.2 1.956 ribbon 0 0 0
Zr Mn 6.25 1.58 91.224 0.4672 0.8354 0.602 film 1 1 1
Mo Zr 6.82 1.39 95.95 0.9164 1.1367 0.951 ribbon 0 0 1
Nb Ni 7.57 1.5 92.906 0.5865 0.84 0.632 bulk 1 1 1
Nb Si 7.57 1.5 92.906 0.6116 0.7333 0.302 ribbon 1 1 0
Ni P 4.44 1.26 58.693 0.7725 0.8413 0.528 ribbon 1 1 0
Ni Pd 4.44 1.26 58.693 0.8761 1.1111 1.813 film 0 0 1
Ti Ni 4.85 1.42 47.867 0.9155 0.8873 1.226 film 1 0 1
Ta Ni 8.1 1.54 180.95 0.5481 0.8182 0.324 ribbon 1 1 1
Ni Y 4.44 1.26 58.693 0.9842 1.4286 1.515 film 0 0 1
Zr Ni 6.25 1.58 91.224 0.7104 0.7975 0.643 ribbon 1 1 1
Pd P 3.89 1.4 106.42 0.8817 0.7571 0.291 film 1 1 0
Pt P 5.84 1.39 195.08 0.5873 0.7626 0.159 ribbon 1 1 0
Si Pd 4.63 1.1 28.085 0.8402 1.2727 3.789 bulk 0 0 0
Zr Pd 6.25 1.58 91.224 0.6224 0.8861 1.167 ribbon 1 0 1
Pt Sb 5.84 1.39 195.08 0.4709 1.1151 0.624 ribbon 0 0 1
Pt Si 5.84 1.39 195.08 0.7928 0.7914 0.144 ribbon 1 1 0
Pt Ti 5.84 1.39 195.08 0.8305 1.0216 0.245 ribbon 0 0 1
Zr Pt 6.25 1.58 91.224 0.9344 0.8797 2.138 ribbon 1 0 1
Ti Si 4.85 1.42 47.867 0.9546 0.7746 0.587 ribbon 1 1 0
Zr Si 6.25 1.58 91.224 0.7408 0.6962 0.308 ribbon 1 1 0
Condition1: ≥ and ≥ ; Condition2: ≥ and ≥ and ≥ ; Condition3: both elements A and B are metals

2.2. Measuring glass-forming ability
After obtaining the quenched solids from the computer simulations, we employed bond orientational order
parameters to characterize the local structures [11,20] . Taking any particle in the simulation box, the nearest