BJP Potential (Bouhadja)¶
The BJP potential, developed by Bouhadja et al., is a Born-Mayer-Huggins (BMH) force field specifically parameterized for calcium aluminosilicate (CAS) glass systems. It provides accurate structural and thermodynamic properties for Ca-Al-Si-O compositions.
Reference¶
Y. Bouhadja, N. Jakse, A. Pasturel. "Structural and dynamic properties of calcium aluminosilicate melts: a molecular dynamics study", J. Chem. Phys. 138, 224510 (2013). DOI:10.1063/1.4809523
Functional Form¶
The total pairwise interaction energy uses the Born-Mayer-Huggins form:
where:
| Symbol | Description |
|---|---|
| \(A_{ij}\) | Repulsion energy prefactor (eV) |
| \(\rho_{ij}\) | Repulsion range parameter (Å) |
| \(C_{ij}\) | Van der Waals attraction coefficient (eV·Å⁶) |
| \(D_{ij}\) | Dipole-quadrupole correction coefficient (eV·Å⁸) |
| \(q_i, q_j\) | Partial atomic charges |
The Coulomb interactions are handled within the LAMMPS born/coul/dsf pair style with a DSF damping parameter of 0.25 Å⁻¹ and a cutoff of 8.0 Å.
LAMMPS pair style: born/coul/dsf 0.25 8.0
Charges¶
All charges are fixed at:
| Element | Charge (\(e\)) |
|---|---|
| O | −1.2 |
| Ca | +1.2 |
| Al | +1.8 |
| Si | +2.4 |
Note: These are the same partial charges as in the PMMCS potential, consistent with the factor-of-0.6 scaling from formal charges.
Supported Elements¶
BJP supports a focused set of 4 elements:
| Element | Role in glass |
|---|---|
| Si | Network former |
| Al | Network former / intermediate |
| Ca | Network modifier |
| O | Anion |
This makes BJP specifically designed for CAS glasses such as: - Anorthite (CaAl₂Si₂O₈) - Gehlenite (Ca₂Al₂SiO₇) - Wollastonite (CaSiO₃) - General Ca-Al-Si-O compositions
Usage¶
from amorphouspy import get_structure_dict, generate_potential
# BJP works only with Ca-Al-Si-O compositions
structure_dict = get_structure_dict(
{"CaO": 0.25, "Al2O3": 0.25, "SiO2": 0.5},
target_atoms=3000,
)
potential = generate_potential(structure_dict, potential_type="bjp")
What the generator produces¶
The BJP generator creates LAMMPS configuration lines that:
1. Define the born/coul/dsf pair style (BMH + DSF Coulomb in one style)
2. Set atomic charges
3. Define BMH parameters (\(A\), \(\rho\), \(\sigma\), \(C\), \(D\)) for all pair interactions
Technical Details¶
Born-Mayer-Huggins vs. Buckingham¶
The BMH form used by BJP differs from the standard Buckingham potential in two ways: - It includes a \(D/r^8\) dipole-quadrupole correction term - The repulsion uses the form \(A \exp(-r/\rho)\) rather than \(A \exp(-Br)\)
These extra terms provide better reproduction of melt structure and dynamics for CAS systems.
When to use BJP¶
- Pure CAS glass studies — Ca-Al-Si-O compositions exclusively
- Structural properties — well-validated for RDFs, coordination, and Qⁿ distributions in CAS melts
- High-temperature melt dynamics — parameterized against ab initio MD of CAS melts
Limitations¶
- Only 4 elements — cannot model glasses with Na, K, Mg, B, or other modifiers
- Adding additional elements requires reparameterization
- Not suitable for borosilicate or alkali silicate glasses