2016
DOI: 10.1007/s00214-015-1778-4
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Describing excited states of [n]cycloparaphenylenes by hybrid and double-hybrid density functionals: from isolated to weakly interacting molecules

Abstract: We theoretically study the excited-state properties of Cycloparaphenylenes ([n]CPPs) for a deeper understanding of their photochemical properties with increasing size n, being n = 6 − 12 the number of repeat units forming the nanoring. We apply hybrid (e.g. PBE0and PBE0-1/3), double-hybrid (e.g. PBE0-DH and PBE-QIDH) and range-separated (e.g. ωB97X) functionals within a Time-Dependent

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Cited by 17 publications
(15 citation statements)
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References 93 publications
(71 reference statements)
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“…It can be immediately seen how for the neutral N‐doped nanohoops 1 ‐ 3 a major absorbance peak is also observed around 340350 nm, slightly red‐shifted on increasing the content of N in perfect agreement with experimental results . Note that contrarily to what was found before for the unsubstituted [8]CPP for these N‐doped [8]CPPs, the HOMO‐LUMO transition is not forbidden due to partial symmetry breaking induced by the presence of nitrogen, although the oscillator strength values are very low. Actually, for both [8]CPP and neutral N‐doped nanohoops 1 ‐ 3 , the transition ( πnormalπ) giving rise to the absorption maximum is composed of approximately equal combinations of one‐electron excitations from HOMO‐1 to LUMO and HOMO to LUMO + 1, and from HOMO‐2 to LUMO and HOMO to LUMO + 2.…”
Section: Resultssupporting
confidence: 87%
See 1 more Smart Citation
“…It can be immediately seen how for the neutral N‐doped nanohoops 1 ‐ 3 a major absorbance peak is also observed around 340350 nm, slightly red‐shifted on increasing the content of N in perfect agreement with experimental results . Note that contrarily to what was found before for the unsubstituted [8]CPP for these N‐doped [8]CPPs, the HOMO‐LUMO transition is not forbidden due to partial symmetry breaking induced by the presence of nitrogen, although the oscillator strength values are very low. Actually, for both [8]CPP and neutral N‐doped nanohoops 1 ‐ 3 , the transition ( πnormalπ) giving rise to the absorption maximum is composed of approximately equal combinations of one‐electron excitations from HOMO‐1 to LUMO and HOMO to LUMO + 1, and from HOMO‐2 to LUMO and HOMO to LUMO + 2.…”
Section: Resultssupporting
confidence: 87%
“…The M06‐2X and ωB97XD methods behave similarly, especially for the 1,15‐diaza‐[8]CPP 2 and N , N ‐dimethyl‐1,15‐diaza‐[8]CPP 2+ 8 cases, while B3LYP‐D3(BJ) lies between M06‐L and M06‐2X, following the increasing weight of the HF‐like exchange introduced into the method . We also note that the ωB97XD method had been shown previously to overestimate systematically the experimental absorption maxima for the set of increasingly longer [ 612]CPPs, and we will, thus, rely in the following in the B3LYP‐D3(BJ) optimized geometries as a compromise. We calculate with this method a diameter of 11.0±0.5 Å for molecule 1 , to be compared with an experimental (X‐ray) value of 10.9±0.2 Å, [31] and that the precise location of the N atom could not be experimentally resolved, which precludes a more detailed comparison between experimental and theoretical results for individual bond lengths.…”
Section: Resultsmentioning
confidence: 54%
“…The idea of DH scheme can be traced back to the work of Ernzerhof which used by Zhao et al through the multi‐coefficient methods and finally popularized by Grimme, the author of the B2‐PLYP model. In recent years, a large number of DHs with variety of density functional approximations (DFAs) has been proposed and validated on different properties . We refer the interested reader to the recent review articles in the field of DH‐DFT …”
Section: Theoretical and Methodological Frameworkmentioning
confidence: 99%
“…[ 281 ] This issue has also been investigated for selected 6CPP dimers representing the crystalline packing. [ 282 ] Depending on the relative orientation and distance between the monomers of these weakly interacting dimers, the excited‐state energies of isolated molecules (Ω) are splitted into normalΩ=Ω±β, with β the resonance energy given by the coupling between the ground‐state (CPP) and excited‐state (CPP ⋆ ) wavefunctions normalΨnormalCPPnormalΨCPP|V̂|normalΨCPPnormalΨnormalCPP, with the results driven by long‐range interactions and differing for each excited state. Traditionally, single‐reference methods, such as TD‐DFT, can not describe the effects giving rise to this kind of excited‐states [ 283,284 ] and this has motivated the use of more advanced methods or corrections to standard TD‐DFT.…”
Section: Optical and Photophysical Propertiesmentioning
confidence: 99%