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Electron transport in open systems from finite-size calculations: Examination of the principal layer method applied to linear gold chains
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10.1063/1.2905219
/content/aip/journal/jcp/128/15/10.1063/1.2905219
http://aip.metastore.ingenta.com/content/aip/journal/jcp/128/15/10.1063/1.2905219

Figures

Image of FIG. 1.
FIG. 1.

Typical input structure for the quantum chemical code of a gold chain where a gap is introduced.

Image of FIG. 2.
FIG. 2.

Conductance of gold chain, dotted-dashed line denotes Fermi energy. (a) Bulk calculation for different principal layer sizes, LANL2DZ-nw basis set. (b) Conductor calculation for different gap sizes in atomic distances (ad), principal layer size six atoms, LANL2DZ-nw basis set. (c) Conductor calculation for different gap sizes in atomic distances (ad), principal layer size six atoms, LANL2DZ-cry basis set.

Image of FIG. 3.
FIG. 3.

Band structure of a gold chain, the Fermi level is indicated by a dashed-dotted line. (a) Periodic CRYSTAL calculation, six atoms in unit cell, LANL2DZ-nw. (b) Principal layer method, six atoms in principal layer, LANL2DZ-nw; arrows mark unphysical band. (c) Principal layer method, six atoms in principal layer, LANL2DZ-cry. For transport-based calculations, the bands are represented by dots on the energy grid. This is due to the fact that in that case the bands are expressed as rather than since is an input parameter of the Green’s function approach. It follows that some bands might look dotted when the band is flat since step sizes in energy are finite.

Image of FIG. 4.
FIG. 4.

Hamiltonian projected onto the basis function along a 24 atom gold chain, finite-size NWCHEM calculation: Upper panel LANL2DZ-nw and lower panel LANL2DZ-cry. The inset panels enlarge the scale for the Hamiltonian elements along atoms 7–18a. (a) Principal layer approximation by replicating values from atoms 7–12 for atoms 13–18. (b) Hamiltonian elements from NWCHEM calculation. (c) Hamiltonian elements from CRYSTAL calculation.

Tables

Generic image for table
Table I.

Largest absolute values of the NWCHEM Hamiltonian in a.u. and overlap matrix elements between the next nearest neighbors for different principal layer sizes and basis sets.

Generic image for table
Table II.

Largest absolute values of the differences between the NWCHEM Hamiltonian elements in a.u. of a principal layer and its neighbor and potential differences at layer transition in a.u. measured as the absolute value of the difference between the NWCHEM Hamiltonian projected onto the function of the first and the last atom in the principal layer for different principal layer sizes, buffer sizes, and basis sets.

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/content/aip/journal/jcp/128/15/10.1063/1.2905219
2008-04-18
2014-04-25
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Electron transport in open systems from finite-size calculations: Examination of the principal layer method applied to linear gold chains
http://aip.metastore.ingenta.com/content/aip/journal/jcp/128/15/10.1063/1.2905219
10.1063/1.2905219
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