Ultrafast nonadiabatic dynamics of [Fe(II)(bpy)(3)](2+) in solution

The ultrafast relaxation of aqueous iron(II)-tris(bipyridine) upon excitation into the singlet metal-to-ligand charge-transfer band (1MLCT) has been characterized by femtosecond fluorescence up-conversion and transient absorption (TA) studies. The fluorescence experiment shows a very short-lived broad 1MLCT emission band at approximately 600 nm, which decays in < or =20 fs, and a weak emission at approximately 660 nm, which we attribute to the 3MLCT, populated by intersystem crossing (ISC) from the 1MLCT state. The TA studies show a short-lived (<150 fs) excited-state absorption (ESA) below 400 nm, and a longer-lived one above 550 nm, along with the ground-state bleach (GSB). We identify the short-lived ESA as being due to the 3MLCT state. The long-lived ESA decay and the GSB recovery occur on the time scale of the lowest excited high-spin quintet state 5T2 lifetime. A singular value decomposition and a global analysis of the TA data, based on a sequential relaxation model, reveal three characteristic time scales: 120 fs, 960 fs, and 665 ps. The first is the decay of the 3MLCT, the second is identified as the population time of the 5T2 state, while the third is its decay time to the ground state. The anomalously high ISC rate is identical in [RuII(bpy)3]2+ and is therefore independent of the spin-orbit constant of the metal atom. To reconcile these rates with the regular quasi-harmonic vibrational progression of the 1MLCT absorption, we propose a simple model of avoided crossings between singlet and triplet potential curves, induced by the strong spin-orbit interaction. The subsequent relaxation steps down to the 5T2 state dissipate approximately 2000 cm-1/100 fs. This rate is discussed, and we conclude that it nevertheless can be described by the Fermi golden rule, despite its high value.     

(Sub)-picosecond spectral evolution of fluorescence in photoactive proteins studied with a synchroscan streak camera system

The spectral evolution of three photoactive proteins has been investigated by measuring the fluorescence with good temporal and wavelength resolution and a high signal-to-noise ratio. Upon excitation at 400 nm wild-type (wt) PYP both at neutral pH and in the low-pH blueshifted pBdark state exhibited a strong quenching of the fluorescence, the major part of which could be described by lifetimes of about 1.7 and 7.7 ps. The remaining fluorescence decay occurred multiexponentially with lifetimes between 30 and 125 ps. Additionally, in wtPYP at neutral pH, a dynamic Stokes shift was found to occur with a time constant of about 0.25 ps. In a PYP preparation that was reconstituted with the chromophore 7-hydroxy-coumarin-3- carboxylic acid rather than the native coumaric acid, and which is therefore not capable of performing the cis-trans-isomerization that initiates the photocycle in wtPYP, the fluorescence was found to decay multiexponentially with lifetimes of 51 ps, 0.33 and 3.77 ns. Additionally, dynamic Stokes shifts were observed with time constants of about 0.1 and 3.5 ps. Upon comparison of the dynamics of this preparation with that of wtPYP the multiexponential decay with lifetimes of 1.7 and 7.7 ps found in wtPYP was attributed to photochemistry of the p-coumaric-acid chromophore. The emission from bacteriorhodopsin mutant D85S upon excitation at 635 nm decays biexponentially with estimated lifetimes of 5.2 and 19.1 ps. No dynamic Stokes shift was observed here. Four lifetimes were needed to describe the decay of the emission from the A* state in the green fluorescent protein. From a target analysis it was concluded that the longer lifetimes are accompanied by a decreasing probability of forming I*, which approaches zero with the longest A* lifetime of 1.5 ns. These observations may be explained by heterogeneity of A and by relaxation of A*. In all three systems studied, multiexponential decay of emission was present, suggesting that heterogeneity is a common feature of these chromophore protein complexes.     

3-Fluoro-N-methyl-D-aspartic acid (3F-NMDA) stereoisomers as conformational probes for exploring agonist binding at NMDA receptors

N-Methyl-D-aspartate (NMDA) is the prototypical agonist of the NMDA receptor subtype of ionotropic glutamate receptors. Stereogenic placement of a C-F bond at the 3-position of (S)-NMDA generates either the (2S,3S)- or (2S,3R)- diastereoisomers of 3F-NMDA. The individual diastereoisomers were prepared by synthesis in enantiomerically pure forms and it was found that (2S,3S)-3F-NMDA is an agonist with a comparable potency to NMDA itself, whereas the (2S,3R)-diastereoisomer has negligible potency. The difference in potency of these stereoisomers is attributed to a preference of the C-F bond (2S,3S)-3F-NMDA to adopt a gauche conformation to the C-N(+) bond in the binding conformation, whereas the (2S,3R)-3F-NMDA forces these bonds anti, losing electrostatic stabilisation, to achieve the required binding conformation. These observations illustrate the utility of stereoselective fluorination in influencing the molecular conformation of β-fluorinated amino acids and thus probing the active conformations of bioactive compounds at receptors.     

Ultrabroadband femtosecond two-dimensional ultraviolet transient absorption

We present a broadband two-dimensional transient absorption setup for the UV around 300 nm with a time resolution of 150 fs. A narrowband, frequency tunable pump pulse and a broadband probe pulse are generated from the output of a noncollinear optical parametric amplifier operated at 20 kHz repetition rate and combined in a spectrally resolved transient absorption experiment. The high repetition rate and low noise of the setup allow us to acquire high quality two-dimensional data as a function of time delay with an unsurpassed frequency window of 10,000 and 8000 cm(-1) along the probe and pump axis, respectively. The performance of the setup is demonstrated on 2,5-Diphenyloxazol dissolved in cyclohexane.     

Low-energy electron scattering with the purine bases of DNA/RNA using the R-matrix method

R-matrix calculations on electron collisions with the purine bases found in DNA and RNA (i.e., adenine and guanine) are presented. Resonant anion states of these systems are identified by employing different approximation levels of ab initio theoretical methods, such as the static exchange, the static exchange plus polarization, and the close-coupling methods. The results are compared with other available calculations and experiments. All of these ab initio approximations, which we refer to as a scattering "model," give four shape resonances of (2)A' (π) symmetry within the energy range of 10 eV for both molecules. For adenine, the most sophisticated method, the close-coupling model, gives two very narrow (2)A' (σ) symmetry Feshbach-type resonances at energies above 5 eV. Quantitative results for the total elastic and electronic excitation cross sections are also presented.     

Comment on "aromatic-backbone interactions in model alpha-helical peptides" [Palermo et al., J Comput Chem 2007, 28, 1208

Palermo et al. have recently published a method to correct for intramolecular basis set superposition errors (J Comput Chem 2007, 28, 1208) in intramolecular interactions occurring in peptides. By considering the intermolecular equivalent of this method, it is shown that the method presented by Palermo et al. underestimates the magnitude of the intramolecular BSSE.     

3‐Fluoro‐N‐methyl‐D‐aspartic acid (3F‐NMDA) Stereoisomers as Conformational Probes for Exploring Agonist Binding at NMDA Receptors

N‐Methyl‐D ‐aspartate (NMDA) is the prototypical agonist of the NMDA receptor subtype of ionotropic glutamate receptors. Stereogenic placement of a C? F bond at the 3‐position of (S)‐NMDA generates either the (2S,3S)‐ or (2S,3R)‐ diastereoisomers of 3F‐NMDA. The individual diastereoisomers were prepared by synthesis in enantiomerically pure forms and it was found that (2S,3S)‐3F‐NMDA is an agonist with a comparable potency to NMDA itself, whereas the (2S,3R)‐diastereoisomer has negligible potency. The difference in potency of these stereoisomers is attributed to a preference of the C? F bond (2S,3S)‐3F‐NMDA to adopt a gauche conformation to the C? N⁺ bond in the binding conformation, whereas the (2S,3R)‐3F‐NMDA forces these bonds anti, losing electrostatic stabilisation, to achieve the required binding conformation. These observations illustrate the utility of stereoselective fluorination in influencing the molecular conformation of β‐fluorinated amino acids and thus probing the active conformations of bioactive compounds at receptors.     

DNA base stacking: The stacked uracil/uracil and thymine/thymine minima

The potential energy surfaces of stacked uracil dimer (U/U) and stacked thymine dimer (T/T) have been explored at the counterpoise (CP)‐corrected M06‐2X/6‐31+G(d) level of theory, in the gas phase and in solution (with water and, for U/U, 1,4‐dioxane as the solvents) modeled by a continuum solvent using the polarizable continuum model. Potential energy scans were created by rotation of one monomer around its center‐of‐mass, whereas the other monomer remained still. Both face‐to‐back (one molecule exactly on top of the other) and face‐to‐face (one base molecule flipped by 180°) structures were considered. Five or six (dependent on whether CP correction is included or not) stacked uracil dimer minima and six stacked thymine dimer minima were located. A number of transition states on the U/U and T/T potential energy surfaces were likewise identified. The general effect of the continuum solvent is a flattening of the potential energy surface. Comparison of the gas‐phase M06‐2X/6‐31+G(d) U/U interaction energies with estimated CCSD(T)/complete basis set values (where available) show the excellent performance of this functional for stacking energies. © 2012 Wiley Periodicals, Inc.