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Exploring quantum interference in heteroatom-substituted graphene-like molecules

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Exploring quantum interference in heteroatom-substituted graphene-like molecules. / Sangtarash, Sara; Sadeghi, Hatef; Lambert, Colin.
In: Nanoscale, Vol. 2016, No. 27, 8, 21.07.2016, p. 13199-13205.

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Sangtarash S, Sadeghi H, Lambert C. Exploring quantum interference in heteroatom-substituted graphene-like molecules. Nanoscale. 2016 Jul 21;2016(27):13199-13205. 8. Epub 2016 Jun 16. doi: 10.1039/C6NR01907B

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Sangtarash, Sara ; Sadeghi, Hatef ; Lambert, Colin. / Exploring quantum interference in heteroatom-substituted graphene-like molecules. In: Nanoscale. 2016 ; Vol. 2016, No. 27. pp. 13199-13205.

Bibtex

@article{c511d667924c453b9f090b9eca6c47a5,
title = "Exploring quantum interference in heteroatom-substituted graphene-like molecules",
abstract = "If design principles for controlling quantum interference in single molecules could be elucidated and verified, then this will lay the foundations for exploiting such effects in nanoscale devices and thin-film materials. When the core of a graphene-like polyaromatic hydrocarbon (PAH) is weakly coupled to external electrodes by atoms i and j, the single-molecule electrical conductance σ_ij depends on the choice of connecting atoms i, j. Furthermore, provided the Fermi energy is located between the HOMO and LUMO, conductance ratios σ_ij/σ_lm corresponding to different connectivities i, j and l,m are determined by quantum interference within the PAH core. In this paper, we examine how such conductance ratios change when one of the carbon atoms within the {\textquoteleft}parent{\textquoteright} PAH core is replaced by a heteroatom to yield a {\textquoteleft}daughter{\textquoteright} molecule. For bipartite parental cores, in which odd-numbered sites are connected to even-numbered sites only, the effect of heteroatom substitution onto an odd-numbered site is summarized by the following qualitative rules: (a) When i and j are odd, both parent and daughter have low conductances, (b) When i is odd and j is even, or vice versa both parent and daughter have high conductances and (c) When i,j are both even, the parent has a low conductance and the daughter a high conductance. These rules are verified by comparison with density-functional calculations on naphthalene, anthracene, pyrene and anthanthrene cores connected via two different anchor groups to gold electrodes.",
author = "Sara Sangtarash and Hatef Sadeghi and Colin Lambert",
note = "{\textcopyright} Royal Society of Chemistry 2016.",
year = "2016",
month = jul,
day = "21",
doi = "10.1039/C6NR01907B",
language = "English",
volume = "2016",
pages = "13199--13205",
journal = "Nanoscale",
issn = "2040-3364",
publisher = "Royal Society of Chemistry",
number = "27",

}

RIS

TY - JOUR

T1 - Exploring quantum interference in heteroatom-substituted graphene-like molecules

AU - Sangtarash, Sara

AU - Sadeghi, Hatef

AU - Lambert, Colin

N1 - © Royal Society of Chemistry 2016.

PY - 2016/7/21

Y1 - 2016/7/21

N2 - If design principles for controlling quantum interference in single molecules could be elucidated and verified, then this will lay the foundations for exploiting such effects in nanoscale devices and thin-film materials. When the core of a graphene-like polyaromatic hydrocarbon (PAH) is weakly coupled to external electrodes by atoms i and j, the single-molecule electrical conductance σ_ij depends on the choice of connecting atoms i, j. Furthermore, provided the Fermi energy is located between the HOMO and LUMO, conductance ratios σ_ij/σ_lm corresponding to different connectivities i, j and l,m are determined by quantum interference within the PAH core. In this paper, we examine how such conductance ratios change when one of the carbon atoms within the ‘parent’ PAH core is replaced by a heteroatom to yield a ‘daughter’ molecule. For bipartite parental cores, in which odd-numbered sites are connected to even-numbered sites only, the effect of heteroatom substitution onto an odd-numbered site is summarized by the following qualitative rules: (a) When i and j are odd, both parent and daughter have low conductances, (b) When i is odd and j is even, or vice versa both parent and daughter have high conductances and (c) When i,j are both even, the parent has a low conductance and the daughter a high conductance. These rules are verified by comparison with density-functional calculations on naphthalene, anthracene, pyrene and anthanthrene cores connected via two different anchor groups to gold electrodes.

AB - If design principles for controlling quantum interference in single molecules could be elucidated and verified, then this will lay the foundations for exploiting such effects in nanoscale devices and thin-film materials. When the core of a graphene-like polyaromatic hydrocarbon (PAH) is weakly coupled to external electrodes by atoms i and j, the single-molecule electrical conductance σ_ij depends on the choice of connecting atoms i, j. Furthermore, provided the Fermi energy is located between the HOMO and LUMO, conductance ratios σ_ij/σ_lm corresponding to different connectivities i, j and l,m are determined by quantum interference within the PAH core. In this paper, we examine how such conductance ratios change when one of the carbon atoms within the ‘parent’ PAH core is replaced by a heteroatom to yield a ‘daughter’ molecule. For bipartite parental cores, in which odd-numbered sites are connected to even-numbered sites only, the effect of heteroatom substitution onto an odd-numbered site is summarized by the following qualitative rules: (a) When i and j are odd, both parent and daughter have low conductances, (b) When i is odd and j is even, or vice versa both parent and daughter have high conductances and (c) When i,j are both even, the parent has a low conductance and the daughter a high conductance. These rules are verified by comparison with density-functional calculations on naphthalene, anthracene, pyrene and anthanthrene cores connected via two different anchor groups to gold electrodes.

U2 - 10.1039/C6NR01907B

DO - 10.1039/C6NR01907B

M3 - Journal article

VL - 2016

SP - 13199

EP - 13205

JO - Nanoscale

JF - Nanoscale

SN - 2040-3364

IS - 27

M1 - 8

ER -