2005
DOI: 10.1103/physrevb.71.033201
|View full text |Cite
|
Sign up to set email alerts
|

Exciton sizes of conducting polymers predicted by time-dependent density functional theory

Abstract: The electronic structure and size scaling of spectroscopic observables in conjugated polymers are investigated using time-dependent density functional theory. We show that local density approximations and gradientcorrected functionals do not have an effective attractive Coulomb interaction between photoexcited electronhole pairs to form bound states and therefore do not reproduce finite exciton sizes. Long-range nonlocal and nonadiabatic density functional corrections ͑such as hybrid mixing with an exact Hartr… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1

Citation Types

3
197
0

Year Published

2005
2005
2017
2017

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 205 publications
(200 citation statements)
references
References 30 publications
3
197
0
Order By: Relevance
“…This positive correlation can be understood as the onset of exciton binding. This result sheds new light on the observations by Tretiak et al 39 that bound excitons in large conjugated systems can only be described by LRC functionals.…”
mentioning
confidence: 74%
“…This positive correlation can be understood as the onset of exciton binding. This result sheds new light on the observations by Tretiak et al 39 that bound excitons in large conjugated systems can only be described by LRC functionals.…”
mentioning
confidence: 74%
“…In Fig 1, we plot is a strong function of the exact orbital-dependent exchange (Fock-like exchange) present in the functional [35]. For example, the ZINDO (100% of exact-exchange) curve saturates faster to the constant long-chain-limit than B3LYP (20% of exact-exchange) results.…”
Section: Resultsmentioning
confidence: 99%
“…During excited-state geometry optimization the bonds along the conjugated backbone stretch, so that the bond-length alternation caused by uneven distribution of π-electronic density reduces. 28 This allows the electrons to become more delocalized, and the excited-state energy is reduced. The magnitude of the observed Stokes shift and the respective geometry changes intensify with an increase of the fraction of exchange.…”
Section: Resultsmentioning
confidence: 99%
“…With the most commonly used approximate kernels, such as LDA and GGA models, many bound exciton states are not described at all. 27,28 This is because the kernal is local and the orbital overlap is negligible. This problem is further complicated by the neglect of an important derivative discontinuity in most functionals.…”
Section: Introductionmentioning
confidence: 99%