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Fixed CO2RR Ag111 library descriptions
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input/thermo/libraries/CO2RR_Adsorbates_Ag111.py

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solvent = "water"
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shortDesc = u"CO2RR adsorbate thermochemistry on Ag(111) from DFT"
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longDesc = u"""
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NASA polynomial thermochemistry for C1 and C2 adsorbate intermediates
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relevant to electrochemical CO2 reduction (CO2RR) on Ag(111).
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Adsorbates are labeled with a trailing or interleaved 'X' to indicate
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surface binding sites, per RMG conventions.
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This library contains NASA polynomial thermochemistry for adsorbate
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intermediates relevant to electrochemical CO2 reduction (CO2RR) on the
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Ag(111) surface. All adsorbates are denoted with a trailing 'X' (or
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interleaved 'X' for bidentate species) to indicate surface binding sites,
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consistent with RMG conventions.
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DFT (Manish Kumar Kothakonda, Northeastern): VASP with PBE + Grimme D3
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zero-damping (IVDW = 12) and PAW pseudopotentials.
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A two-stage protocol was used:
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Initial geometries were pre-optimized at ENCUT = 400 eV with a 3x3x1
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Monkhorst-Pack k-mesh, then fully re-relaxed to force convergence at
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tighter settings of ENCUT = 500 eV and 4x4x1 k-mesh (IBRION = 2,
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EDIFFG = -0.03 eV/A). All final energies - adsorbate slabs, bare-slab
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reference, and vibrational frequencies - were computed at the tight
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settings.
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DFT calculations were performed by Manish Kumar Kothakonda (Northeastern University).
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Geometry optimization of adsorbates on a periodic Ag(111) slab.
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Calculations used VASP 6.3.1 with the PBE exchange-correlation functional,
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Grimme D3 zero-damping dispersion correction (IVDW = 12), and PAW
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pseudopotentials. Plane-wave cutoff ENCUT = 500 eV; 3x3x1 Gamma-centered
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Monkhorst-Pack k-point mesh; Methfessel-Paxton smearing (ISMEAR = 1,
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SIGMA = 0.10 eV); spin-polarized (ISPIN = 2); SCF convergence
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EDIFF = 1E-6 eV; ionic force convergence EDIFFG = -0.03 eV/A
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(IBRION = 2). The slab is a hexagonal Ag(111) supercell with lattice
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parameters a = b = 11.506 A, c = 31.046 A (cell volume 3559.27 A^3),
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containing 64 Ag atoms arranged in 4 atomic layers; the bottom 3 layers
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were held fixed (F F F) while the top layer plus adsorbate atoms were
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allowed to relax (T T T). Implicit solvation in water was applied via
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VASPsol. Harmonic vibrational frequencies were computed using finite-difference
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displacements (IBRION = 5, NFREE = 2, POTIM = 0.015 A) on the relaxed
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atoms (adsorbate plus top slab layer).
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Post-processing and thermo (Su Sun) via the Westgroup pipeline
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(adapted from input_generator.py and compute_NASA_for_adsorbates): VASP
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outputs converted to ASE .traj and inspected; vibrational frequencies
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Post-processing and stat thermo calculations were performed by
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Su Sun (Northeastern University) via the Westgroup pipeline
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(adapted from input_generator.py and compute_NASA_for_adsorbates):
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VASP outputs converted to ASE .traj and inspected; vibrational frequencies
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and ZPEs consolidated into per-species zpe_log_<species>.txt files;
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imaginary modes replaced with 12 cm^-1. Heat of formation at 0 K was
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computed from a thermochemical cycle against CH4, H2O, and H2 references

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