2019
DOI: 10.1039/c8cp07189f
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Ultrafast and radiationless electronic excited state decay of uracil and thymine cations: computing the effects of dynamic electron correlation

Abstract: In this article we characterise the radiationless decay of the first few electronic excited states of the cations of DNA/RNA nucleobases uracil and thymine, including the effects of dynamic electron correlation on energies and geometries (optimised with XMS-CASPT2).

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Cited by 22 publications
(77 citation statements)
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“…Whilst D 0 and D 1 vertical ionisation and D 0 adiabatic CASPT2 averaged values fall within the registered experimental data, larger differences of ∼0.3 and ∼0.4 eV are found for D 2 and D 3 , respectively. Similar to what we have found in recent works on cationic uracil and thymine, the use of the IPEA shift blue‐shifts the estimates by ∼0.2 eV and overestimates the experimental data when used in conjunction with multistate CASPT2 variants (either MS or XMS), as these already feature ionisation energies closer to the experimental range within IPEA=0.0 a.u.…”
Section: Resultssupporting
confidence: 85%
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“…Whilst D 0 and D 1 vertical ionisation and D 0 adiabatic CASPT2 averaged values fall within the registered experimental data, larger differences of ∼0.3 and ∼0.4 eV are found for D 2 and D 3 , respectively. Similar to what we have found in recent works on cationic uracil and thymine, the use of the IPEA shift blue‐shifts the estimates by ∼0.2 eV and overestimates the experimental data when used in conjunction with multistate CASPT2 variants (either MS or XMS), as these already feature ionisation energies closer to the experimental range within IPEA=0.0 a.u.…”
Section: Resultssupporting
confidence: 85%
“…A small energy gap can be observed at the CASSCF level at the effective 3‐state degeneracy, displaying a well‐separated D 1 state at the (D3/D2)CI . Dynamic electron correlation therefore has the opposite effect in cytosine from that previously reported in uracil, helping to bring the electronic states together and effectively promoting a 3‐state degeneracy instead of splitting the energy levels and disrupting this crossing. Significant differences are also observed when comparing the energy of the D3(2nN+) state at the FC and (D3/D2)CI geometries, showing a 0.40 eV stabilisation at CASSCF and a more pronounced 1.06 eV at the XMS‐CASPT2 level, which appears to be correlated to the overall bond length shortenings observed with the latter level of theory.…”
Section: Resultsmentioning
confidence: 71%
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