| Method / sample set | ΔH | ΔS estimate |
|---|---|---|
| uMLIP (PBE sample set) |
— eV/atom
— kJ/mol of atoms
|
—
eV/(atom K)
— J/(mol of atoms K)
|
| PBE |
— eV/atom
— kJ/mol of atoms
|
—
eV/(atom K)
— J/(mol of atoms K)
|
| uMLIP (R2SCAN sample set) |
— eV/atom
— kJ/mol of atoms
|
—
eV/(atom K)
— J/(mol of atoms K)
|
| R2SCAN |
— eV/atom
— kJ/mol of atoms
|
—
eV/(atom K)
— J/(mol of atoms K)
|
ΔH is the liquid-minus-solid value reported by the existing correction workflow. Each uMLIP row uses the sample set matched to that DFT method. Uncertainties are standard errors; — means unavailable.
ΔS is estimated as ΔHuMLIP/Tm,uMLIP. Its propagated uncertainty assumes these two quantities are independent. The current PBE/R2SCAN correction inherits this entropy estimate; it is not an independently calculated DFT entropy.
| Sample set | Cp,solid | Cp,liquid |
|---|---|---|
| uMLIP (PBE sample set) |
— J/(mol of atoms K)
— eV/(atom K)
|
— J/(mol of atoms K)
— eV/(atom K)
|
| uMLIP (R2SCAN sample set) |
— J/(mol of atoms K)
— eV/(atom K)
|
— J/(mol of atoms K)
— eV/(atom K)
|
Values reported in SLUSCHI.out by the correction workflow. These are uMLIP potential-energy–temperature slopes for the PBE/R2SCAN sample sets, not full thermodynamic heat capacities or independent DFT heat capacities. The workflow may substitute the other phase's slope when one is unavailable. Uncertainties are not reported; — means unavailable.
| Vsolid [ų/atom] | Vliquid [ų/atom] | ΔV [ų/atom] |
|---|---|---|
| — | — | — |
No SLUSCHI.out has been received yet. The job may still be queued, pending, or starting on Sol.
Re2 1.0 2.7653358199999998 -0.0000000000000000 -0.0000000000000000 -1.3826679099999999 2.3948523599999998 0.0000000000000000 -0.0000000000000000 0.0000000000000000 4.4735766300000002 Re 2 direct 0.3333330000000000 0.6666670000000000 0.2500000000000000 Re 0.6666670000000000 0.3333330000000000 0.7500000000000000 Re
No output files have been received yet.