2026-06-29T02:37:55Zhttps://docta.ucm.es/rest/oai/request
oai:docta.ucm.es:20.500.14352/942912024-07-16T00:03:07Zcom_20.500.14352_14col_20.500.14352_15
Docta Complutense author Rodríguez, Javier author González, Marta author Rubio-Lago, Luis author Bañares Morcillo, Luis 2024-01-22T10:32:31Z 2024-01-22T10:32:31Z 2014 1463-9076 10.1039/c3cp54362e https://hdl.handle.net/20.500.14352/94291 1463-9084 https://doi.org/10.1039/c3cp54362e The photodynamics of phenol–ammonia clusters, PhOH(NH3)3–5, after one UV photon absorption, has been investigated using velocity map imaging of the NH4(NH3)2–4 cluster products. The dependence of the NH4(NH3)2 translational energy distributions on the available energy reveals three dynamical regions in close correspondence with the photodissociation of bare phenol. At low excitation energies (between 282 and 260 nm), the NH4(NH3)2 distribution mirrors the hydrogen-atom passage through the 11 pp*–11 ps* barrier, constituting the first evidence of hydrogen-atom tunneling dynamics in an excited state hydrogen transfer (ESHT) reaction. At excitation wavelengths below 260 nm, the product distributions are consistent with two separate barrierless dissociation processes associated, respectively, with excitation to the 11 pp* and 21 pp* excited electronic states. Similar conclusions can be derived from the velocity map imaging results on the larger NH4(NH3)3,4 cluster products. eng Attribution-NoDerivatives 4.0 International Direct evidence of hydrogen-atom tunneling dynamics in the excited state hydrogen transfer (ESHT) reaction of phenol–ammonia clusters journal article 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 URL https://docta.ucm.es/bitstreams/d528b114-7f53-4ca1-b47a-70626e853fbd/download File MD5 095c619307f4cb36f1ef86c048cc7e27 2052878 application/pdf Hydrogen-atom_tunneling_dynamics.pdf