Abstract:The absorption spectra and transition moment directions of the
four DNA bases and uracil were calculated,
utilizing the semiempirical INDO/S-CI method and the ab
initio CIS/6-31G* method. A linear scaling of
the
CIS/6-31G* transition energies was necessary to get good agreement with
the observed energies. CASPT2
π → π* transition energies and polarizations of adenine were also
calculated. Fully MP2/6-31G*-optimized
geometries were used in the calculations of the electronic spectra.
The effect of possible taut… Show more
“…Table I shows the computed wavelengths and oscillator strengths for the lowest energy vertical transitions of the single-stranded (three base) and doubled-stranded (six base) structures studied. As the method used, CIS, is known to systematically over-estimate transition energies, mainly due to its neglect of electron correlation, the computed energies have been scaled by a constant factor of 0.72, as recommended by Broo and Holmén [9]. It should be noted that the absolute values of the oscillator strengths will also be lower than those predicted by the CIS method.…”
2-Aminopurine (2AP) is a widely used marker for nucleic acid structure because the fluorescence of 2AP in double-stranded DNA is approximately half that of 2AP in single-stranded DNA. The underlying photophysical mechanism responsible for the change in fluorescence with structure is not understood. We have performed CIS and TDB3LYP level calculations on double-stranded trinucleotide models, (X2APX)⅐(YTY), where X and Y represent the natural nucleobases. The results reveal that base stacking combined with hydrogen bonding reduces the oscillator strength for the fluorescence transition, and hence the fluorescence quantum yield. It is also shown that the electronic transitions of double-stranded trinucleotides are not simply those of the individual bases, but rather involve orbitals that are delocalized across several bases. Although the results obtained at the CIS level suffer from the neglect of electron correlation, the results obtained at the TDB3LYP level are not necessarily better because this method has problems describing long-range interactions and tends to underestimate the energies of charge-transfer states. Calculations on a full (rather than model) dinucleotide 5Ј-G2AP-3Ј confirm that the inclusion of the sugar and phosphate groups is not necessary when studying the energetically low-lying excited states of nucleic acids containing 2AP.
“…Table I shows the computed wavelengths and oscillator strengths for the lowest energy vertical transitions of the single-stranded (three base) and doubled-stranded (six base) structures studied. As the method used, CIS, is known to systematically over-estimate transition energies, mainly due to its neglect of electron correlation, the computed energies have been scaled by a constant factor of 0.72, as recommended by Broo and Holmén [9]. It should be noted that the absolute values of the oscillator strengths will also be lower than those predicted by the CIS method.…”
2-Aminopurine (2AP) is a widely used marker for nucleic acid structure because the fluorescence of 2AP in double-stranded DNA is approximately half that of 2AP in single-stranded DNA. The underlying photophysical mechanism responsible for the change in fluorescence with structure is not understood. We have performed CIS and TDB3LYP level calculations on double-stranded trinucleotide models, (X2APX)⅐(YTY), where X and Y represent the natural nucleobases. The results reveal that base stacking combined with hydrogen bonding reduces the oscillator strength for the fluorescence transition, and hence the fluorescence quantum yield. It is also shown that the electronic transitions of double-stranded trinucleotides are not simply those of the individual bases, but rather involve orbitals that are delocalized across several bases. Although the results obtained at the CIS level suffer from the neglect of electron correlation, the results obtained at the TDB3LYP level are not necessarily better because this method has problems describing long-range interactions and tends to underestimate the energies of charge-transfer states. Calculations on a full (rather than model) dinucleotide 5Ј-G2AP-3Ј confirm that the inclusion of the sugar and phosphate groups is not necessary when studying the energetically low-lying excited states of nucleic acids containing 2AP.
“…As a rule, excitation energies are substantially overestimated in the CIS calculations, since it fails to properly account for differences in dynamical electron correlation in the ground and the excited states. Broo and Holmén have suggested that this difference is comparable in all the nucleobases and have used a scaling factor of 0.72 for the excitation energies of π − π * transitions [22].…”
Abstract:We have theoretically characterized the ground state and the excited state properties of wybutine, a naturally fluorescent modified base occuring in tRNAs, using configuration interaction singles (CIS) and time dependent density functional (TDDFT) methods. Both gas phase excited state properties and solvent effects, modelled through Onsager reaction field method, were considered. In addition to vertical excitation energies, the fluorescence transitions were calculated, based on S 1 equilibrium geometry optimized at CIS level. Our computations show encouraging agreement with known experimental data either directly (TDDFT) or after applying empirical scaling (CIS). The fluorescence Stokes' shift for the S 0 ← S 1 transition is computed taking into account the contributions from both intramolecular and solvent reorganization processes. The results suggest that intramolecular relaxation of the S 1 state accounts for the major part of the magnitude of the Stokes' shift, while the role of solvent reorganization seems to be of less importance.
“…Guanine has been the subject of many theoretical [15][16][17][18][19][20][21][22][23][24][25][26][27][28][29] and experimental investigations. [30][31][32][33][34][35][36][37][38] Over the years a wealth of information about its ground and electronically electronic states has been gathered.…”
Electronic spectra of guanine in the gas phase and in water were studied by quantum mechanical/molecular mechanical (QM/MM) methods. Geometries for the excited-state calculations were extracted from ground-state molecular dynamics (MD) simulations using the self-consistent-charge density functional tight binding (SCC-DFTB) method for the QM region and the TIP3P force field for the water environment. Theoretical absorption spectra were generated from excitation energies and oscillator strengths calculated for 50 to 500 MD snapshots of guanine in the gas phase (QM) and in solution (QM/MM). The excited-state calculations used time-dependent density functional theory (TDDFT) and the DFT-based multireference configuration interaction (DFT/MRCI) method of Grimme and Waletzke, in combination with two basis sets. Our investigation covered keto-N7H and keto-N9H guanine, with particular focus on solvent effects in the low-energy spectrum of the keto-N9H tautomer. When compared with the vertical excitation energies of gas-phase guanine at the optimized DFT (B3LYP/TZVP) geometry, the maxima in the computed solution spectra are shifted by several tenths of an eV. Three effects contribute: the use of SCC-DFTB-based rather than B3LYP-based geometries in the MD snapshots (red shift of ca. 0.1 eV), explicit inclusion of nuclear motion through the MD snapshots (red shift of ca. 0.1 eV), and intrinsic solvent effects (differences in the absorption maxima in the computed gas-phase and solution spectra, typically ca. 0.1-0.3 eV). A detailed analysis of the results indicates that the intrinsic solvent effects arise both from solvent-induced structural changes and from electrostatic solute-solvent interactions, the latter being dominant.
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