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 inJournal of physical chemistry. C Vol. 117; no. 5; pp. 2160 - 2165
Main Authors Carro, P, Pensa, E, Vericat, C, Salvarezza, R. C
Format Journal Article
LanguageEnglish
Published 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).
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
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  givenname: R. C
  surname: Salvarezza
  fullname: Salvarezza, R. C
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Issue 5
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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Snippet A detailed density functional calculation (DFT) study including van der Waals (vdW) dispersion forces of different adatom-containing models (RS–Auad–SR) at...
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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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