Comparison between Ultrafast Fluorescence Dynamics of FMN Binding Protein from Desulfovibrio vulgaris, Strain Miyazaki, in Solution vs Crystal Phases

Equivalence between inverted regions of the energy gap law and inverted regions of donor–acceptor distances in photoinduced electron transfer processes in flavoproteins

In the present work, we discuss about the relationship between the energy gap law and extended Dutton law in flavoproteins. The extend Dutton law is defined herein as the dependence of logarithmic rates (ln Rate) of photoinduced electron transfer (ET) from aromatic amino acids to excited isoalloxazine (Iso*) on donor–acceptor distances (Rcs). Both functions of ln Rate vs. negative values of the standard free energy gap and ln Rate vs. Rc display a parabolic behavior, when the ET rates are ultrafast. The negative values of the standard free energy gap at peaks of ln Rate [X_m(ES)] were obtained for FMN-binding protein, wild-type pyranose 2-oxidase, T169S (Thr169 is replaced by Ser) pyranose 2-oxidase, and medium-chain acyl-CoA dehydrogenase. The values of Rc at peaks of ln Rate [X_m(Rc)] were also obtained for these flavoproteins. The negative values of the standard free energy gap decreased with approximate linear functions of Rc. The negative values of standard free energy gap [X_m(ESRc)] at Rc = X_m(Rc) were evaluated using the linear functions of the negative standard free energy gap with Rc. The values of X_m(ESRc) were mostly in very good agreement with the values of X_m(ES). This implies that the energy gap law and the extend Dutton law are equivalent. X_m(ES) values in ET donors displaying the linear extend Dutton law with Rc were obtained by energy gap law, and then X_m(Rc) values were evaluated with the negative standard free energy gap. Thus, the obtained X_m(Rc) values were much smaller than the Rc range obtained by the method of molecular dynamics simulation. This suggests that ET processes with linear profiles of the extend Dutton law could be parabolic when Rc becomes much shorter than the Rc range obtained by the method of molecular dynamics simulation.

Relationship between EXDL and SEGL.

Synthesis, crystal structure and photophysical properties of 1,4-bis(1,3-diazaazulen-2-yl)benzene: a new π building block

A dimerized 1,3-diazaazulene derivative, namely 1,4-bis(1,3-diazaazulen-2-yl)benzene [or 2,2'-(1,4-phenylene)bis(1,3-diazaazulene)], C₂₂H₁₄N₄, (I), has been synthesized successfully through the condensation reaction between 2-methoxytropone and benzene-1,4-dicarboximidamide hydrochloride, and was characterized by ¹H NMR and ¹³C NMR spectroscopies, and ESI-MS. X-ray diffraction analysis reveals that (I) has a nearly planar structure with good π-electron delocalization, indicating that it might serve as a π building block. The crystal belongs to the monoclinic system. One-dimensional chains were formed along the a axis through π-π interactions and adjacent chains are stabilized by C-H...N interactions, forming a three-dimensional architecture. The solid emission of (I) in the crystalline form exhibited a 170 nm red shift compared with that in the solution state. The observed optical bandgap for (I) is 3.22 eV and a cyclic voltammetry experiment confirmed the energy levels of the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO). The calculated bandgap for (I) is 3.37 eV, which is very close to the experimental result. In addition, the polarizability and hyperpolarizability of (I) were appraised for its further application in second-order nonlinear optical materials.

Conformational difference between two subunits in flavin mononucleotide binding protein dimers from Desulfovibrio vulgaris (MF): molecular dynamics simulation

The structural and dynamical properties of five FMN binding protein (FBP) dimers, WT (wild type), E13K (Glu13 replaced by Lys), E13R (Glu13 replaced by Arg), E13T (Glu13 replaced by Thr) and E13Q (Glu13 replaced by Gln), were investigated using a method of molecular dynamics simulation (MDS). In crystal structures, subunit A (Sub A) and subunit B (Sub B) were almost completely equivalent in all of the five FBP dimers. However, the predicted MDS structures of the two subunits were not equivalent in solution, revealed by the distances and inter-planar angles between isoalloxazine (Iso) and aromatic amino acids (Trp32, Tyr35 and Trp106) as well as the hydrogen bonding pairs between Iso and nearby amino acids. Residue root of mean square fluctuations (RMSF) also displayed considerable differences between Sub A and Sub B and in the five FBP dimers. The dynamics of the whole protein structures were examined with the distance (RNN) between the peptide N atom of the N terminal (Met1) and the peptide N atom of the C terminal (Leu122). Water molecules were rarely accessible to Iso in all FBP dimers which are in contrast with other flavoenzymes.

Classification of the mechanisms of photoinduced electron transfer from aromatic amino acids to the excited flavins in flavoproteins

Emission wavelength-dependence of the relationship between logarithmic ET rate vs. donor–acceptor distance in pyranose 2-oxidase.

Excited state dynamics can be used to probe donor-acceptor distances for H-tunneling reactions catalyzed by flavoproteins

In enzyme systems where fast motions are thought to contribute to H-transfer efficiency, the distance between hydrogen donor and acceptor is a very important factor. Sub-ångstrom changes in donor-acceptor distance can have a large effect on the rate of reaction, so a sensitive probe of these changes is a vital tool in our understanding of enzyme function. In this study we use ultrafast transient absorption spectroscopy to investigate the photoinduced electron transfer rates, which are also very sensitive to small changes in distance, between coenzyme analog, NAD(P)H4, and the isoalloxazine center in the model flavoenzymes morphinone reductase (wild-type and selected variants) and pentaerythritol tetranitrate reductase (wild-type). It is shown that upon addition of coenzyme to the protein the rate of photoinduced electron transfer is increased. By comparing the magnitude of this increase with existing values for NAD(P)H4-FMN distances, based on charge-transfer complex absorbance and experimental kinetic isotope effect reaction data, we show that this method can be used as a sensitive probe of donor-acceptor distance in a range of enzyme systems.

Photoinduced electron transfer modeling to simulate flavoprotein fluorescence decay

A method of analysis is described on the photoinduced electron transfer (PET) from aromatic amino acids as tryptophans (Trp) and tyrosines (Tyr) to the excited isoalloxazine (Iso*) in FMN-binding proteins (FBP) from Desulfovibrio vulgaris (strain, Miyazaki F). Time-dependent geometrical factors as the donor-acceptor distances are determined by means of a molecular dynamics simulation (MDS) of the proteins. Fluorescence decays of the single mutated isoforms of FBP are used as experimental data. The electrostatic (ES) energy between the photoproducts and ionic groups in the proteins is introduced into the Kakitani and Mataga (KM) model, which is modeled for an electron transfer process in solution. The PET parameters contained in the KM rate are determined by means of a nonlinear least square method, according to the Marquardt algorithm. The agreement between the observed and calculated decays is quite good, but not optimal. Characteristics on PET in flavoproteins, obtained by the present method, are described. Possible improvements of the method are discussed.

Theoretical analyses of the fluorescence lifetimes of the d-amino acid oxidase–benzoate complex dimer from porcine kidney: molecular dynamics simulation and photoinduced electron transfer

The mechanism of photoinduced electron transfer from benzoate and aromatic amino acids to the excited isoalloxazine in the d-amino acid oxidase–benzoate complex dimer was studied using molecular dynamics simulation and an electron transfer theory.

Femtosecond dynamics of short-range protein electron transfer in flavodoxin

Intraprotein electron transfer (ET) in flavoproteins is important for understanding the correlation of their redox, configuration, and reactivity at the active site. Here, we used oxidized flavodoxin as a model system and report our complete characterization of a photoinduced redox cycle from the initial charge separation in 135-340 fs to subsequent charge recombination in 0.95-1.6 ps and to the final cooling relaxation of the product(s) in 2.5-4.3 ps. With 11 mutations at the active site, we observed that these ultrafast ET dynamics, much faster than active-site relaxation, mainly depend on the reduction potentials of the electron donors with minor changes caused by mutations, reflecting a highly localized ET reaction between the stacked donor and acceptor at a van der Waals distance and leading to a gas-phase type of bimolecular ET reaction confined in the active-site nanospace. Significantly, these ultrafast ET reactions ensure our direct observation of vibrationally excited reaction product(s), suggesting that the back ET barrier is effectively reduced because of the decrease in the total free energy in the Marcus inverted region, leading to the accelerated charge recombination. Such vibrationally coupled charge recombination should be a general feature of flavoproteins with similar configurations and interactions between the cofactor flavin and neighboring aromatic residues.

Effects of the disappearance of one charge on ultrafast fluorescence dynamics of the FMN binding protein

Crystal structures of E13T (Glu13 was replaced by Thr13) and E13Q (Glu13 was replaced by Gln13) FMN binding proteins (FMN-bp) from Desulfovibrio vulgaris, strain Miyazaki F, were determined by the X-ray diffraction method. Geometrical factors related to photoinduced electron transfer from Trp32, Tyr35, and Trp106 to the excited isoalloxazine (Iso*) were compared among the three forms of FMN-bp. The rate of ET is considered to be fastest from Trp32 to Iso* in FMN-bp and then from Tyr35 and Trp106. The distances between Iso and Trp32 did not change appreciably (0.705-0.712 nm) among WT, E13T, and E13Q FMN-bps, though the distances between Iso and Tyr35 or Trp106 became a little shorter by ca. 0.01 nm in both mutated FMN-bps. The distances between the residue at 13 and the ET donors or acceptor in the mutated proteins, however, changed markedly, compared to WT. Hydrogen bonding pairs and distances between Iso and surrounding amino acids were not modified when Glu13 was replaced by Thr13 or Gln13. Effects of elimination of ionic charge at Glu13 on the ultrafast fluorescence dynamics in E13T and E13Q were investigated comparing to WT, by means of a fluorescence up-conversion method. Fluorescence lifetimes were tau(1) = 107 fs (alpha(1) = 0.86), tau(2) = 475 fs (alpha(2) = 0.12), and tau(3) = 30 ps (alpha(3) = 0.02) in E13T and tau(1) = 134 fs (alpha(1) = 0.85), alpha(2) = 746 fs (alpha(2) = 0.12), and tau(3) = 30 ps (alpha(3) = 0.03) in E13Q, which are compared to the reported lifetimes in WT, tau(1) = 168 fs (alpha(1) = 0.95) and alpha(2) = 1.4 ps (alpha(2) = 0.05). Average lifetimes (tau(AV) = Sigma(i=1)(2or3)alpha(i)tau(i)) were 0.75 ps in E13T, 1.10 ps in E13Q, and 0.23 ps in WT, which implies that tau(AV) was 3.3 times longer in E13T and 4.8 times longer in E13Q, compared to WT. The ultrafast fluorescence dynamics of WT did not change when solvent changed from H(2)O to D(2)O. Static ET rates (inverse of average lifetimes) were analyzed with static structures of the three systems of FMN-bp. Net electrostatic (ES) energies of Iso and Trp32, on which ET rates depend, were 0.0263 eV in WT, 0.322 eV in E13T, and 0.412 eV in E13Q. The calculated ET rates were in excellent agreement with the observed ones in all systems.

Ultrafast solvation dynamics of flavin mononucleotide in the reductase component of p-hydroxyphenylacetate hydroxylase

The reductase unit of p-hydroxyphenylacetate hydroxylase contains flavin mononucleotide (FMN) as a cofactor. Fluorescence decay curves measured by fluorescence up-conversion method were remarkably dependent on monitored emission wavelength. The fluorescence lifetime was shorter at the shorter emission wavelengths and longer at the longer wavelengths. Spectral shift correlation function of p-coumaric acid in water and FMN in C1 protein in buffer solution were expressed by two-exponential functions. Correlation times, phi1 and phi2, of p-coumaric acid were 0.053 and 0.650 ps, respectively, which was similar to previous works. phi1 and phi2 of C1 were 0.455 and 250 ps, respectively. The Stokes shift from t=0 to t=infinity was 2200 cm(-1), while it is 500 cm(-1) in the static Stokes shift obtained by the solvent effect of the fluorescence spectrum under static excitation. This suggests that the isoalloxazine ring of FMN in C1 is exposed in hydrophilic environment. Such large Stokes shift was unusual among flavoproteins. The biphasic decay of the spectral correlation function in C1 was discussed and compared to the biphasic decay of tryptophan in proteins.

Acceleration of electron-transfer-induced fluorescence quenching upon conversion to the signaling state in the blue-light receptor, TePixD, from Thermosynechococcus elongatus

TePixD is a blue light using flavin (BLUF) protein of a thermophilic cyanobacterium, Thermosynechococcus elongatus. The fluorescence dynamics of TePixD was observed for the first time in both its dark-adapted and signaling (red-shifted) forms with a 200-fs time resolution. The fluorescence up-conversion setup was used in the time region up to 60 ps, and the streak-camera setup was used in the time region up to 1 ns. To avoid the accumulation of the red-shifted form by the exciting laser irradiation, the sample solution was circulated using a diaphragm pump. A handmade flow cuvette with a small cross section was used to achieve a fast flow of the solution in the excited region. The fluorescence decay times were unequivocally determined to be 13.6 and 114 ps for the dark-adapted form and 1.37 ps for the red-shifted form. The double-exponential fluorescence decay in the dark-adapted form suggested the coexistence of two conformations that have the 13.6- and 114-ps decay components, respectively. The single-exponential fluorescence decay in the red-shifted form suggested the elimination of heterogeneity in the conformation upon the light-induced conversion. The fast fluorescence-quenching components were almost eliminated in the mutant in which the conserved tyrosine Tyr8 is replaced by phenylalanine. Thus, the fluorescence quench was concluded to arise from the electron transfer from Tyr8, to the excited flavin chromophore. The 10-fold-faster quenching in the red-shifted form suggested the acceleration of the electron transfer. The faster decay time of 13.6 ps for the dark-adapted form was found to be almost temperature independent in the region from 10 to 40 degrees C. This suggested that the energy gap, DeltaG, in Marcus's electron-transfer theory is optimized to give the fastest rate. The acceleration of the electron transfer in the red-shifted form is interpreted to be due to the enhancement of the electronic-coupling factor between the donor and acceptor. A shortening of the Tyr8-flavin distance by 1.0-1.5 A was suggested if we adopt the empirical formula for the donor-acceptor distance dependence of the electron transfer rate.

Simultaneous analysis of ultrafast fluorescence decays of FMN binding protein and its mutated proteins by molecular dynamic simulation and electron transfer theory

Ultrafast fluorescence decays of FMN binding proteins (FBP) from Desulfovibrio vulgaris (Miyazaki F) were analyzed with an electron transfer (ET) theory by Kakitani and Mataga (KM theory). Time-dependent distances among isoalloxazine (Iso) and Trp-32, Tyr-35, and Trp-106 in wild-type FBP (WT), among Iso and Tyr-32, Tyr-35, and Trp-106 in W32Y (Trp-32 was replaced by Tyr-32), and among Iso and Tyr-35 and Trp-106 in W32A (Trp-32 was replaced by Ala-32) were determined by molecular dynamic simulation (MD). Electrostatic energies between Iso anion and all other ionic groups, between Trp-32 cation and all other ionic groups, and between Tyr-32 cation and all other ionic groups were calculated in WT, W32Y, and W32A, from the MD coordinates. ET parameters contained in KM theory, such as frequency (nu 0), a coefficient of the ET process (beta), a critical distance of the ET process ( R 0), standard free energy related to the electron affinity of the excited Iso ( G Iso (0)), and the static dielectric constant in FBP species (epsilon 0), were determined with and without inclusion of the electrostatic energy, so as to fit the calculated fluorescence decays with the observed decays of all FBP species, by a nonlinear least-squares method according to the Marquardt algorithm. In the analyses the parameters, nu 0, beta, and R 0 were determined separately between Trp residues and Tyr residues among all FBP species. Calculated fluorescence intensities with the inclusion of the electrostatic energy fit quite well with the observed ones of all WT, W32Y, and W32A.

Ultrafast structural dynamics in BLUF domains: transient infrared spectroscopy of AppA and its mutants

The structural dynamics following photoexcitation of a photosensing BLUF (blue light sensing using FAD) domain protein have been investigated by ultrafast transient infrared spectroscopy. Specifically, the transcriptional antirepressor AppA from Rhodobacter sphaeroides has been studied in the light and dark adapted forms and in photoactive and inactive mutants W104F and Q63L. A transient absorption has been observed at 1666 cm(-1) which is a marker mode for the photoactive state of the protein. This instantaneously formed transient is tentatively assigned to a vibrational mode of a protein residue modified through its interaction with the excited state of the chromophore. A plausible candidate consistent with the mutant studies is the carbonyl stretch of the Q63 amide side chain. These results suggest that modification of the strength of protein chromophore H-bonded interactions is the primary step in the BLUF domain photocycle. No new species were observed to be formed during the first nanosecond. Measurement of the ultrafast ground state recovery showed that the excited state of light adapted AppA is strongly quenched compared to the dark adapted state. It is proposed that the reorganization which occurs to form the signaling state is favorable to electron-transfer quenching.