2019
DOI: 10.1021/acs.jpca.8b11216
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Computational Study on the Photolysis of BrHgONO and the Reactions of BrHgO with CH4, C2H6, NO, and NO2: Implications for Formation of Hg(II) Compounds in the Atmosphere

Abstract: Global models suggest BrHgONO to be the major Hg­(II) species initially formed in atmospheric oxidation of Hg(0) in most of the atmosphere, but its atmospheric fate has not been previously investigated. In the present work, we use quantum chemistry to predict that BrHgONO photolysis produces the thermally stable radical BrHgO•. Subsequently, BrHgO• may react with NO2 to form thermally stable BrHgONO2, or with NO to re-form BrHgONO. Additionally, BrHgO• abstracts hydrogen atoms from CH4 and C2H6 with higher rat… Show more

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Cited by 33 publications
(91 citation statements)
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“…For syn ‐HgBrONO, two types of transitions of distinct nature result in the population of S 1 ; i) a mainly monoconfigurational transition in which the electron excitation is localized in the ONO part of the molecule, the electronic density redistribution takes place from an in‐plane oxygen lone pair orbital of the N=O moiety to the antibonding π* orbital (see the violet box in Figure a), and ii) a multiconfigurational transition described mainly by the excitation of type (i) plus a second excitation in which now the electron departs from an orbital with contributions also from the Hg and Br atoms (delocalized orbital) to the same π* orbital (see the pink box in Figure a). While type (i) occurs at the Franck–Condon geometry (band maximum), type (ii) appears in other surrounding geometries and contributes to the increase in the intensity of the S 1 band. Type (ii) contributions, from excitations of the HgBr part of the molecule, shall affect the photodynamics of the system, as shown below.…”
Section: Resultssupporting
confidence: 89%
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“…For syn ‐HgBrONO, two types of transitions of distinct nature result in the population of S 1 ; i) a mainly monoconfigurational transition in which the electron excitation is localized in the ONO part of the molecule, the electronic density redistribution takes place from an in‐plane oxygen lone pair orbital of the N=O moiety to the antibonding π* orbital (see the violet box in Figure a), and ii) a multiconfigurational transition described mainly by the excitation of type (i) plus a second excitation in which now the electron departs from an orbital with contributions also from the Hg and Br atoms (delocalized orbital) to the same π* orbital (see the pink box in Figure a). While type (i) occurs at the Franck–Condon geometry (band maximum), type (ii) appears in other surrounding geometries and contributes to the increase in the intensity of the S 1 band. Type (ii) contributions, from excitations of the HgBr part of the molecule, shall affect the photodynamics of the system, as shown below.…”
Section: Resultssupporting
confidence: 89%
“…The remaining trajectories (10 %) yield HgBr upon release of NO 2 . These results confirm previous CCSD(T) estimations, which pointed to HgBrO as the main photoproduct . However, the present dynamic calculations allow us to quantify the specific yield of each reaction channel.…”
Section: Resultssupporting
confidence: 89%
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