Activation of electron transfer reactions of the blue proteins.

Thermal activation of electron transfer reactions of the blue proteins is considered in terms of vibronic coupling. Use of the electron paramagnetic resonance spectral distribution to obtain an estimate of the force constant for the relevant protein mode is proposed and demonstrated. This analysis leads to a model in which the configurations of the cupric and cuprous sites are displaced only a few degrees from each other, both being close to the configuration midway between planar and tetrahedral.     

An asymmetric dimer exciton model. Application to the primary electron donor of bacterial photoreaction center

An asymmetric dimer excition theory is developed that takes into account both environmental and vibronic effects on the electronic transition energies. Explicit equations are presented for the transition energies, the dipole moments, the angle between the dipole moments and the dipole and rotational strengths for the electronic transitions in this asymmetric dimer. This model is proposed to describe the structure of the special pair of bacteriochlorophyll a molecules believed to constitute the primary electron donor of bacterial photoreaction center. The model is found to be consistent with most of the spectroscopic properties of the photoreaction center. We used the equations derived from the asymmetric model along with absorption and circular dichroism spectroscopy data to predict a geometrical structure for the primary electron donor.     

Correct interpretation of heme protein spectra allows distinguishing between the heme and the protein dynamics

It is shown by using the vibronic approach that the iron displacement out of the porphyrin plane in deoxyheme proteins intermixes the porphyrin pi and axial iron-histidine sigma electronic subsystems. This intermixing explains the substantial coupling of the iron-histidine vibration to the heme Soret excitation, the appearance of the iron-histidine band in the corresponding resonance Raman spectra, and a number of other experimental data, including the dependence of the iron-histidine vibrational frequency on the extent of the iron displacement out of the porphyrin plane. This dependence implies that there is an anharmonic coupling between the corresponding vibrations, which is shown to be the cause of the specific temperature dependence of the iron-histidine band. The anharmonic coupling and the dependence of the dipole transition moment of the charge transfer optical absorption band III on the iron-porphyrin distance cause the anomalous temperature and pressure dependencies of this band. It is shown that the change in both the magnitude and the distribution of the iron-porphyrin distance is expected to affect the band III intensity. Consequently, the stationarity of the band III intensity can be considered as a signature of the stationarity of the iron-porphyrin distance and its distribution in deoxyheme proteins, whereas the band III position and width could be also affected by the change in the protein electric field, caused by the protein globule dynamics.     

On electron transfer.

The tunneling transfer of electrons between two sites, appropriate to biological intermolecular electron transfer, contains physical considerations which are not important in the tunneling transfer between two metals. Analyses (such as the recent one by Hales) based on the well-known formula for the latter but applied to the former case are quantitatively and qualitatively misleading.     

The effect of iron displacement out of the porphyrin plane on the resonance Raman spectra of heme proteins and iron porphyrins.

The causes of the strong coupling of the iron-histidine vibration to the Soret resonance in the resonance Raman spectra of deoxyhemoglobin, myoglobin, and peroxidase are explored, using the vibronic theory. It is shown that the extent of the iron displacement out of the plane of the porphyrin nitrogens is the main structural parameter controlling the Fe-NHis band features, such as the dependence of its frequency and intensity on the protein conformation and number of the axial ligands, time evolution after the photolysis of the diatomic complexes of the proteins under consideration, and inverse relationship between the changes Fe-NHis and v4 porphyrin breathing mode frequencies.     

On the influence of pigment-protein interactions on the energy transfer processes in photosynthetic membrane structures. 2. LH2 complex of Rhodobacter sphaeroides

Low-temperature heterogeneous absorption and circular dichroism spectra of the Rb. sphaeroides LH2 complexes are calculated within the framework of the mini-exciton theory and diagonal static random disorder for the pure electronic transitions of the monomeric Bchl molecules. The coupling of Bchl molecules with the surrounding amino acid residues has been shown to change both the exciton distribution between the pigment molecules in each of the exciton states. The value of the delocalization index depends on the excitation wavelength and varies between 2-6 Bchl molecules. The optical transitions occurring at 780-790 and 820 nm have been found to be strongly mixed so that all Bchl molecules of the LH2 complex predetermine absorption in these spectral regions. On the other hand, absorption at 800 and 850 nm is mainly determined by the cycles of 9 and 18 Bchl molecules, respectively. Thus, the light energy absorbed by the B800 molecules at 800 nm is transferred to the B850 molecules by the interlevel exciton relaxation processes due to the population of the heavily mixed 820-nm exciton levels. The width of the heterogeneous absorption band for the cyclic monomeric aggregate has been shown to decrease as compared with the monomeric absorption band by square root(Ndel) time, where Ndel is the mean number of pigments over which the exciton is delocalized within the excited absorption band.     

藻胆素的构象变化及其对光吸收的影响

研究藻胆蛋白中藻胆素构象的变化对藻胆素光谱性质的影响,在光合作用原初过程的研究中有重要意义．由于四吡咯发色团构象的非同源性随机涨落,藻胆素的电子激发态能级呈类Boltzmann分布;藻胆素的电子－振动吸收跃迁谱带线型因子可描述为与构象随机分布因子有关的卷积形式;藻胆素构象的随机分布导致电子－振动吸收跃迁谱带的不对称增宽．     

Present status and future directions of research in electron-transfer mediated by DNA

 This commentary article presents an overview of recent experimental results on DNA-mediated electron transfer (ET) from the perspective of semiclassical ET theory. The question concerning whether or not DNA can act as a wire is addressed. Much of the article focuses on a discussion of the decay of electronic coupling (β) between electron donors and acceptors with increasing donor/acceptor separation in DNA and in protein systems. In particular, the dependence of the electronic coupling itself (H _AB) on the energy gap between the tunneling energy of the reactants and the virtual ionic states of the DNA bridge is highlighted. The article concludes by suggesting that future experimental and theoretical work in this field should focus on the tunneling gap energies of the systems studied and that special attention should be paid to systems that are likely to be in the "small tunneling gap" regime. It is these systems that are expected to exhibit enhanced electronic couplings and consequently enhanced rates of long-distance ET. Received, accepted: 5 January 1998     

A molecular mechanism of the energetic coupling of a sequence of electron transfer reactions to endergonic reactions.

A molecular mechanism of the energetic coupling of a sequence of electron transfer reactions to endergonic reactions is proposed and discussed from a physical point of view. The scheme represents a synthesis of concepts of electron transfer by tunneling and the conformational and chemiosmotic aspects of energy coupling processes. Its relation to existing experimental information and theoretical models is discussed, and further experimental tests are suggested.     

Mechanism for electron transfer within and between proteins

Examination of a growing range of electron transfer proteins is clarifying what design elements are and are not naturally selected. Intraprotein electron transfer between natural redox centers is generally engineered to be robust and resistant to mutational changes and thermal fluctuations, by using chains of redox centers connected by electron tunneling distances of 14 A or less. This assures that tunneling rates are faster than the typical millisecond bond-breaking at catalytic sites. Interprotein electron transfer addresses the potential problem of slow diffusion by designing attractive docking sites that permit a conformational search for short tunneling distances.     

Geometry for the Primary Electron Donor and the Bacteriopheophytin Acceptor in Rhodopseudomonas viridis Photosynthetic Reaction Centers

The tetrapyrrole electron donors and acceptors (bacteriochlorophyll, BCh; bacteriopheophytin, BPh) within the bacterial photosynthetic reaction center (RC) are arranged with a specific geometry that permits rapid (picosecond time scale) electron tunneling to occur between them. Here we have measured the angle between the molecular planes of the bacteriochlorophyll dimer (primary donor), B₂, and the acceptor bacteriopheophytin, H, by analyzing the dichroism of the absorption change associated with H reduction, formed by photoselection with RCs of Rhodopseudomonas viridis. This angle between molecular planes is found to be 60° ± 2. This means that the ultrafast electron tunneling must occur between donors and acceptors that are fixed by the protein to have a noncoplanar alignment. Nearly perpendicular alignments have been determined for other electron tunneling complexes involving RCs. These geometries can be contrasted with models proposed for heme-heme electron transfer complexes, which have emphasized that mutually parallel orientations should permit the most kinetically facile transfers.     

B800-->B850 energy transfer mechanism in bacterial LH2 complexes investigated by B800 pigment exchange

Femtosecond transient absorption measurements were performed on native and a series of reconstituted LH2 complexes from Rhodopseudomonas acidophila 10050 at room temperature. The reconstituted complexes contain chemically modified tetrapyrrole pigments in place of the native bacteriochlorophyll a-B800 molecules. The spectral characteristics of the modified pigments vary significantly, such that within the B800 binding sites the B800 Q(y) absorption maximum can be shifted incrementally from 800 to 670 nm. As the spectral overlap between the B800 and B850 Q(y) bands decreases, the rate of energy transfer (as determined by the time-dependent bleaching of the B850 absorption band) also decreases; the measured time constants range from 0.9 ps (bacteriochlorophyll a in the B800 sites, Q(y) absorption maximum at 800 nm) to 8.3 ps (chlorophyll a in the B800 sites, Q(y) absorption maximum at 670 nm). This correlation between energy transfer rate and spectral blue-shift of the B800 absorption band is in qualitative agreement with the trend predicted from F?rster spectral overlap calculations, although the experimentally determined rates are approximately 5 times faster than those predicted by simulations. This discrepancy is attributed to an underestimation of the electronic coupling between the B800 and B850 molecules.     

Wave packet motions coupled to electron transfer in reaction centers of Chloroflexus aurantiacus

Transient absorption difference spectroscopy with ~20 femtosecond (fs) resolution was applied to study the time and spectral evolution of low-temperature (90 K) absorbance changes in isolated reaction centers (RCs) of Chloroflexus (C.) aurantiacus. In RCs, the composition of the B-branch chromophores is different with respect to that of purple bacterial RCs by occupying the B(B) binding site of accessory bacteriochlorophyll by bacteriopheophytin molecule (Phi(B)). It was found that the nuclear wave packet motion induced on the potential energy surface of the excited state of the primary electron donor P* by ~20 fs excitation leads to a coherent formation of the states $P;{+}\Phi_{\rm B};{-}$ and $P;{+}B_{\rm A};{-}$ (B(A) is a bacteriochlorophyll monomer in the A-branch of cofactors). The processes were studied by measuring coherent oscillations in kinetics of the absorbance changes at 900 nm and 940 nm (P* stimulated emission), at 750 nm and 785 nm (Phi(B) absorption bands), and at 1,020-1028 nm ($B_{\rm A};{-}$ absorption band). In RCs, the immediate bleaching of the P band at 880 nm and the appearance of the stimulated wave packet emission at 900 nm were accompanied (with a small delay of 10-20 fs) by electron transfer from P* to the B-branch with bleaching of the Phi(B) absorption band at 785 nm due to $\Phi_{\rm B};{-}$ formation. These data are consistent with recent measurements for the mutant HM182L Rb. sphaeroides RCs (Yakovlev et al., Biochim Biophys Acta 1757:369-379, 2006). Only at a delay of 120 fs was the electron transfer from P* to the A-branch observed with a development of the $B_{\rm A};{-}$ absorption band at 1028 nm. This development was in phase with the appearance of the P* stimulated emission at 940 nm. The data on the A-branch electron transfer in C. aurantiacus RCs are consistent with those observed in native RCs of Rb. sphaeroides. The mechanism of charge separation in RCs with the modified B-branch pigment composition is discussed in terms of coupling between the nuclear wave packet motion and electron transfer from P* to Phi(B) and B(A) primary acceptors in the B-branch and A-branch, respectively.     

Study of exciton interactions in some pyrimidine dinucleotides in aqueous solution by means of absorption spectroscopy

The near ultraviolet absorption spectra of CpC, TpT and UpU in aqueous solution have been measured and compared with the corresponding spectra of C, T and U. The differences in shapes of the spectral envelopes between the monomeric and dimeric species have been interpreted in terms of exciton coupling between the bases. The largest differences were observed for the pair CpC/C in neutral solution and these were analysed by the use of vibronic coupling theory. Parameters characteristic of the relative conformation of and the rate of energy transfer between the bases in CpC were derived.     

Vibrational equilibration in absorption difference spectra of chlorophyll a.

We describe Franck-Condon simulations of vibrational cooling effects on absorption difference spectra in chlorophyll a (Chl a). The relative contributions of vibrational equilibration in the electronic ground and excited states depend on the pump and probe wavelengths. For Franck-Condon-active vibrational modes exhibiting small Huang-Rhys factors (S < 0.1, characteristic in Chl a pigments), vibrational thermalization causes essentially no spectral changes when the origin band is excited. Significant spectral evolution does occur for S < 0.1 when the 0-1 and 1.0 (hot) vibronic bands are excited. However, vibrational equilibration in these cases causes no spectral shifting in the empirical photobleaching/stimulated emission band maximum. This result bears on the interpretation of time-resolved absorption difference spectra of Chl a-containing antennae such as the Chl a/b light-harvesting peripheral antenna of photosystem II.     

Local dynamic properties of the heme pocket in native and solvent-induced molten-globule-like states of cytochrome c

We report the Soret absorption band, down to cryogenic temperature, of native and molten-globule-like state of horse heart cytochrome c. The band profile is analyzed in terms of vibronic coupling of the heme normal modes to the electronic transition in the framework of the Franck-Condon approximation. From the temperature dependence of the Gaussian broadening and of the peak position, we obtain information on the 'bath' of low frequency harmonic motions of the heme group within the heme pocket. The reported data indicate that, compared to the native state, the less rigid tertiary structure of the molten globule is reflected in a higher flexibility of the heme pocket and in greater conformational disorder, allowing the transduction of large-amplitude motion of the protein to the dynamics of the heme pocket.     

Covalently linked zinc chlorophyll dimers as a model of a chlorophyllous pair in photosynthetic reaction centers

A heterodimer, where zinc pyropheophorbide-a was linked with zinc pyropheophorbide-d through ethylene glycol diester, was prepared, as well as the corresponding homodimers. The synthetic dimers were complexed with methanol in benzene to give folded dimers by mutual Zn...O(Me)-H...O=C13(1) bonding. Such complexes had furthest red (Qy) absorption bands at longer wavelengths than the monomeric species. These red-shifts were ascribable to excitonic coupling of the Qy transition states in the chlorin pi-pi stacking conformer. In the heterodimeric system, a minor band was observed at the shorter wavelength side of the main Qy band. This observation can be explained by an additional contribution of Qy vibronic state to the exciton-coupled states. Based on the experimental results, a pair of chlorophyll(Chl)-d with Chl-a as well as a Chl-d homopair were proposed as dimers in reaction centers of Chl-d dominating cyanobacteria.     

Kinetics of electron transfer between the primary and the secondary electron acceptor in reaction centers from Rhodopseudomonas sphaeroides.

Photoreduction of the two ubiquinone molecules, UQ1 and UQ2, bound to purified reaction center from Rhodopseudomonas sphaeroides induces different absorption band shifts of bacteriochlorophyll and bacteriopheophytin molecules depending on which ubiquinone is photoreduced. This allows us to study electron transfer between UQ1 and UQ2 directly by absorption spectrometry. The results support a model in which electrons are transferred one by one from UQ1 to UQ2 with a half-time 200 micro seconds, and two by two from fully reduced UQ2 to the secondary acceptor pool.     

Local dynamics of DNA probed with optical absorption spectroscopy of bound ethidium bromide.

We have studied the local dynamics of calf thymus double-helical DNA by means of an "optical labeling" technique. The study has been performed by measuring the visible absorption band of the cationic dye ethidium bromide, both free in solution and bound to DNA, in the temperature interval 360-30 K and in two different solvent conditions. The temperature dependence of the absorption line shape has been analyzed within the framework of the vibronic coupling theory, to extract information on the dynamic properties of the system; comparison of the thermal behavior of the absorption band of free and DNA-bound ethidium bromide gave information on the local dynamics of the double helix in the proximity of the chromophore. For the dye free in solution, large spectral heterogeneity and coupling to a "bath" of low-frequency (soft) modes is observed; moreover, anharmonic motions become evident at suitably high temperatures. The average frequency of the soft modes and the amplitude of anharmonic motions depend upon solvent composition. For the DNA-bound dye, at low temperatures, heterogeneity is decreased, the average frequency of the soft modes is increased, and anharmonic motions are hindered. However, a new dynamic regime characterized by a large increase in anharmonic motions is observed at temperatures higher than approximately 280 K. The DNA double helix therefore appears to provide, at low temperatures, a rather rigid environment for the bound chromophore, in which conformational heterogeneity is reduced and low-frequency motions (both harmonic vibrations and anharmonic contributions) are hindered. The system becomes anharmonic at approximately 180 K; however, above approximately 280 K, anharmonicity starts to increase much more rapidly than for the dye free in solution; this can be attributed to the onset of wobbling of the dye in its intercalation site, which is likely connected with the onset of (functionally relevant) DNA motions, involving local opening/unwinding of the double helix. As shown by parallel measurements of the melting curves, these motions precede the melting of the double helix and depend upon solvent composition much more than does the melting itself.     

Biological electron transfer

Many oxidoreductases are constructed from (a) local sites of strongly coupled substrate-redox cofactor partners participating in exchange of electron pairs, (b) electron pair/single electron transducing redox centers, and (c) nonadiabatic, long-distance, single-electron tunneling between weakly coupled redox centers. The latter is the subject of an expanding experimental program that seeks to manipulate, test, and apply the parameters of theory. New results from the photosynthetic reaction center protein confirm that the electronic-tunneling medium appears relatively homogeneous, with any variances evident having no impact on function, and that control of intraprotein rates and directional specificity rests on a combination of distance, free energy, and reorganization energy. Interprotein electron transfer between cytochromec and the reaction center and in lactate dehydrogenase, a typical oxidoreductase from yeast, are examined. Rates of interprotein electron transfer appear to follow intraprotein guidelines with the added essential provision of binding forces to bring the cofactors of the reacting proteins into proximity.