Electrostatic control of charge separation in bacterial photosynthesis

Electrostatic interaction energies of the electron carriers with their surroundings in a photosynthetic bacterial reaction center are calculated. The calculations are based on the detailed crystal structure of reaction centers from Rhodopseu-domonas viridis, and use an iterative, self-consistent procedure to evaluate the effects of induced dipoles in the protein and the surrounding membrane. To obtain the free energies of radical-pair states, the calculated electrostatic interaction energies are combined with the experimentally measured midpoint redox potentials of the electron carriers and of bacteriochlorophyll (BChl) and bacteriopheophytin (BPh) in vitro. The P+HL- radical-pair, in which an electron has moved from the primary electron donor (P) to a BPh on the 'L' side of the reaction center (HL), is found to lie approx. 2.0 kcal/mol below the lowest excited singlet state (P*), when the radical-pair is formed in the static crystallographic structure. The reorganization energy for the subsequent relaxation of P+HL- is calculated to be 5.0 kcal/mol, so that the relaxed radical-pair lies about 7 kcal/mol below P*. The unrelaxed P+BL- radical-pair, in which the electron acceptor is the accessory BChl located between P and HL, appears to be essentially isoenergetic with P*.P+BM-, in which an electron moves to the BChl on the 'M' side, is calculated to lie about 5.5 kcal/mol above P*. These results have an estimated error range of +/- 2.5 kcal/mol. They are shown to be relatively insensitive to various details of the model, including the charge distribution in P+, the atomic charges used for the amino acid residues, the boundaries of the structural region that is considered microscopically and the treatments of the histidyl ligands of P and of potentially ionizable amino acids. The calculated free energies are consistent with rapid electron transfer from P* to HL by way of BL, and with a much slower electron transfer to the pigments on the M side. Tyrosine M208 appears to play a particularly important role in lowering the energy of P+BL-. Electrostatic interactions with the protein favor localization of the positive charge of P+ on PM, one of the two BChl molecules that make up the electron donor.     

Energy level of P+B- with respect to P* found from recombination fluorescence measurements in pheophytin-modified reaction centres.

Recent studies of reaction centres from Rhodobacter sphaeroides (R-26), in which bacteriopheophytins a were replaced by plant pheophytins a, have shown that at low temperature the excited state of primary electron donor P* is converted to the state P+B-(A) (where B(A) is a bacteriochlorophyll a monomer in branch A) which has a long lifetime (about 600 ps [8]). This allows the direct measurement of the free energy difference between P* and P+B-(A) using the temperature dependence of the recombination fluorescence from P+B-(A). The data show that P+B-(A) is located below P* by 550+/-30 mV. Thus, the primary conversion of P* leads to the formation of P+B-(A) which is below P* in energy and is a real intermediate in electron transfer.     

How does reorganization energy change upon protein unfolding? Monitoring the structural perturbations in the heme cavity of cytochrome c

In several classes of proteins the redox center provides an additional intrinsic biophysical probe that could be used to study the protein structure and function. In present report reorganization energy (lambda, as a parameter describing electron transfer properties) was used to study the protein structural changes around the heme prosthetic group in cytochrome c (cyt c). We attempted to monitor the value of this parameter upon the unfolding process of cyt c by urea, during which it was increased sigmoidally from about 0.52 to 0.82 eV for native and unfold protein, respectively. Results indicate that by structural changes in the heme site, lambda provides a complementary tool for following the unfolding process. Assuming a reversible two-state model for cyt c unfolding, Delta G(H2O), Cm and m values were determined to be 8.32+/-0.7 kcal mol(-1), 1.53+/-0.19 kcalmol(-1)M(-1) and 5.03 M, respectively.     

Comparison of the energetics of lactose active transport: artificial versus enzyme-associated energy source

To further consider the thermochemical method as a useful approach for active transport research and to investigate the characteristic of a proton electrochemical potential (delta mu H+) across the membrane, the energetics of lactose active transport across Escherichia coli membrane vesicles coupled with an artificial electron donor (phenazine methosulfate-ascorbate) has been investigated. The results were compared with those obtained with an enzyme-associated electron donor (lactate dehydrogenase-D-lactate). The oxidation of an electron donor provided the energy necessary for the transport process. The observed higher heat of ascorbate oxidation reaction in the presence of a proton ionophore (carbonyl cyanide m-chlorophenylhydrazone) further confirmed the formation of delta mu H+ across the membrane. Part of the oxidation energy was utilized to form delta mu H+. Comparison of the energetics revealed that the magnitudes of delta Hox (the enthalpy of the oxidation reaction) and delta Hm (the enthalpy of the formation of delta mu H+) in the two energy sources were comparable (-46 kcal/mol of ascorbate to -40 kcal/mol of D-lactate for delta Hox and 9.6 kcal/mol of ascorbate to 14 kcal/mol of D-lactate for delta Hm). Comparable and low value (about 1%) was also found in the free energy transfer (defined by delta Gm/delta Gox) from the oxidation reaction to the formation of delta mu H+. These results, in combination with the close values of delta mu H+ observed in the two systems, suggested that the characteristic of the created delta mu H+ was independent of the energy source. Examination of delta Hm might provide the information on the ratio of the number of protons produced, as 1 mol of two different electron donors was oxidized. The oxidation reaction in the presence of membrane vesicles was discussed.     

Membrane phospholipids and the dark side of vision

The key step in the visual pigment regeneration process is an enzyme-catalyzedtrans tocis retinoid isomerization reaction. This reaction is of substantial general interest, because it requires the input of metabolic energy. The energy is needed because the 11-cis-retinoid reaction products are approximately 4kcal/mol higher in energy than their all-trans congeners. In the retinal pigment epithelium a novel enzymatic system has been discovered which is capable of converting all-trans-retinol into all-trans retinyl esters, by means of a lecithin retinol acyl transferase (LRAT), followed by the direct processing of the ester into 11-cis-retinol. In this process the free energy of hydrolysis of a retinyl ester, estimated to be approximately –5kcal/mol, is coupled to the endothermic (+4kcal/mol) isomerization reaction, resulting in an overall exothermic process. The overall process is analogous to ATP-dependent group transfer reactions, but here the energy is provided by the membrane phospholipids. This process illustrates a new role for membranes: they can serve as an energy source.     

Thermodynamic Characteristics of Plasminogen Activation by Indirect Activators

Several indirect plasminogen (Pg) activators are known including streptokinase and the monoclonal antibody IV-Ic, whose mechanism of activation is well studied. To characterize thermodynamically the activation of Pg by streptokinase (SK) and the monoclonal antibody (mAB) IV-Ic, the activation energies were calculated for various reaction stages. Activation energy of 7.4 kcal/mol was determined for the interaction of the chromogenic substrate S-2251 with plasmin (Pm) and activated equimolar complexes Pm-SK and Pg*SK at the steady-state reaction stage, and 18.7 kcal/mol with the complexes Pg*IV-Ic. A 2.5-fold increase in the energy of activation for the Pg*IV-Ic complex suggests a more intricate mechanism of its interaction with the substrate. At the stage of increasing active center concentrations and the formation of activated complexes Pg*SK and Pg*mAB IV-Ic, the activation energy was found to be 10.5 and 38 kcal/mol, respectively. At this reaction stage the conformational rearrangement of Pg molecule with the formation of active center is the limiting stage determining the reaction rate. Unexpectedly high energy of activation at the second stage of interaction between mAB IV-Ic and Pg suggests several simultaneous reactions and complexity of conformation rearrangement in the Pg molecule in activated complexes, thus requiring large energy expense. Formation of the active center is probably accompanied by its transition within a narrow temperature range into another conformation state with the change in activation parameters of the reaction. Quantitative evaluation of the studied reactions from the perspective of thermodynamics of the enzymatic reactions gives more comprehensive characteristics of the activation mechanism.     

Biochemical characterization and electron-transfer reactions of sym1, a Rhodobacter capsulatus reaction center symmetry mutant which affects the initial electron donor.

A 51 bp section of the Rhodobacter capsulatus photosynthetic reaction center M subunit gene (nucleotides M562-M612 of the pufM structural sequence) encoding amino acids M187-M203 was replaced by the homologous region of the L subunit gene. This resulted in the symmetrization of much of the amino acid environment of the reaction center initial electron donor, P. This is the first in a series of large-scale symmetry mutations and is referred to as sym1. The sym1 mutant was able to grow photosynthetically, indicating that reaction center function was largely intact. Isolated reaction centers showed an approximately 10-nm blue shift in the QY band of P. The standard free energy change between P* and P+BphA- determined from analysis of the long-lived fluorescence from quinone-reduced reaction centers decreased from about -120 meV in the wild-type to about -75 meV in the sym1 mutant. A 65-70% quantum yield of electron transfer from P* to P+QA- was observed, most of the yield loss occurring between P* and P+BphA-. The decay of the stimulated emission from P* was about 3-fold slower in this mutant than in the wild-type. Time-resolved spectral analysis of the charge-separated intermediates formed in sym1 reaction centers indicated that the major product was P+BphA-. A model-dependent analysis of the observed rates and electron-transfer yields gave the following microscopic rate constants for sym1 reaction centers (wild-type values under the same conditions are given in parentheses): [formula: see text] Analysis of the sym1 mutant, mutants near P made by other groups, and interspecies variation of amino acids in the vicinity of P suggests that the protein asymmetry in the environment of the initial electron donor is important for optimizing the rate and yield of electron transfer, but is not strictly required for overall reaction center function.     

Role of the protein's low dielectric constant in the functioning of the photosynthetic reaction center

The high efficiency of the energy storage in the photosynthetic reaction center (RC) is determined by a successful competition of electron transfer from bacteriopheophytin to quinone, as compared to backward recombination of the primary charge-separated state. This relationship is caused by a fine matching of the reorganization energy and the free energy gap making the forward processes activationless, and hence very fast, and mismatching of these two quantities for the backreaction, therefore retarding it strongly. In this study, we show that this matching is due to a low dielectric constant of the RC's protein core because a low dielectric affects strongly electrostatic polarization components of both the reorganization energy and the equilibrium free energy of reaction. If the protein and membrane were replaced by a homogeneous medium with a high dielectric constant, the effective energy storage would be impractical.     

QM/MM study of the active site of free papain and of the NMA-papain complex.

Hybrid quantum mechanical/molecular mechanical (QM/MM) calculations using restricted and unrestricted Hartree-Fock and B3LYP ab initio (QM) and Amber force field (MM), respectively, have been applied to study the catalytic site of papain in both free and substrate bonded forms. Ab initio geometry optimizations have been performed for the active site of papain and the N-methyl-acetamide (NMA)-papain complex within the molecular mechanical treatment of the protein environment. A covalent tetrahedral intermediate structure could be obtained only when the amide N atom of the substrate molecule was protonated through a proton transfer from the His-159 in the catalytic site. Our results support the previous assumption that a proton transfer from His-159 to the amide N atom of the substrate occurs prior to or concerted with the nucleophilic attack of the Cys-25 sulfur atom to the carbonyl group of the substrate. The electron correlation effect will reduce the proton transfer barrier. Therefore, this proton transfer can be easily observed in the B3LYP/6-31G* calculations. The HF/6-31G* method overestimates the reaction barrier against this proton transfer. The sulfur atom of Cys-25 and the imidazole ring of His-159 are found to be coplanar in the free form of the enzyme. However, the rotation of the imidazole ring of His-159 was observed during the formation of the tetrahedral intermediate. Without the papain environment, the coplanar thiolate-imidazolium ion pair RS-...ImH+ is much less stable than the neutral form of RSH....Im. Within the protein environment, however, the thiolate-imidazolium ion pair becomes more stable than its neutral form by 4.1 and 0.4 kcal/mol in HF/6-31G* and B3LYP/6-31G* calculations, respectively. The barrier of proton transfer from S-H group of Cys-25 to the imidazole ring of His-159 was reduced from 22.0 kcal/mol to 15.2 kcal/mol by the protein environment in HF/6-31G* calculations. This barrier is found to be much smaller (2.5 kcal/mol) in B3LYP/6-31G* calculations.     

Nonclassical hydrophobic effect in membrane binding equilibria.

The enthalpy of transfer of four different amphiphilic molecules from the aqueous phase to the lipid membrane was determined by titration calorimetry. The four molecules investigated were the potential-sensitive dye 2-(p-toluidinyl)naphthalene-6-sulfonate (TNS), the membrane conductivity inducing anion tetraphenylborate (TPB), the Ca2+ channel blocker amlodipine [B?uerle, H. D., & Seelig, J. (1991) Biochemistry 30, 7203-7211], and the positively charged local anesthetic dibucaine. All four amphiphiles penetrate into the hydrophobic part of the membrane, and their binding constants, after correcting for electrostatic effects, range between 600 M-1 for dibucaine and 60,000 M-1 for tetraphenylborate. The corresponding changes in free energy were about -6 to -9 kcal/mol. Binding of the amphiphiles to membrane vesicles composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine was accompanied by exothermic heats of reaction for all four molecules. For TNS, TPB, and amlodipine, the enthalpies of transfer were almost identical and corresponded to delta H approximately -9 kcal/mol, essentially accounting for the total free energy change. Thus, the binding of these charged amphiphiles to the hydrophobic membrane was driven by enthalpy. This is in contrast to the classical hydrophobic effect, where the transfer is considered to be entropy driven. For dibucaine, the enthalpy of transfer was smaller with delta H approximately -2 kcal/mol but was still about one-third of the total free energy change. All enthalpies of transfer exhibited a distinct temperature dependence with molar heat capacities delta Cp of -30 to -100 cal mol-1K-1 for the transfer from water to the membrane.(ABSTRACT TRUNCATED AT 250 WORDS)     

Bovine skeletal muscle adenosine deaminase: kinetic and thermodynamic studies

Adenosine deaminase from bovine skeletal muscle catalyzes the hydrolytic deamination of adenosine to inosine and ammonia via an ordered Uni-Bi mechanism, if water is not considered as a true second substrate, as deduced from the inhibition pattern products. The inhibition constants (Ki) obtained for inosine and ammonia were 316 mumol/l and 2 mol/l, respectively. The activation energy of the reaction has been calculated as 10 kcal/mol, delta H* and delta F* as 7.9 and 15.6 kcal/mol, respectively, and delta S* as -23 cal/mol/degrees K.     

Characteristics of a lysosomal membrane transport system for tyrosine and other neutral amino acids in rat thyroid cells

Tyrosine countertransport was used to demonstrate the existence of a carrier system for neutral amino acids in the lysosomal membrane of FRTL-5 thyroid cells. In addition to tyrosine, the carrier system recognized the neutral amino acids leucine, histidine, phenylalanine, and tryptophan. Cystine and lysine, amino acids for which a lysosomal carrier system has been demonstrated, showed no competition with tyrosine for countertransport. The tyrosine system showed stereospecificity and cation independence. It did not require an acidic lysosome or the availability of free thiols. The apparent Km for tyrosine was approximately 100 microM; the energy of activation of the system was approximately 9.7 kcal/mol. This new lysosomal membrane carrier system for neutral amino acids resembles the plasma membrane L system in 3T3 Chinese hamster ovary cells and melanoma B-16 cells.     

Transfer of phosphatidylcholine between different membranes in Tetrahymena as studied by spin labeling

Transfer of phosphatidylcholine molecules between different membrane fractions of Tetrahymena pyriformis cells grown at 15, 27 and 39.5°C was studied by electron spin resonance (ESR). Microsomes were labeled densely with a phosphatidylcholine spin label and the spin-labeled microsomes were incubated with non-labeled cilia, pellicles or microsomes. The transfer of the phosphatidylcholine spin labels was measured by decrease in the exchange broadening of the electron spin resonance spectrum. In one experiment, the lipid transfer was measured between ³²P-labeled microsomes and non-labeled pellicles by use of their radioactivity. The result was in good agreement with that by ESR. The fluidity of the membrane was estimated using a fatty-acid spin label incorporated into the membranes. Transfer between lipid vesicles was also studied. The results obtained were as follows: (1) The transfer between sonicated vesicles of egg- or dipalmitoyl phosphatidylcholine occurred rapidly in the liquid crystalline phase, with an activation energy of 20 kcal/mol, whereas it hardly occurred in the solid crystalline phase. (2) The transfer rate between microsomal membranes increased with temperature, and an activation energy of the reaction was 17.8 kcal/mol. (3) The transfer from the spin-labeled microsomes to subcellular membranes of the cells grown at 15°C was larger than that to the membranes of the cells grown at 39.5°C. The membrane fluidity was larger for the cells grown at lower temperature. (4) Similar tendency was observed for the transfer between microsomal lipid vesicles prepared from the cells grown at 15°C and at 39.5°C. (5) The transfer from microsomes to various membrane fractions increased in the order, cilia < pellicles < microsomes. The order of increase in the membrane fluidity was cilia < microsomes < pellicles, although the difference between microsomes and pellicles was slight. These results indicate a crucial role of the membrane fluidity in the transfer reaction. (6) Some evidence supported the idea that the lipid transfer between these organelles occurred through the lipid exchange rather than through the fusion.     

Theoretical investigations of the hydrolysis pathway of verdoheme to biliverdin

Conversion of iron(II) verdoheme to iron biliverdin in the presence of OH(-) was investigated using B3LYP method. Both 3-21G and 6-31G* basis sets were employed for geometry optimization calculation as well as energy stabilization estimation. Calculation at 6-31G* level was found necessary for a correct spin state estimation of the iron complexes. Two possible pathways for the conversion of iron verdoheme to iron biliverdin were considered. In one path the iron was six-coordinate while in the other it was considered to be five-coordinate. In the six-coordinated pathway, the ground state of bis imidazole iron verdoheme is singlet while that for open chain iron biliverdin it is triplet state with 4.86 kcal/mol more stable than the singlet state. The potential energy surface suggests that a spin inversion take place during the course of reaction after TS. The ring opening process in the six-coordinated pathway is in overall -2.26 kcal/mol exothermic with a kinetic barrier of 9.76 kcal/mol. In the five-coordinated pathway the reactant and product are in the ground triplet state. In this path, hydroxyl ion attacks the iron center to produce a complex, which is only 1.59 kcal/mol more stable than when OH(-) directly attacks the macrocycle. The activation barrier for the conversion of iron hydroxy species to the iron biliverdin complex by a rebound mechanism is estimated to be 32.68 kcal/mol. Large barrier for rebound mechanism, small barrier of 4.18 kcal/mol for ring opening process of the hydroxylated macrocycle, and relatively same stabilities for complexes resulted by the attack of nucleophile to the iron and macrocycle indicate that five-coordinated pathway with direct attack of nucleophile to the 5-oxo position of macrocycle might be the path for the conversion of verdoheme to biliverdin.     

Theoretical Investigation of the Molecular Structure of the πκ DNA Base Pair

Abstract

The structure of the nonclassical πκ base pair (7–methyl-oxoformycin … 2,4-diaminopyrimidine) was studied at the ab initio Hartree-Fock (HF) and MP2 levels using the 6–31G* and 6–31G** basis sets. The πκ base pair is bound by three parallel hydrogen bonds with the donor-acceptor-donor recognition pattern. Recently, these bases were proposed as an extension of the genetic alphabet from four to six letters (Piccirilli et al. Nature 343, 33(1990)). By the HF/6- 31G* method with full geometry optimization we calculated the 12 degree propeller twist for the minimum energy structure of this complex. The linearity of hydrogen bonds is preserved in the twisted structure by virtue of the pyramidal arrangement of the κ-base amino groups. The rings of both the π and κ molecules remain nearly planar. This nonplanar structure of the πκ base pair is only 0.1 kcal/mol more stable than the planar (Cs) conformation. The HF/6- 31G* level gas-phase interaction energy of πκ (—13.5 kcal/mol) calculated by us turned out to be nearly the same as the interaction energy obtained previously for the adenine-thymine base pair (—13.4 kcal/mol) at the same computational level. The inclusion of p-polarization functions on hydrogens, electron correlation effects (MP2/6–31G** level), and the correction for the basis set superposition error (BSSE) increase this energy to -14.0 kcal/mol.     

Isolation, characterization, and amino acid sequences of auracyanins, blue copper proteins from the green photosynthetic bacterium Chloroflexus aurantiacus.

Three small blue copper proteins designated auracyanin A, auracyanin B-1, and auracyanin B-2 have been isolated from the thermophilic green gliding photosynthetic bacterium Chloroflexus aurantiacus. All three auracyanins are peripheral membrane proteins. Auracyanin A was described previously (Trost, J. T., McManus, J. D., Freeman, J. C., Ramakrishna, B. L., and Blankenship, R. E. (1988) Biochemistry 27, 7858-7863) and is not glycosylated. The two B forms are glycoproteins and have almost identical properties to each other, but are distinct from the A form. The sodium dodecyl sulfate-polyacrylamide gel electrophoresis apparent monomer molecular masses are 14 (A), 18 (B-2), and 22 (B-1) kDa. The amino acid sequences of the B forms are presented. All three proteins have similar absorbance, circular dichroism, and resonance Raman spectra, but the electron spin resonance signals are quite different. Laser flash photolysis kinetic analysis of the reactions of the three forms of auracyanin with lumiflavin and flavin mononucleotide semiquinones indicates that the site of electron transfer is negatively charged and has an accessibility similar to that found in other blue copper proteins. Copper analysis indicates that all three proteins contain 1 mol of copper per mol of protein. All three auracyanins exhibit a midpoint redox potential of +240 mV. Light-induced absorbance changes and electron spin resonance signals suggest that auracyanin A may play a role in photosynthetic electron transfer. Kinetic data indicate that all three proteins can donate electrons to cytochrome c-554, the electron donor to the photosynthetic reaction center.     

Carbinolamine formation and dehydration in a DNA repair enzyme active site

In order to suggest detailed mechanistic hypotheses for the formation and dehydration of a key carbinolamine intermediate in the T4 pyrimidine dimer glycosylase (T4PDG) reaction, we have investigated these reactions using steered molecular dynamics with a coupled quantum mechanics-molecular mechanics potential (QM/MM). We carried out simulations of DNA abasic site carbinolamine formation with and without a water molecule restrained to remain within the active site quantum region. We recovered potentials of mean force (PMF) from thirty replicate reaction trajectories using Jarzynski averaging. We demonstrated feasible pathways involving water, as well as those independent of water participation. The water-independent enzyme-catalyzed reaction had a bias-corrected Jarzynski-average barrier height of approximately (6.5 kcal mol(-1) (27.2 kJ mol(-1)) for the carbinolamine formation reaction and 44.5 kcal mol(-1) (186 kJ mol(-1)) for the reverse reaction at this level of representation. When the proton transfer was facilitated with an intrinsic quantum water, the barrier height was approximately 15 kcal mol(-1) (62.8 kJ mol(-1)) in the forward (formation) reaction and 19 kcal mol(-1) (79.5 kJ mol(-1)) for the reverse. In addition, two modes of unsteered (free dynamics) carbinolamine dehydration were observed: in one, the quantum water participated as an intermediate proton transfer species, and in the other, the active site protonated glutamate hydrogen was directly transferred to the carbinolamine oxygen. Water-independent unforced proton transfer from the protonated active site glutamate carboxyl to the unprotonated N-terminal amine was also observed. In summary, complex proton transfer events, some involving water intermediates, were studied in QM/MM simulations of T4PDG bound to a DNA abasic site. Imine carbinolamine formation was characterized using steered QM/MM molecular dynamics. Dehydration of the carbinolamine intermediate to form the final imine product was observed in free, unsteered, QM/MM dynamics simulations, as was unforced acid-base transfer between the active site carboxylate and the N-terminal amine.     

In vivo non-specific binding of lambda CI and Cro repressors is significant

We propose a thermodynamic model that includes the non-specific binding of the lambda phage regulatory proteins CI and Cro. By fitting the model to experimental in vivo data on activities of the two promoters P(RM) and P(R) versus concentration, we estimate the free energy upon non-specific binding to be -4.1+/-0.9 kcal/mol for CI and -4.2+/-0.8 kcal/mol for Cro. For concentrations >100 nM of CI or Cro, we find that >50% of these proteins are non-specifically bound. In particular, in a lysogen (approximately 250 CI monomeric equivalents per cell) nearly 90% of CI is non-specifically bound.     

Ultrafast transient absorption studies on Photosystem I reaction centers from Chlamydomonas reinhardtii. 1. A new interpretation of the energy trapping and early electron transfer steps in Photosystem I

The energy transfer and charge separation kinetics in core Photosystem I (PSI) particles of Chlamydomonas reinhardtii has been studied using ultrafast transient absorption in the femtosecond-to-nanosecond time range. Although the energy transfer processes in the antenna are found to be generally in good agreement with previous interpretations, we present evidence that the interpretation of the energy trapping and electron transfer processes in terms of both kinetics and mechanisms has to be revised substantially as compared to current interpretations in the literature. We resolved for the first time i), the transient difference spectrum for the excited reaction center state, and ii), the formation and decay of the primary radical pair and its intermediate spectrum directly from measurements on open PSI reaction centers. It is shown that the dominant energy trapping lifetime due to charge separation is only 6-9 ps, i.e., by a factor of 3 shorter than assumed so far. The spectrum of the first radical pair shows the expected strong bleaching band at 680 nm which decays again in the next electron transfer step. We show furthermore that the early electron transfer processes up to approximately 100 ps are more complex than assumed so far. Several possibilities are discussed for the intermediate redox states and their sequence which involve oxidation of P700 in the first electron transfer step, as assumed so far, or only in the second electron transfer step, which would represent a fundamental change from the presently assumed mechanism. To explain the data we favor the inclusion of an additional redox state in the electron transfer scheme. Thus we distinguish three different redox intermediates on the timescale up to 100 ps. At this level no final conclusion as to the exact mechanism and the nature of the intermediates can be drawn, however. From comparison of our data with fluorescence kinetics in the literature we also propose a reversible first charge separation step which has been excluded so far for open PSI reaction centers. For the first time an ultrafast 150-fs equilibration process, occurring among exciton states in the reaction center proper, upon direct excitation of the reaction center at 700 nm, has been resolved. Taken together the data call for a fundamental revision of the present understanding of the energy trapping and early electron transfer kinetics in the PSI reaction center. Due to the fact that it shows the fastest trapping time observed so far of any intact PSI particle, the PSI core of C. reinhardtii seems to be best suited to further characterize the electron transfer steps and mechanisms in the reaction center of PSI.