Models studied in this work. These include metallic glass-forming models based on the embedded atom method (EAM) potential, Kob-Andersen model based on Lennard-Jones potential (KA-LJ), Weeks-Chandler-Andersen model based on Lennard-Jones potential (WCA-LJ), and the three-body Tersoff potential for SiO2.
# . | System . | Force-field . | Conditions . |
---|---|---|---|
1 | Al85Sm15 | EAM | NPT (p = 0, and different p) |
2 | Ni80P20 | EAM | NPT (p = 0) |
3 | Y65Cu35 | EAM | NPT (p = 0) |
4 | Pd80Si20 | EAM | NPT (p = 0) |
5 | A80B20 | KA-LJ | NVT (N/V = 1.558) |
6 | A80B20 | WCA-LJ | NVT (N/V = 1.558) |
7 | SiO2 | Tersoff | NPT (p = 0) |
# . | System . | Force-field . | Conditions . |
---|---|---|---|
1 | Al85Sm15 | EAM | NPT (p = 0, and different p) |
2 | Ni80P20 | EAM | NPT (p = 0) |
3 | Y65Cu35 | EAM | NPT (p = 0) |
4 | Pd80Si20 | EAM | NPT (p = 0) |
5 | A80B20 | KA-LJ | NVT (N/V = 1.558) |
6 | A80B20 | WCA-LJ | NVT (N/V = 1.558) |
7 | SiO2 | Tersoff | NPT (p = 0) |
Models studied in this work. These include metallic glass-forming models based on the embedded atom method (EAM) potential, Kob-Andersen model based on Lennard-Jones potential (KA-LJ), Weeks-Chandler-Andersen model based on Lennard-Jones potential (WCA-LJ), and the three-body Tersoff potential for SiO2.
# . | System . | Force-field . | Conditions . |
---|---|---|---|
1 | Al85Sm15 | EAM | NPT (p = 0, and different p) |
2 | Ni80P20 | EAM | NPT (p = 0) |
3 | Y65Cu35 | EAM | NPT (p = 0) |
4 | Pd80Si20 | EAM | NPT (p = 0) |
5 | A80B20 | KA-LJ | NVT (N/V = 1.558) |
6 | A80B20 | WCA-LJ | NVT (N/V = 1.558) |
7 | SiO2 | Tersoff | NPT (p = 0) |
# . | System . | Force-field . | Conditions . |
---|---|---|---|
1 | Al85Sm15 | EAM | NPT (p = 0, and different p) |
2 | Ni80P20 | EAM | NPT (p = 0) |
3 | Y65Cu35 | EAM | NPT (p = 0) |
4 | Pd80Si20 | EAM | NPT (p = 0) |
5 | A80B20 | KA-LJ | NVT (N/V = 1.558) |
6 | A80B20 | WCA-LJ | NVT (N/V = 1.558) |
7 | SiO2 | Tersoff | NPT (p = 0) |
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