The structural dynamics of mismatched base pairs in duplex DNA have been studied by time-resolved fluorescence anisotropy decay measurements on a series of duplex oligodeoxynucleotides of the general type d[CGG(AP)GGC].d[GCCXCCG], where AP is the fluorescent adenine analogue 2-aminopurine and X = T, A, G, or C. The anisotropy decay is caused by internal rotations of AP within the duplex, which occur on the picosecond time scale, and by overall rotational diffusion of the duplex. The correlation time and angular range of internal rotation of AP vary among the series of AP.X mismatches, showing that the native DNA bases differ in their ability to influence the motion of AP. These differences are correlated with the strength of base-pairing interactions in the various AP.X mismatches. The interactions are strongest with X = T or C. The ability to discern differences in the strength of base-pairing interactions at a specific site in DNA by observing their effect on the dynamics of base motion is a novel aspect of the present study. The extent of AP stacking within the duplex is also determined in this study since it influences the excited-state quenching of AP. AP is thus shown to be extrahelical in the AP.G mismatch. The association state of the AP-containing oligodeoxynucleotide strand is determined from the temperature-dependent tumbling correlation time. An oligodeoxynucleotide triplex is formed with a particular base sequence in a pH-dependent manner.

The solvent-dependent ground-state conformational equilibrium and excited-state dynamics of 2-(2′-hydroxyphenyl)benzoxazole have been characterized in several solvents on the femtosecond to nanosecond time scales. The only observable ground-state tautomer is the enol, which exists in equilibrium between the syn-and anti-rotational isomers. In the anti-enol isomer, the phenyl hydroxyl group appears to not interact strongly with solvent but rather forms a strong intramolecular hydrogen bond with the benzoxazole oxygen atom. In the syn-enol isomer, the phenyl hydroxyl proton may interact with solvent or form an internal hydrogen bond with the benzoxazole nitrogen atom. Upon excitation, the proton is transferred from the oxygen atom to the nitrogen atom of the internally hydrogen bonded syn-enol isomer in 170 fs, regardless of the solvent. The lifetime of the resulting excited keto tautomer is solvent dependent and on the order of picoseconds. In addition to these dynamics, several additional dynamic processes are detected which may correspond to relaxation of a distorted excited keto tautomer.

The conductance of molecular junctions, formed by breaking gold point contacts dressed with various thiol functionalized organic molecules, is measured at 293 K and at 30 K. In the presence of molecules, individual conductance traces measured as a function of increasing gold electrode displacement show clear steps below the quantum conductance steps of the gold contact. These steps are distributed over a wide range of molecule-dependent conductance values. Histograms constructed from all conductance traces therefore do not show clear peaks either at room or low temperatures. Filtering of the data sets by an objective automated procedure only marginally improves the visibility of such features. We conclude that the geometrical junction to junction variations dominate the conductance measurements.

To understand in atomic detail how a chromophore and a protein interact to sense light and send a biological signal, we are characterizing photoactive yellow protein (PYP), a water-soluble, 14 kDa blue-light receptor which undergoes a photocycle upon illumination. The active site residues glutamic acid 46, arginine 52, tyrosine 42, and threonine 50 form a hydrogen bond network with the anionic p-hydroxycinnamoyl cysteine 69 chromophore in the PYP ground state, suggesting an essential role for these residues for the maintenance of the chromophore's negative charge, the photocycle kinetics, the signaling mechanism, and the protein stability. Here, we describe the role of T50 and Y42 by use of site-specific mutants. T50 and Y42 are involved in fine-tuning the chromophore's absorption maximum. The high-resolution X-ray structures show that the hydrogen-bonding interactions between the protein and the chromophore are weakened in the mutants, leading to increased electron density on the chromophore's aromatic ring and consequently to a red shift of its absorption maximum from 446 nm to 457 and 458 nm in the mutants T50V and Y42F, respectively. Both mutants have slightly perturbed photocycle kinetics and, similar to the R52A mutant, are bleached more rapidly and recover more slowly than the wild type. The effect of pH on the kinetics is similar to wild-type PYP, suggesting that T50 and Y42 are not directly involved in any protonation or deprotonation events that control the speed of the light cycle. The unfolding energies, 26.8 and 25.1 kJ/mol for T50V and Y42F, respectively, are decreased when compared to that of the wild type (29.7 kJ/mol). In the mutant Y42F, the reduced protein stability gives rise to a second PYP population with an altered chromophore conformation as shown by UV/visible and FT Raman spectroscopy. The second chromophore conformation gives rise to a shoulder at 391 nm in the UV/visible absorption spectrum and indicates that the hydrogen bond between Y42 and the chromophore is crucial for the stabilization of the native chromophore and protein conformation. The two conformations in the Y42F mutant can be interconverted by chaotropic and kosmotropic agents, respectively, according to the Hofmeister series. The FT Raman spectra and the acid titration curves suggest that the 391 nm form of the chromophore is not fully protonated. The fluorescence quantum yield of the mutant Y42F is 1.8% and is increased by an order of magnitude when compared to the wild type.