Electronic transitions and ESIPT kinetics of the thienyl-3-hydroxychromone nucleobase surrogate in DNA duplexes: a DFT/MD-TDDFT study

The fluorescent nucleobase surrogate M (2-thienyl-3-hydroxychromone fluorophore) when imbedded in DNA opposite an abasic site exhibits a two colour response highly sensitive to environment changes and base composition. Its two colour emission originates from an excited state intramolecular proton transfer (ESIPT), which converts the excited normal N* form into its T* tautomer. To get deeper insight on the spectroscopic properties of M in DNA duplexes, quantum chemical calculations were performed on M stacked with different base pairs in model trimers extracted from MD simulations. The photophysics of M in duplexes appeared to be governed by stacking interactions as well as charge and hole transfer. Indeed, stacking of M in DNA screens M from H-bonding with water molecules, which favours ESIPT and thus, the emission of the T* form. With A and T flanking bases, the electronic densities in the frontier MOs were localized on M, in line with its effective absorption and emission. In addition, reduction of the free rotation between the thienyl and chromone groups together with the shielding of the dye from water molecules largely explain its enhanced quantum yield in comparison to the free M in solution. By contrast, the localisation of the electron density on the flanking G residues in the ground state and the energetically favorable hole transfer from M to G in the excited state explains the reduced quantum yield of M sandwiched between CG pairs. Finally, the much higher brightness of M as compared to 2-aminopurine when flanked by A and T residues could be related to the much stronger oscillator strength of its S₀ → S₁ transition and the ineffective charge transfer from M to A or T residues.

The fluorescent nucleobase surrogate M (2-thienyl-3-hydroxychromone fluorophore) when imbedded in DNA opposite an abasic site exhibits a two colour response highly sensitive to environment changes and base composition.

Structural and Dynamical Impact of a Universal Fluorescent Nucleoside Analogue Inserted Into a DNA Duplex

Recently, a 3-hydroxychromone based nucleoside 3HCnt has been developed as a highly environment-sensitive nucleoside surrogate to investigate protein-DNA interactions. When it is incorporated in DNA, the probe is up to 50-fold brighter than 2-aminopurine, the reference fluorescent nucleoside. Although the insertion of 3HCnt in DNA was previously shown to not alter the overall DNA structure, the possibility of the probe inducing local effects cannot be ruled out. Hence, a systematic structural and dynamic study is required to unveil the 3HCnt's limitations and to properly interpret the data obtained with this universal probe. Here, we investigated by NMR a 12-mer duplex, in which a central adenine was replaced by 3HCnt. The chemical shifts variations and nOe contacts revealed that the 3HCnt is well inserted in the DNA double helix with extensive stacking interactions with the neighbor base pairs. These observations are in excellent agreement with the steady-state and time-resolved fluorescence properties indicating that the 3HCnt fluorophore is protected from the solvent and does not exhibit rotational motion. The 3HCnt insertion in DNA is accompanied by the extrusion of the opposite nucleobase from the double helix. Molecular dynamics simulations using NMR-restraints demonstrated that 3HCnt fluorophore exhibits only translational dynamics. Taken together, our data showed an excellent intercalation of 3HCnt in the DNA double helix, which is accompanied by localized perturbations. This confirms 3HCnt as a highly promising tool for nucleic acid labeling and sensing.

Ab initio study of the solvent H-bonding effect on ESIPT reaction and electronic transitions of 3-hydroxychromone derivatives

The electronic transitions occurring in 4-(N,N-dimethylamino)-3-hydroxyflavone (DMAF) and 2-furanyl-3-hydroxychromone (FHC) were investigated using the TDDFT method in aprotic and protic solvents. The solvent effect was incorporated into the calculations via the PCM formalism. The H-bonding between solute and protic solvent was taken into account by considering a molecular complex between these molecules. To examine the effect of the H-bond on the ESIPT reaction, the absorption and emission wavelengths as well as the energies of the different states that intervene during these electronic transitions were calculated in acetonitrile, ethanol and methanol. The calculated positions of the absorption and emission wavelengths in various solvents were in excellent agreement with the experimental spectra, validating our approach. We found that in DMAF, the hydrogen bonding with protic solvents makes the ESIPT reaction energetically unfavourable, which explains the absence of the ESIPT tautomer emission in protic solvents. In contrast, the excited tautomer state of FHC remains energetically favourable in both aprotic and protic solvents. Comparing our calculations with the previously reported time-resolved fluorescence data, the ESIPT reaction of DMAF in aprotic solvents is reversible because the emitting states are energetically close, whereas in FHC, ESIPT is irreversible because the tautomer state is below the corresponding normal state. Therefore, the ESIPT reaction in DMAF is controlled by the relative energies of the excited states (thermodynamic control), while in FHC the ESIPT is controlled probably by the energetic barrier (kinetic control).

Time-resolved fluorescent properties of 8-vinyl-deoxyadenosine and 2-amino-deoxyribosylpurine exhibit different sensitivity to their opposite base in duplexes

8-Vinyl-deoxyadenosine (8VA) has been recently introduced as a fluorescent analogue of adenosine that is less perturbing and less quenched than the well-established 2-amino-deoxyribosylpurine (2AP) probe when inserted in oligonucleotides. To further validate 8VA as a fluorescent substitute of A, we compared the ability of 8VA and 2AP in sequences of the type d(CGT TTT XNX TTT TGC) (with N=8VA or 2AP and X=T and C) to discriminate the nature of the opposite base (Y) in duplexes. For both probes, systematic variations in the amplitudes of the short- and long-lived lifetimes of the fluorescence intensity decays as well as in the amplitude of the fast rotational correlation time of the fluorescence anisotropy decays were observed as a function of the nature of Y. From these parameters, we inferred a stability order 8VA-T > 8VA-G > 8VA-A > 8VA-C, similar to the stability order with the native A base, but different from the stability order with 2AP. Using a combination of molecular mechanics and ab initio calculations, we found that the time-resolved parameters of 8VA, but not the 2AP ones, correlate well with the geometry and the strength of the A-Y base-pairing interaction. This may be rationalized by the smaller structural and electronic perturbations induced by the vinyl group in position 8 as compared to the amino group at position 2. As a consequence, substitution of A by 8VA in a base pair was found to only minimally modify the structure and interaction energy of the base pair. Thus, 8VA can be used as a fluorescent substitute of the natural A, to straightforwardly discriminate the nature of the opposite base. This may find interesting applications notably in the elucidation of the mechanisms and dynamics of the DNA mismatch repair system.

Excited-State Properties and Transitions of Fluorescent 8-Vinyl Adenosine in DNA

8-vinyl-adenosine (8VA) is a new fluorescent nucleoside analogue with improved spectroscopic properties as compared to 2-aminopurine (2AP). To further understand its photophysics, we analyzed by the time-dependent density functional theory and the configuration interaction single method, the electronic properties, and transitions of 8VA in its free form and stacked with one or two flanking bases. For free 8VA, the predicted excited-state energy gaps, absorbance peak position, and oscillator strength were found to be in excellent agreement with the experimentally determined ones. Moreover, its high fluorescence quantum yield was found to be associated with the dipole-allowed S1 --> S0 transition. Stacking of 8VA with C, T, or A in dimers or trimers resulted in fluorescence quenching through mechanisms that depend on the nature and relative orientation of the flanking base(s). When 8VA is stacked with T, quenching mainly results from nonradiative relaxation to low-lying dark excited state(s) that do not exist in free 8VA. When 8VA is stacked with A, quenching results mainly from mixing of the molecular orbitals in the ground state. Both types of quenching are thought to accompany the stacking of 8VA with C. In addition, the C-8VA-C trimer was found to exhibit a low-lying S1 emissive state that may generate an increased fluorescence quantum yield and lifetime. The predicted photophysical properties of the trimers are highly consistent with the spectroscopic data of a series of 15-mer oligonucleotides differing only by the nature of the residues flanking the central 8VA.