### Abstract

The adsorption of ethene on the (111) surface of copper has been studied by using density functional theory calculations with gradient corrections. The surface is described by a periodic (3 x 3) slab, three layers thick, with ethene adsorbed on one side. The energy of the adsorption shows great sensitivity to the k-point sampling employed, with single k-point calculations overestimating the binding by over 800% when compared with a calculation converged with respect to the k-point sampling. In addition, the structure of the adsorbed molecule is considerably distorted, which is in contradiction with conclusions drawn from the experimental vibrational frequencies.

Calculations that are converged with respect to the k-point sampling indicate a much weaker interaction between the molecule and the surface, with adsorption energies of 11.1 and 10.9 kJ mol(-1) for atop-h and atop-b, respectively. This weaker interaction leads to a geometry for the adsorbed molecule that is close to the gas-phase ethene structure, in agreement with the vibrational frequencies.

We have proposed a model of molecular adsorption that is a balance between attraction, resulting from localised bond formation, and repulsion, due to interaction between the: extended electronic states and the molecule's electron density. If the extended electronic states are underestimated, as in cluster or low k-point calculations, the repulsion is underestimated. This results in stronger bonding to the surface and overestimation of the adsorption energy. (C) 2000 Elsevier Science B.V. All rights reserved.

Original language | English |
---|---|

Pages (from-to) | 93-103 |

Number of pages | 11 |

Journal | Surface Science |

Volume | 459 |

Issue number | 1-2 |

Early online date | 23 Jun 2000 |

DOIs | |

Publication status | Published - 1 Jul 2000 |

### Keywords

- ab initio quantum chemical methods and calculations
- chemisorption
- copper
- density functional calculations
- single crystal surfaces
- wave basis-set
- molecular-dynamics
- psedopotentials
- hydrogenation
- transition
- catalysts
- ethylene
- CU(111)

### Cite this

*Surface Science*,

*459*(1-2), 93-103. https://doi.org/10.1016/S0039-6028(00)00444-1

**pi adsorption of ethene on to the {111} surface of copper : A periodic ab initio study of the effect of k-point sampling on the energy, atomic and electronic structure .** / Watson, G.W.; Wells, Richard Peter Kerwin; Willock, D J ; Hutchings, G J .

Research output: Contribution to journal › Article

*Surface Science*, vol. 459, no. 1-2, pp. 93-103. https://doi.org/10.1016/S0039-6028(00)00444-1

}

TY - JOUR

T1 - pi adsorption of ethene on to the {111} surface of copper

T2 - A periodic ab initio study of the effect of k-point sampling on the energy, atomic and electronic structure

AU - Watson, G.W.

AU - Wells, Richard Peter Kerwin

AU - Willock, D J

AU - Hutchings, G J

PY - 2000/7/1

Y1 - 2000/7/1

N2 - The adsorption of ethene on the (111) surface of copper has been studied by using density functional theory calculations with gradient corrections. The surface is described by a periodic (3 x 3) slab, three layers thick, with ethene adsorbed on one side. The energy of the adsorption shows great sensitivity to the k-point sampling employed, with single k-point calculations overestimating the binding by over 800% when compared with a calculation converged with respect to the k-point sampling. In addition, the structure of the adsorbed molecule is considerably distorted, which is in contradiction with conclusions drawn from the experimental vibrational frequencies.Calculations that are converged with respect to the k-point sampling indicate a much weaker interaction between the molecule and the surface, with adsorption energies of 11.1 and 10.9 kJ mol(-1) for atop-h and atop-b, respectively. This weaker interaction leads to a geometry for the adsorbed molecule that is close to the gas-phase ethene structure, in agreement with the vibrational frequencies.We have proposed a model of molecular adsorption that is a balance between attraction, resulting from localised bond formation, and repulsion, due to interaction between the: extended electronic states and the molecule's electron density. If the extended electronic states are underestimated, as in cluster or low k-point calculations, the repulsion is underestimated. This results in stronger bonding to the surface and overestimation of the adsorption energy. (C) 2000 Elsevier Science B.V. All rights reserved.

AB - The adsorption of ethene on the (111) surface of copper has been studied by using density functional theory calculations with gradient corrections. The surface is described by a periodic (3 x 3) slab, three layers thick, with ethene adsorbed on one side. The energy of the adsorption shows great sensitivity to the k-point sampling employed, with single k-point calculations overestimating the binding by over 800% when compared with a calculation converged with respect to the k-point sampling. In addition, the structure of the adsorbed molecule is considerably distorted, which is in contradiction with conclusions drawn from the experimental vibrational frequencies.Calculations that are converged with respect to the k-point sampling indicate a much weaker interaction between the molecule and the surface, with adsorption energies of 11.1 and 10.9 kJ mol(-1) for atop-h and atop-b, respectively. This weaker interaction leads to a geometry for the adsorbed molecule that is close to the gas-phase ethene structure, in agreement with the vibrational frequencies.We have proposed a model of molecular adsorption that is a balance between attraction, resulting from localised bond formation, and repulsion, due to interaction between the: extended electronic states and the molecule's electron density. If the extended electronic states are underestimated, as in cluster or low k-point calculations, the repulsion is underestimated. This results in stronger bonding to the surface and overestimation of the adsorption energy. (C) 2000 Elsevier Science B.V. All rights reserved.

KW - ab initio quantum chemical methods and calculations

KW - chemisorption

KW - copper

KW - density functional calculations

KW - single crystal surfaces

KW - wave basis-set

KW - molecular-dynamics

KW - psedopotentials

KW - hydrogenation

KW - transition

KW - catalysts

KW - ethylene

KW - CU(111)

U2 - 10.1016/S0039-6028(00)00444-1

DO - 10.1016/S0039-6028(00)00444-1

M3 - Article

VL - 459

SP - 93

EP - 103

JO - Surface Science

JF - Surface Science

SN - 0039-6028

IS - 1-2

ER -