Fully quantal description of combined internal conversion and intersystem crossing processes in the smallest Criegee intermediate CH2OO
A quantal description of nuclear motion using coupled fifteen-state potential energy and spin-orbit coupling surfaces for studying the photodissociation of CH2OO to H2CO(X1A1) + O1D and H2CO(X1A1) + O3P channels is presented. For the evaluation of surfaces, multireference electronic wave functions a...
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| Hauptverfasser: | , |
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| Dokumenttyp: | Article (Journal) |
| Sprache: | Englisch |
| Veröffentlicht: |
27 Aug 2024
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| In: |
Physical chemistry, chemical physics
Year: 2024, Jahrgang: 26, Heft: 37, Pages: 24591-24606 |
| ISSN: | 1463-9084 |
| DOI: | 10.1039/D4CP02122C |
| Online-Zugang: | Verlag, kostenfrei, Volltext: https://doi.org/10.1039/D4CP02122C Verlag, kostenfrei, Volltext: https://pubs.rsc.org/en/content/articlelanding/2024/cp/d4cp02122c 
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| Verfasserangaben: | Behnam Nikoobakht and Horst Köppel |
| Zusammenfassung: | A quantal description of nuclear motion using coupled fifteen-state potential energy and spin-orbit coupling surfaces for studying the photodissociation of CH2OO to H2CO(X1A1) + O1D and H2CO(X1A1) + O3P channels is presented. For the evaluation of surfaces, multireference electronic wave functions are employed. For the fully quantal description of the nuclear motion, we diabatize the PESs of the two and four lowest excited singlet and triplet states, respectively, within the three sets of vibronically coupled states, i.e. (B1A′, C1A′), (a3A′, b3A′) and (a3A′′, b3A′′), employing the diabatization by ansatz method. This yields three different adiabatic-to-diabatic mixing angles, which are used for the diabatization of the spin-orbit coupling surfaces and allow to investigate simultaneously the internal conversion and intersystem crossing processes in CH2OO using a nuclear quantum dynamical approach for the first time. Our calculation predicts the presence of a weak spectral band with irregular and discrete structures, which originates from the role of spin-orbit couplings. This band of the spectrum is mainly located between the minimum energy of the a3A′ state and the onset of the B1A′ ← X1A′ spectral band. Furthermore, sizable SOC between the B1A′ and a3A′′ states mixes them via intersystem crossing. Due to the vibronic interaction between the a3A′′ and a3A′ states, the molecule finally relaxes to the a3A′ state and is dissociated to H2CO(X1A1) and O3P products. |
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| Beschreibung: | Gesehen am 13.02.2025 |
| Beschreibung: | Online Resource |
| ISSN: | 1463-9084 |
| DOI: | 10.1039/D4CP02122C |