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Free Energies of Formation of Metal Clusters and Nanoparticles from Molecular Simulations: Al n with n = 2−60
Efficient simulation methods are presented for determining the standard Gibbs free energy changes for the reactions, M + M n -1 ↔ M n (R1), involved in the formation of atomic clusters and nanoparticles (also called particles) in the vapor phase. The standard Gibbs free energy of formation (Δf G°) o...
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Published in: | Journal of physical chemistry. C 2007-11, Vol.111 (44), p.16227-16242 |
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Main Authors: | , , , , |
Format: | Article |
Language: | English |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | Efficient simulation methods are presented for determining the standard Gibbs free energy changes for the reactions, M + M n -1 ↔ M n (R1), involved in the formation of atomic clusters and nanoparticles (also called particles) in the vapor phase. The standard Gibbs free energy of formation (Δf G°) of a particle is obtained from these Gibbs free energy changes (ΔG°) by a recursion relationship using the experimental Δf G° of the monomer. In the present study, this method has been applied to reactions involving Al n particles with n = 2−60. This method has been validated for n = 2, where the experimental thermodynamic properties of Al2 have been recompiled using the latest available experimental or highly accurate theoretical data. For n = 2−4, two completely different approaches, a Monte Carlo configuration integral (MCCI) integration of partition functions and a Monte Carlo direct simulation of the equilibrium constants (MCEC), employing four well-validated potential energy functions have been used to calculate ΔG° of R1. Excellent agreement is observed for these two methods. Although different potential energy functions give different stage-1 results for n ≤ 10, three high-level correction (HLC) terms, namely, a correction for the potential energy difference of the global minima, another for the electronic excitation contribution, and a third based on calculating isomeric−rovibrational contribution, have been applied to mitigate deficiencies in the potential energy functions. For n = 2, good agreement has been found between the corrected simulation results and experimental data. For larger n, the more efficient MCEC method has been used. Finally, accurate ΔG° of R1 and thus Δf G° of Al n particles with n = 2−60 have been determined. This is the first example of the determination of nanoparticle free energies of formation. |
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ISSN: | 1932-7447 1932-7455 |
DOI: | 10.1021/jp073559v |