Hydrocarbon Chain Length Induces Surface Structure Transitions in Alkanethiolate–Gold Adatom Self-Assembled Monolayers on Au(111)
A detailed density functional calculation (DFT) study including van der Waals (vdW) dispersion forces of different adatom-containing models (RS–Auad–SR) at saturation coverage for methanethiol (MT), butanethiol (BT), and hexanethiol (HT) on Au(111) is presented. The stability analysis of these latti...
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Published in | Journal of physical chemistry. C Vol. 117; no. 5; pp. 2160 - 2165 |
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Main Authors | , , , |
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Language | English |
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Columbus, OH
American Chemical Society
07.02.2013
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Abstract | A detailed density functional calculation (DFT) study including van der Waals (vdW) dispersion forces of different adatom-containing models (RS–Auad–SR) at saturation coverage for methanethiol (MT), butanethiol (BT), and hexanethiol (HT) on Au(111) is presented. The stability analysis of these lattices shows a transition from the (3 × 4) to the c(4 × 2) surface structure when the number of C atoms in the alkanethiol chain is larger than 2, fairly predicting recent experimental observations for these systems. The transition takes place when the smaller energy needed to reconstruct the Au(111) surface and the larger binding energy for MT in the (3 × 4) MT lattice is compensated by a larger interaction energy between hydrocarbon chains in the c(4 × 2) lattice for BT and HT. Our calculations therefore explain why the (3 × 4) lattice is more stable for MT and ethanethiol (ET) while the c(4 × 2) lattice predominates for longer alkanethiols, thus shedding light on the behavior of alkanethiol self-assembled monolayers (SAMs) on Au(111). |
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AbstractList | A detailed density functional calculation (DFT) study including van der Waals (vdW) dispersion forces of different adatom-containing models (RS–Auad–SR) at saturation coverage for methanethiol (MT), butanethiol (BT), and hexanethiol (HT) on Au(111) is presented. The stability analysis of these lattices shows a transition from the (3 × 4) to the c(4 × 2) surface structure when the number of C atoms in the alkanethiol chain is larger than 2, fairly predicting recent experimental observations for these systems. The transition takes place when the smaller energy needed to reconstruct the Au(111) surface and the larger binding energy for MT in the (3 × 4) MT lattice is compensated by a larger interaction energy between hydrocarbon chains in the c(4 × 2) lattice for BT and HT. Our calculations therefore explain why the (3 × 4) lattice is more stable for MT and ethanethiol (ET) while the c(4 × 2) lattice predominates for longer alkanethiols, thus shedding light on the behavior of alkanethiol self-assembled monolayers (SAMs) on Au(111). |
Author | Pensa, E Vericat, C Salvarezza, R. C Carro, P |
AuthorAffiliation | Universidad de La Laguna Universidad Nacional de La Plata |
AuthorAffiliation_xml | – name: Universidad Nacional de La Plata – name: Universidad de La Laguna |
Author_xml | – sequence: 1 givenname: P surname: Carro fullname: Carro, P email: pcarro@ull.es – sequence: 2 givenname: E surname: Pensa fullname: Pensa, E – sequence: 3 givenname: C surname: Vericat fullname: Vericat, C – sequence: 4 givenname: R. C surname: Salvarezza fullname: Salvarezza, R. C |
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Keywords | Gold Binding energy Chain length Atomic chain Hydrocarbons Density functional method Adatoms Alkanethiol Self-assembled layers Coverage rate Surface phase transformations Surface structure |
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SubjectTerms | Condensed matter: structure, mechanical and thermal properties Exact sciences and technology Phase transitions and critical phenomena Physics Solid surfaces and solid-solid interfaces Surface structure and topography Surfaces and interfaces; thin films and whiskers (structure and nonelectronic properties) |
Title | Hydrocarbon Chain Length Induces Surface Structure Transitions in Alkanethiolate–Gold Adatom Self-Assembled Monolayers on Au(111) |
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