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76 changes: 76 additions & 0 deletions input/thermo/libraries/surfaceThermoCovDepPt111.py
Original file line number Diff line number Diff line change
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name = "Coverage Dependent Thermo for Pt(111)"
shortDesc = u"thermo with coverage dependence for Pt(111) surface species"
longDesc = u"""
COX coverage dependence as calculated by Jongyoon Bae, Bjarne Kreitz, Andrew A. Peterson, and C. Franklin Goldsmith
Journal of Chemical Information and Modeling 2025 65 (7), 3461-3476
DOI: 10.1021/acs.jcim.4c02167
Polynomial coeffients taken from global minimum Pt Table S3. See Supplemental Material.
"""


entry(
index = 1,
label = "X",
molecule =
"""
1 X u0 p0 c0
""",
thermo = NASA(
polynomials = [
NASAPolynomial(coeffs=[0.0,0,0,0,0,0.0,0.0], Tmin=(298,'K'), Tmax=(1000,'K')),
NASAPolynomial(coeffs=[0.0,0,0,0,0,0.0,0.0], Tmin=(1000,'K'), Tmax=(2000,'K')),
],
Tmin = (298,'K'),
Tmax = (2000,'K'),
),
shortDesc = u"""library value for a vacant surface site""",
longDesc = u"""Zeros, by definition.""",
metal = "Pt",
facet = "111",
)


entry(
index = 2,
label = "XCO",
molecule =
"""
1 X u0 p0 c0 {2,D}
2 C u0 p0 c0 {1,D} {3,D}
3 O u0 p2 c0 {2,D}
""",
thermo=NASA(
polynomials=[
NASAPolynomial(coeffs=[1.42895000E+00, 1.40374509E-02, -2.21178920E-05, 1.78659581E-08, -5.71478802E-12,
-3.45688484E+04, -7.78265517E+00], Tmin=(298.0, 'K'), Tmax=(1000.0, 'K')),
NASAPolynomial(coeffs=[5.48656312E+00, -1.68118543E-03, 3.09030310E-06, -1.71186643E-09, 3.15864598E-13,
-3.54815495E+04, -2.76788365E+01], Tmin=(1000.0, 'K'), Tmax=(2000.0, 'K')),
],
Tmin=(298.0, 'K'),
Tmax=(2000.0, 'K'),
thermo_coverage_dependence = {
"""
1 C u0 p0 {2,D} {3,D}
2 O u0 p2 {1,D}
3 X u0 p0 {1,D}
""": {
'model': 'polynomial',
'enthalpy-coefficients': [(0.312, 'eV/molecule'), (-0.323, 'eV/molecule'), (0.890, 'eV/molecule')],
'entropy-coefficients': [(1.11e-4, 'eV/(molecule*K)'), (-6.48e-5, 'eV/(molecule*K)'), (-1.63e-4, 'eV/(molecule*K)')]
}
},
),
longDesc=u"""Calculated by Bjarne Kreitz at Brown University using statistical mechanics (file: ThermoPt111.py).
Based on DFT calculations by Bjarne Kreitz from Brown University. DFT calculations were performed with Quantum Espresso
using PAW pseudopotentials and the BEEF-vdW functional for an optimized 3x3 supercell (1/9ML coverage)
following the procedure outlined by Blondal et al (DOI:10.1021/acs.iecr.9b01464). The following settings were applied:
kpoints=(5x5x1), 4 layers (2 bottom layers fixed), ecutwfc=60 Ry, smearing='mazari-vanderbilt', mixing_mode='local-TF',
fmax=2.5e-2. DFT binding energy: -1.415 eV.
COX coverage dependence calculated by Jongyoon Bae, Bjarne Kreitz, Andrew A. Peterson, and C. Franklin Goldsmith
Journal of Chemical Information and Modeling 2025 65 (7), 3461-3476
DOI: 10.1021/acs.jcim.4c02167
Polynomial coeffients taken from global minimum Pt Table S3. See Supplemental Material.
""",
metal="Pt",
facet="111",
)
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