2003
DOI: 10.1021/jp0301913
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Time-Dependent Density Functional Study of the Electronic Excited States of Polycyclic Aromatic Hydrocarbon Radical Ions

Abstract: A uniform, comprehensive theoretical interpretation of spectroscopic data is presented for 51 radical ion species of polycyclic aromatic hydrocarbons (PAHs) with the aid of (Tamm−Dancoff) time-dependent density functional theory (TDDFT). TDDFT is capable of predicting the transition energies to the low-lying excited states of PAH ions with quantitative accuracy (the standard deviation from experimental results being less than 0.3 eV) and their intensity patterns qualitatively correctly. The accuracy is hardly … Show more

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Cited by 102 publications
(132 citation statements)
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References 72 publications
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“…This includes the broad absorption peak dominated by σ * ← σ transitions, which matches well both in position and width. Concerning the low-lying excited states of π * ← π character occurring in the near-IR, visible, and near-UV spectral ranges, the computed vertical excitation energies are precise to within a few tenths of eV (in the range 0.1−0.4 eV), which are indeed the typical accuracies achievable by TD-DFT using hybrid or gradient-corrected exchange-correlation functionals (Hirata et al 1999(Hirata et al , 2003. We proved these data to be reliable enough for detailed modelling of PAHs in different charge states when laboratory data are missing (Mulas et al 2006a,b,c).…”
Section: ++supporting
confidence: 57%
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“…This includes the broad absorption peak dominated by σ * ← σ transitions, which matches well both in position and width. Concerning the low-lying excited states of π * ← π character occurring in the near-IR, visible, and near-UV spectral ranges, the computed vertical excitation energies are precise to within a few tenths of eV (in the range 0.1−0.4 eV), which are indeed the typical accuracies achievable by TD-DFT using hybrid or gradient-corrected exchange-correlation functionals (Hirata et al 1999(Hirata et al , 2003. We proved these data to be reliable enough for detailed modelling of PAHs in different charge states when laboratory data are missing (Mulas et al 2006a,b,c).…”
Section: ++supporting
confidence: 57%
“…Hybrid DFT functionals are a little more expensive than other exchange-correlation functionals but yield better results. The B3LYP functional, in particular, is widely used in the study of PAHs and related species (Martin et al 1996;Langhoff 1996;Wiberg 1997;Bauschlicher & Langhoff 1997;Kato et al 1999;Kato & Yamabe 2002;Dessent 2000;Bauschlicher & Bakes 2000Schröder et al 2001;Rienstra-Kiracofe et al 2001;Bauschlicher 2002;Hirata et al 2003;Deleuze et al 2003;Rosi et al 2004;Woon & Park 2004;Jolibois et al 2005;Witt et al 2006;Kadantsev et al 2006). To assess the impact of this choice we also considered some more recently developed functionals, such as the so-called B−97 (Becke 1997) and HCTH (Hamprecht et al 1998), but no significant improvements, if any, were obtained with respect to B3LYP for calculating the ionisation energies of PAHs.…”
Section: Ionisation Energies and Vibrational Propertiesmentioning
confidence: 99%
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“…A range separated density functional, ωB97 (Chai & Head-Gordon 2008), that is specifically designed for weak interactions was also employed. For valence electronic transitions TDDFT has been shown to work well (Hirata et al 1999;Weisman et al 2001;Halasinski et al 2003;Hirata et al 2003). The range-separated functional, ωB97, significantly reduces the serious problems of TDDFT with conventional functionals for charge-transfer excited states (Dreuw & Head-Gordon 2004).…”
Section: Theoretical Methodsmentioning
confidence: 99%
“…4 Here we have used a wider range of basis sets, including the cc-pVDZ and cc-pVTZ basis sets for water and 6-31G, cc-pVDZ, and cc-pVTZ basis sets for nitrogen. 34,35 For assessment, we carried out calculations with state-of-the-art internally contracted multireference methods-second-and third-order perturbation theory ͑CASPT2 and CASPT3͒, [36][37][38][39] configuration interaction ͑MR-CI͒, 40-42 the a posteriori size-extensivity corrected configuration interaction due to Davidson ͑MR-CI+ Q͒, 43,44 averaged coupled pair functional ͑MR-ACPF͒, 45,46 and averaged quadratic coupled cluster theory 47 ͑MR-AQCC͒ ͑both a priori size-extensivity modifications of configuration interaction͒, as well as single-reference coupled cluster calculations at the CCSD and CCSDT level 48,49 ͒. Full configuration interaction ͑FCI͒ energies were also used for comparison where available.…”
Section: Calculations a Water And Nitrogen Potential Energy Curvesmentioning
confidence: 99%