Pleas Ge rdeo e nn o Ct ah de j mu si ts mt r ya rgins
DOI: 10.1039/C7GC00387K
Journal Name
ARTICLE
exchange-correlation functional approximation for the 8. J. Anderson, F.-M. McKenna, A. Linares-Solano and R. K.
reaction pathway calculation and only gamma point is used for Wells, Catal Lett., 2007, 119, 16-20.
the Brillouin zone sampling. However, for the adsorption or 9. Z. Jiang, G. Lan, X. Liu, H. Tang and Y. Li, Catal. Sci. Technol.,
4
0
dissociation energy calculation, PBEsol functional with van
der Waals interaction involved and a (2×2×1) k-point grid are 10. H. Wang and F. Zhao, Int. J. Mol. Sci., 2007,
used to obtain more precise results. A plane wave basis set 11. T. Maegawa, A. Akashi, K. Yaguchi, Y. Iwasaki, M. Shigetsura,
2016, 6, 7259-7266.
8
, 628.
with an energy cutoff of 400 eV is used. A p (5×5) surpercell
containing a four-layer slab with 100 atoms was modeled. The
Y. Monguchi and H. Sajiki, Chem. Eur. J., 2009, 15, 6953-
6963.
periodic condition is employed along the x and y direction. The 12. J. M. Thomas, B. F. G. Johnson, R. Raja, G. Sankar and P. A.
vacuum space along the z direction was set to be 13 Å. For Midgley, Acc. Chem. Res., 2003, 36, 20-30.
alloy catalysts, taking RuPd catalyst as an example, Pd was 13. R. Raja, T. Khimyak, J. M. Thomas, S. Hermans and B. F. G.
alloyed to the sub-layer of Ru catalyst. The upper two layer Johnson, Angew. Chem. Int. Ed., 2001, 40, 4638-4642.
atoms in the cell are allowed to relax during the structure 14. Z. Guo, L. Hu, H.-h. Yu, X. Cao and H. Gu, RSC Adv., 2012,
optimization and the bottom two layer atoms are fixed. The 3477-3480.
relaxation is stopped when the force residue on the atom is 15. M. Li, F. Xu, H. Li and Y. Wang, Catal. Sci. Technol., 2016,
smaller than 0.02 eV/ Å. The transition states are calculated by 3670-3693.
using the climbing image nudged elastic band (CI-NEB) method 16. X. Xu, M. Tang, M. Li, H. Li and Y. Wang, ACS Catal., 2014,
2
6
4
,
,
,
4
1
.
3132-3135.
The adsorption and dissociation energy for molecule 17. M. Tang, S. Mao, M. Li, Z. Wei, F. Xu, H. Li and Y. Wang, ACS
chemisorption or dissociation are defined respectively as:
Eads/dis = Etot – Eslab – Emol
Catal., 2015, 5, 3100-3107.
18. R. A. Van Santen and M. Neurock, Catal. Rev., 1995, 37, 557-
Where Etot is the total energy after a molecule adsorption
698.
or dissociation the on catalysts; Eslab is the energy of the clean 19. C.-R. Chang, Z.-Q. Huang and J. Li, WIREs Comput. Mol. Sci.,
catalyst alone; Emol is the energy of the molecule in the gas
phase.
2016, 6, 679-693.
20. S. Siahrostami and A. Vojvodic, J. Phys. Chem. C., 2015, 119
,
The energy discrepancy is defined as:
ΔE = Eads/dis (1) - Eads/dis (2)
1032-1037.
21. X.-F. Yang, A. Wang, B. Qiao, J. Li, J. Liu and T. Zhang, Acc.
Chem. Res., 2013, 46, 1740-1748.
where (1) and (2) represent different molecules.
1
7
More details can refer to our previous work
.
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Somorjai, Nano Lett., 2007, , 3097-3101.
,
1
2
2
2
Acknowledgements
2
Financial support from the National Natural Science
Foundation of China (21622308, 91534114, 21376208), the
MOST (2016YFA0202900), the Fundamental Research Funds
for the Central Universities, and the computing time supported
by Special Program for Applied Research on Super
Computation of the NSFC-Guangdong Joint Fund (the second
phase) are greatly appreciated.
7
5. E. Schmidt, A. Vargas, T. Mallat and A. Baiker, J. Am. Chem.
Soc., 2009, 131, 12358-12367.
2
2
6. X. Xu, H. Li and Y. Wang, ChemCatChem, 2014, 6, 3328-3332.
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Delannoy, Phys. Chem. Chem. Phys., 2015, 17, 28022-28032.
8. X. Xu, Y. Li, Y. Gong, P. Zhang, H. Li and Y. Wang, J. Am. Chem.
Soc., 2012, 134, 16987-16990.
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