2015
DOI: 10.1063/1.4908560
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Counting the number of excited states in organic semiconductor systems using topology

Abstract: Exciton Scattering (ES) theory attributes excited electronic states to standing waves in quasione-dimensional molecular materials by assuming a quasi-particle picture of optical excitations. The quasi-particle properties at branching centers are described by the corresponding scattering matrices. Here we identify the topological invariant of a scattering center, referred to as its winding number, and apply topological intersection theory to count the number of quantum states in a quasi-one-dimensional system.

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Cited by 3 publications
(2 citation statements)
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“…The tight-binding models can be build in an efficient way by studying the the topological properties of the scattering matrices, namely the integer-valued topological charge, or equivalently winding number associated with the corresponding scattering matrix [48]. The topological charge provides useful information on how many cites in the related tight-binding model are needed to adequately describe a scattering center.…”
Section: Discussionmentioning
confidence: 99%
“…The tight-binding models can be build in an efficient way by studying the the topological properties of the scattering matrices, namely the integer-valued topological charge, or equivalently winding number associated with the corresponding scattering matrix [48]. The topological charge provides useful information on how many cites in the related tight-binding model are needed to adequately describe a scattering center.…”
Section: Discussionmentioning
confidence: 99%
“…Previously we have characterized how a molecular vertex affects the number of excitonic states in a molecule in terms of the analytical and topological properties of the ES matrix. 28,29,36 In the case of PA bond-length alternation, the topological charge Q T = (w(Γ) − 1)/2 = 0 has been found due to w(ϕ 0 ) = w(ϕ 1 ) = 1, where the winding number w describes how many times the scattering amplitude e iϕ(k) winds over the unit circle it resides on, while the quasimomentum k goes once over the Brillouin zone. In addition, a bound state localized in the vicinity of the stretched CC has been observed in the structures with triple-bond length change >3% or has been expected in sufficiently long molecules with moderately stretched (≤3%) triple bond.…”
mentioning
confidence: 99%