Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.

We introduce a mapping from configuration interaction singles wavefunctions, expressed as linear combinations of particle-hole excitations between Hartree-Fock molecular orbitals, to real-space exciton wavefunctions, expressed as linear combinations of particle-hole excitations between localized Wan...

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Váldodahkkit: Barford, W, Paiboonvorachat, N
Materiálatiipa: Journal article
Giella:English
Almmustuhtton: 2008
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author Barford, W
Paiboonvorachat, N
author_facet Barford, W
Paiboonvorachat, N
author_sort Barford, W
collection OXFORD
description We introduce a mapping from configuration interaction singles wavefunctions, expressed as linear combinations of particle-hole excitations between Hartree-Fock molecular orbitals, to real-space exciton wavefunctions, expressed as linear combinations of particle-hole excitations between localized Wannier functions. The exciton wavefunction is a two-dimensional amplitude for the exciton center-of-mass coordinate, R, and the electron-hole separation (or relative coordinate), r, having an exact analogy to one-dimensional hydrogenlike wavefunctions. We describe the excitons by their appropriate quantum numbers, namely, the principle quantum number, n, associated with r and the center-of-mass pseudomomentum quantum number, j, associated with R. In addition, for models with particle-hole symmetry, such as the Pariser-Parr-Pople model, we emphasize the connection between particle-hole symmetry and particle-hole parity. The method is applied to the study of excitons in trans-polyacetylene and poly(para-phenylene).
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spelling oxford-uuid:e89126e2-52b9-4185-8e4b-ffac8e35c9ac2022-03-27T10:47:48ZExcitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.Journal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:e89126e2-52b9-4185-8e4b-ffac8e35c9acEnglishSymplectic Elements at Oxford2008Barford, WPaiboonvorachat, NWe introduce a mapping from configuration interaction singles wavefunctions, expressed as linear combinations of particle-hole excitations between Hartree-Fock molecular orbitals, to real-space exciton wavefunctions, expressed as linear combinations of particle-hole excitations between localized Wannier functions. The exciton wavefunction is a two-dimensional amplitude for the exciton center-of-mass coordinate, R, and the electron-hole separation (or relative coordinate), r, having an exact analogy to one-dimensional hydrogenlike wavefunctions. We describe the excitons by their appropriate quantum numbers, namely, the principle quantum number, n, associated with r and the center-of-mass pseudomomentum quantum number, j, associated with R. In addition, for models with particle-hole symmetry, such as the Pariser-Parr-Pople model, we emphasize the connection between particle-hole symmetry and particle-hole parity. The method is applied to the study of excitons in trans-polyacetylene and poly(para-phenylene).
spellingShingle Barford, W
Paiboonvorachat, N
Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title_full Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title_fullStr Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title_full_unstemmed Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title_short Excitons in conjugated polymers: wavefunctions, symmetries, and quantum numbers.
title_sort excitons in conjugated polymers wavefunctions symmetries and quantum numbers
work_keys_str_mv AT barfordw excitonsinconjugatedpolymerswavefunctionssymmetriesandquantumnumbers
AT paiboonvorachatn excitonsinconjugatedpolymerswavefunctionssymmetriesandquantumnumbers