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. 2022 Aug 4;13(30):7072-7080.
doi: 10.1021/acs.jpclett.2c01694. Epub 2022 Jul 28.

A Plausible Mechanism of Uracil Photohydration Involves an Unusual Intermediate

Affiliations

A Plausible Mechanism of Uracil Photohydration Involves an Unusual Intermediate

Woojin Park et al. J Phys Chem Lett. .

Abstract

It is well-known that photolysis of pyrimidine nucleobases, such as uracil, in an aqueous environment results in the formation of hydrate as one of the main products. Although several hypotheses regarding photohydration have been proposed in the past, e.g., the zwitterionic and "hot" ground-state mechanisms, its detailed mechanism remains elusive. Here, theoretical nonadiabatic simulations of the uracil photodynamics reveal the formation of a highly energetic but kinetically stable intermediate that features a half-chair puckered pyrimidine ring and a strongly twisted intracyclic double bond. The existence and the kinetic stability of the intermediate are confirmed by a variety of computational chemistry methods. According to the simulations, the unusual intermediate is mainly formed almost immediately (∼50-200 fs) upon photoabsorption and survives long enough to engage in a hydration reaction with a neighboring water. A plausible mechanism of uracil photohydration is proposed on the basis of the modeling of nucleophilic insertion of water into the twisted double bond of the intermediate.

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Conflict of interest statement

The authors declare no competing financial interest.

Figures

Chart 1
Chart 1. Uracil (1), Its Photohydrate (2), and Photohydration Mechanism Hypothesized in ref (5)a
Chart 2
Chart 2. A Reactive Intermediate Proposed in This Worka
Figure 1
Figure 1
(a) Evolution of the population of the adiabatic S0–S3 states during the NAMD simulations. The time constants of the monoexponential fit of the S2 population and the biexponential fit of S0 are also shown. The margins of error were determined by bootstrapping. (b) Evolution of the HC5C6H dihedral angle (φ) during the NAMD simulations. The red circles show the S2 → S1 nonadiabatic transitions (surface hops), and the blue circles the S1 → S0 nonadiabatic transitions. The dashed horizontal lines show the dihedral angle values in the structures given to the right of the plot (see the text for more details). (c) MEPs on the S2 (blue), S1 (red), and S0 (black) PESs of uracil obtained using the nudged elastic band (NEB) optimization, in connection with the MRSF-TDDFT/BH&HLYP/6-31G* method. The MEPs are described in terms of the HC5C6H dihedral angle (denoted as φ) and the BLA distortion. The relative energies (in electronvolts) are given with respect to the S0 equilibrium geometry of uracil. The (BLA (Å), φ (deg), ΔE (eV)) values of the critical structures are (0, 0, 6.09) for FC, (0.13, 0.36, 5.58) for CI21,BLA, (0.19, 48.0, 5.27) for CI21,+ , (0.21, 2.00, 4.23) for S1,min, (0.02, 118.21, 4.35) for CI10,+, and (−0.04, 176.33, 3.54) for S0,min+. The green arrows show the relaxation paths characterized by distinct decay constants, τ1–τ3. The S1,min → CI10,+ path merges with the CI21,+ → CI10,+ MEP (at BLA = 0.013 Å, φ = 152.4°, and ΔE = 4.32 eV). (d) Structure and frontier orbitals of intermediate 4.
Chart 3
Chart 3. (a) Conformations of Hydroxo-uracila and (b) Relative Energies (kilocalories per mole) of the Intermediate Species in the Mechanism of Uracil 1 Hydration Obtained Using the BH&HLYP/cc-pVTZ Method on the PES of the Electronic Ground Stateb
Chart 4
Chart 4. Mechanism of Uracil Photohydration Suggested in This Worka

References

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