Steady-state and femtosecond photoinduced processes of blepharismins bound to alpha-crystallin.

The interaction of blepharismin (BP) and oxyblepharismin (OxyBP) with bovine alpha-crystallin (BAC) has been studied both by steady-state and femtosecond spectroscopy, with the aim of assessing the possible phototoxicity of these compounds toward the eye tissues. We showed that these pigments form with BAC potentially harmful ground-state complexes, the dissociation constants of which have been estimated to be 6 +/- 2 micromol L(-1) for OxyBP and 9 +/- 4 micromol L(-1) for BP. Irradiation with steady-state visible light of solutions of blepharismins in the presence of BAC proved to induce a quenching of both the pigment and the intrinsic protein fluorescences. These effects were tentatively rationalized in terms of structural changes of alpha-crystallin. On the other hand, femtosecond transient absorption spectroscopy was used to check the occurrence of any type I photoactivity of oxyblepharismin bound to alpha-crystallin. The existence of a particular type of fast photoinduced reaction, not observed in former studies with human serum albumin but present in the natural oxyblepharismin-binding protein, could here be evidenced but no specific reaction was observed during the first few nanoseconds after excitation. Partial denaturation of alpha-crystallin was however found to alter the excited-state behaviour of its complex with oxyblepharismin, making it partly resemble that of free oxyblepharismin in solution.     

Ultrafast excited-state dynamics in the green fluorescent protein variant S65T/H148D. 1. Mutagenesis and structural studies

Wild type green fluorescent protein (wt-GFP) and the variant S65T/H148D each exhibit two absorption bands, A and B, which are associated with the protonated and deprotonated chromophores, respectively. Excitation of either band leads to green emission. In wt-GFP, excitation of band A ( approximately 395 nm) leads to green emission with a rise time of 10-15 ps, due to excited-state proton transfer (ESPT) from the chromophore hydroxyl group to an acceptor. This process produces an anionic excited-state intermediate I* that subsequently emits a green photon. In the variant S65T/H148D, the A band absorbance maximum is red-shifted to approximately 415 nm, and as detailed in the accompanying papers, when the A band is excited, green fluorescence appears with a rise time shorter than the instrument time resolution ( approximately 170 fs). On the basis of the steady-state spectroscopy and high-resolution crystal structures of several variants described herein, it is proposed that in S65T/H148D, the red shift of absorption band A and the ultrafast appearance of green fluorescence upon excitation of band A are due to a very short (相似文献   

Contrasting the excited-state dynamics of the photoactive yellow protein chromophore: protein versus solvent environments

Wavelength- and time-resolved fluorescence experiments have been performed on the photoactive yellow protein, the E46Q mutant, the hybrids of these proteins containing a nonisomerizing “locked” chromophore, and the native and locked chromophores in aqueous solution. The ultrafast dynamics of these six systems is compared and spectral signatures of isomerization and solvation are discussed. We find that the ultrafast red-shifting of fluorescence is associated mostly with solvation dynamics, whereas isomerization manifests itself as quenching of fluorescence. The observed multiexponential quenching of the protein samples differs from the single-exponential lifetimes of the chromophores in solution. The locked chromophore in the protein environment decays faster than in solution. This is due to additional channels of excited-state energy dissipation via the covalent and hydrogen bonds with the protein environment. The observed large dispersion of quenching timescales observed in the protein samples that contain the native pigment favors both an inhomogeneous model and an excited-state barrier for isomerization.     

Picosecond study of energy-transfer kinetics in phycobilisomes of Synechococcus 6301 and the mutant AN 112

Excitation-energy-transfer kinetics in isolated phycobilisomes from the cyanobacterium Synechococcus 6301 (Anacystis nidulans) and the mutant AN 112 (rods containing one hexameric C-phycocyanin unit only) was investigated by picosecond absorption and fluorescence techniques. The different chromophores in the phycobilisomes were selectively excited. A lifetime component of about 10 ps was found for both C-phycocyanin and allophycocyanin in both types of phycobilisomes. We assign these signals to a transfer of excitation energy from sensitizing (‘s’) to fluorescing (‘f’) chromophores within C-phycocyanin and allophycocyanin units. A 10 ps component was also observed in the anisotropy relaxation measurements. The anisotropy decay is attributed mainly to differently oriented transition dipole moments of ‘s’- and ‘f’-chromophores and partially to ‘f’ → ‘f’ transfer. An absorption recovery signal of τ ≈ 90 ps at λ ≤ 630 nm in phycobilisomes of Synechococcus 6301 is reduced to 40–50 ps in AN 112 phycobilisomes. This is rationalized in terms of a decreased rod → core transfer time in the shorter rods of AN 112. The 40–50 ps lifetime of fluorescence and absorption recovery in AN 112 phycobilisomes is assigned mainly to a rate-limiting transfer step between C-phycocyanin and the allophycocyanin core. A decay component of allophycocyanin τ ≈ 50 ps was observed both in absorption recovery measurements and in fluorescence decay. It is assigned to energy transfer to the terminal chromophores. The final emitter(s) of the phycobilisomes from AN 112 have fluorescence lifetimes of 1.9 and 1.3 ns. We find a good correlation in the fluorescence kinetics between the decay times of phycocyanin and allophycocyanin and the fluorescence risetimes of the terminal emitters.     

Green-fluorescent protein from the bioluminescent jellyfish Clytia gregaria is an obligate dimer and does not form a stable complex with the Ca(2+)-discharged photoprotein clytin

Green-fluorescent protein (GFP) is the origin of the green bioluminescence color exhibited by several marine hydrozoans and anthozoans. The mechanism is believed to be Fo?rster resonance energy transfer (FRET) within a luciferase-GFP or photoprotein-GFP complex. As the effect is found in vitro at micromolar concentrations, for FRET to occur this complex must have an affinity in the micromolar range. We present here a fluorescence dynamics investigation of the recombinant bioluminescence proteins from the jellyfish Clytia gregaria, the photoprotein clytin in its Ca(2+)-discharged form that is highly fluorescent (λ(max) = 506 nm) and its GFP (cgreGFP; λ(max) = 500 nm). Ca(2+)-discharged clytin shows a predominant fluorescence lifetime of 5.7 ns, which is assigned to the final emitting state of the bioluminescence reaction product, coelenteramide anion, and a fluorescence anisotropy decay or rotational correlation time of 12 ns (20 °C), consistent with tight binding and rotation with the whole protein. A 34 ns correlation time combined with a translational diffusion constant and molecular brightness from fluorescence fluctuation spectroscopy all confirm that cgreGFP is an obligate dimer down to nanomolar concentrations. Within the dimer, the two chromophores have a coupled excited-state transition yielding fluorescence depolarization via FRET with a transfer correlation time of 0.5 ns. The 34 ns time of cgreGFP showed no change upon addition of a 1000-fold excess of Ca(2+)-discharged clytin, indicating no stable complexation below 0.2 mM. It is proposed that any bioluminescence FRET complex with micromolar affinity must be one formed transiently by the cgreGFP dimer with a short-lived (millisecond) intermediate in the clytin reaction pathway.     

Early molecular events in the photoactive yellow protein: role of the chromophore photophysics.

We report a comparative study of the isomerization reaction in native and denatured photoactive yellow protein (PYP) and in various chromophore analogues in their trans deprotonated form. The excited-state relaxation dynamics was followed by subpicosecond transient absorption and gain spectroscopy. The free p-hydroxycinnamate (pCA(2-)) and its amide analogue (pCM(-)) are found to display a quite different transient spectroscopy from that of PYP. The excited-state deactivation leads to the formation of the ground-state cis isomer without any detectable intermediate with a mechanism comparable to trans-stilbene photoisomerization. On the contrary, the early stage of the excited-state deactivation of the free thiophenyl-p-hydroxycinnamate (pCT(-)) and of the denatured PYP is similar to that of the native protein. It involves the formation of an intermediate absorbing in the spectral region located between the bleaching and gain bands in less than 2 ps. However, in these two cases, the formation of the cis isomer has not been proved yet. This difference with pCA(-) and pCM(-) might result from the fact that, in the thioester substituted chromophore, simultaneous population of two quasi-degenerate excited states occurs upon excitation. This comparative study highlights the determining role of the chromophore structure and of its intrinsic properties in the primary molecular events in native PYP.     

Ultrafast electron transfer in the complex between fluorescein and a cognate engineered lipocalin protein, a so-called anticalin

Anticalins are a novel class of engineered ligand-binding proteins with tailored specificities derived from the lipocalin scaffold. The anticalin FluA complexes fluorescein as ligand with high affinity, and it effects almost complete quenching of its steady-state fluorescence. To study the underlying mechanism, we have applied femtosecond absorption spectroscopy, which revealed excited-state electron transfer within the FluA*Fl complex to be responsible for the strong fluorescence quenching. On the basis of a comparison of redox potentials, either tryptophan or tyrosine may serve as electron donor to the bound fluorescein group in its excited singlet state, thus forming the fluorescein trianion radical within 400 fs. The almost monoexponential rate points to a single, well-defined binding site, and its temperature independence suggests an (almost) activationless process. Applying conventional electron transfer theory to the ultrafast forward and slower back-rates, the resulting electronic interaction is rather large, with approximately 140 cm(-1) for tyrosine, which would be consistent with a coplanar arrangement of both aromatic moieties within van der Waals distance. The weak residual steady-state fluorescence originates from a small (approximately 10%) component with a time constant in the 40-60 ps range. These results demonstrate the power of time-resolved absorption spectroscopy as a diagnostic tool for the elucidation of a fluorescence quenching mechanism and the temporal profiles of the processes involved. The high structural and dynamic definition of the complexation site suggests the anticalin FluA to be a promising model in order to tailor and probe electronic interactions and energetics in proteins.     

Ultrafast carotenoid-to-chlorophyll singlet energy transfer in the cytochrome b6f complex from Bryopsis corticulans

Ultrafast carotenoid-to-chlorophyll (Car-to-Chl) singlet excitation energy transfer in the cytochrome b(6)f (Cyt b(6)f) complex from Bryopsis corticulans is investigated by the use of femtosecond time-resolved absorption spectroscopy. For all-trans-alpha-carotene free in n-hexane, the lifetimes of the two low-lying singlet excited states, S(1)(2A(g)(-)) and S(2)(1B(u)(+)), are determined to be 14.3 +/- 0.4 ps and 230 +/- 10 fs, respectively. For the Cyt b(6)f complex, to which 9-cis-alpha-carotene is bound, the lifetime of the S(1)(2A(g)(-)) state remains unchanged, whereas that of the S(2)(1B(u)(+)) state is significantly reduced. In addition, a decay-to-rise correlation between the excited-state dynamics of alpha-carotene and Chl a is clearly observed. This spectroscopic evidence proves that the S(2)(1B(u)(+)) state is able to transfer electronic excitations to the Q(x) state of Chl a, whereas the S(1)(2A(g)(-)) state remains inactive. The time constant and the partial efficiency of the energy transfer are determined to be 240 +/- 40 fs and (49 +/- 4)%, respectively, which supports the overall efficiency of 24% determined with steady-state fluorescence spectroscopy. A scheme of the alpha-carotene-to-Chl a singlet energy transfer is proposed based on the excited-state dynamics of the pigments.     

Energy transfer kinetics of phycoerythrocyanin trimer from cyanobacteriumAnabaena variabilis (II)

The excitation energy transfer processes in trimeric PEC have been studied by using steady-state and time-resolved fluorescence spectra techniques in detail. The results indicate that the energy transfer processes should take place between α₈₄-PVB and β₈₄-or β₁₅₅-PCB chromophores with the time constants 34.7 ps and 175–200 ps individually; in contrast with monomeric PEC, from time-resolved fluorescence anisotropic spectrum technique, the decay constant of 45 ps which was assigned to the energy transfer time among three β₈₄-PCB chromophores was observed and the energy levels of β₈₄-and/or β₁₅₅-PCB chromophores were confirmed to turn over in trimeric PEC.     

Femtosecond kinetics of photoconversion of the higher plant photoreceptor phytochrome carrying native and modified chromophores

The photoprocesses of native (phyA of oat), and of C-terminally truncated recombinant phytochromes, assembled instead of the native phytochromobilin with phycocyanobilin (PCB-65 kDa-phy) and iso-phycocyanobilin (iso-PCB-65 kDa-phy) chromophores, have been studied by femtosecond transient absorption spectroscopy in both their red absorbing phytochrome (P_r) and far-red absorbing phytochrome (P_fr) forms. Native P_r phytochrome shows an excitation wavelength dependence of the kinetics with three main picosecond components. The formation kinetics of the first ground-state intermediate I₇₀₀, absorbing at ∼690 nm, is mainly described by 28 ps or 40 ps components in native and PCB phytochrome, respectively, whereas additional ∼15 and 50 ps components describe conformational dynamics and equilibria among different local minima on the excited-state hypersurface. No significant amount of I₇₀₀ formation can be observed on our timescale for iso-PCB phytochrome. We suggest that iso-PCB-65 kDa-phy either interacts with the protein differently leading to a more twisted and/or less protonated configuration, or undergoes P_r to P_fr isomerization primarily via a different configurational pathway, largely circumventing I₇₀₀ as an intermediate. The isomerization process is accompanied by strong coherent oscillations due to wavepacket motion on the excited-state surface for both phytochrome forms. The femto- to (sub-)nanosecond kinetics of the P_fr forms is again quite similar for the native and the PCB phytochromes. After an ultrafast excited-state relaxation within ∼150 fs, the chromophores return to the first ground-state intermediate in 400-800 fs followed by two additional ground-state intermediates which are formed with 2-3 ps and ∼400 ps lifetimes. We call the first ground-state intermediate in native phytochrome I_fr·750, due to its pronounced absorption at that wavelength. The other intermediates are termed I_fr·675 and pseudo-P_r. The absorption spectrum of the latter already closely resembles the absorption of the P_r chromophore. PCB-65 kDa-phy shows a very similar kinetics, although many of the detailed spectral features in the transients seen in native phy are blurred, presumably due to wider inhomogeneous distribution of the chromophore conformation. Iso-PCB-65 kDa-phy shows similar features to the PCB-65 kDa-phy, with some additional blue-shift of the transient spectra of ∼10 nm. The sub-200 fs component is, however, absent, and the picosecond lifetimes are somewhat longer than in 124 kDa phytochrome or in PCB-65 kDa-phy. We interpret the data within the framework of two- and three-dimensional potential energy surface diagrams for the photoisomerization processes and the ground-state intermediates involved in the two photoconversions.     

Redox effects on the excited-state lifetime in chlorosomes and bacteriochlorophyll c oligomers.

Oligomers of [E,E] BChl CF (8, 12-diethyl bacteriochlorophyll c esterified with farnesol (F)) and [Pr,E] BChl CF (analogously, M methyl, Pr propyl) in hexane and aqueous detergent or lipid micelles were studied by means of steady-state absorption, time-resolved fluorescence, and electron spin resonance spectroscopy. The maximum absorption wavelength, excited-state dynamics, and electron spin resonance (EPR) linewidths are similar to those of native and reconstituted chlorosomes of Chlorobium tepidum. The maximum absorption wavelength of oligomers of [E,E] BChl CF was consistently blue-shifted as compared to that of [Pr,E] BChl CF oligomers, which is ascribed to the formation of smaller oligomers with [E,E] BChl CF than [Pr,E] BChl CF. Time-resolved fluorescence measurements show an excited-state lifetime of 10 ps or less in nonreduced samples of native and reconstituted chlorosomes of Chlorobium tepidum. Under reduced conditions the excited-state lifetime increased to tens of picoseconds, and energy transfer to BChl a or long-wavelength absorbing BChl c was observed. Oligomers of [E,E] BChl CF and [Pr,E] BChl CF in aqueous detergent or lipid micelles show a similar short excited-state lifetime under nonreduced conditions and an increase up to several tens of picoseconds upon reduction. These results indicate rapid quenching of excitation energy in nonreduced samples of chlorosomes and aqueous BChl c oligomers. EPR spectroscopy shows that traces of oxidized BChl c radicals are present in nonreduced and absent in reduced samples of chlorosomes and BChl c oligomers. This suggests that the observed short excited-state lifetimes in nonreduced samples of chlorosomes and BChl c oligomers may be ascribed to excited-state quenching by BChl c radicals. The narrow EPR linewidth suggests that the BChl c are arranged in clusters of 16 and 6 molecules in chlorosomes of Chlorobium tepidum and Chloroflexus aurantiacus, respectively.     

Spectroscopic Studies of the Supramolecular Interactions Between Uracil and 5-Hydroxy-6-Methyluracil with Bovine Serum Albumin and its Bilirubin Complex

Using fluorescence and absorption spectroscopy the interaction of bovine serum albumin and its bilirubin complex with uracil and 5-hydroxy-6-methyluracil in phosphate buffer at pH 7.4 was investigated. The parameters of forming intermolecular complexes (binding constants, quenching rate constants, the radius of the quenching sphere and etc.) were determined. The interaction between serum albumin and uracils is carried out by the static quenching of protein fluorescence and has predominantly hydrophobic character. Using synchronous fluorescence spectroscopy the influence of uracil and 5-hydroxy-6-methyluracil on the conformational changes of the protein molecule was studied. Uracils effectively binds to bilirubin-albumin complex compared to free protein, which is caused by the interaction with tetrapyrrolic pigment in macromolecular complex. Molecular docking calculations also being presented.     

Photoisomerization in Rhodopsin

This article reviews the primary reaction processes in rhodopsin, a photoreceptive pigment for twilight vision. Rhodopsin has an 11-cis retinal as the chromophore, which binds covalently with a lysine residue through a protonated Schiff base linkage. Absorption of a photon by rhodopsin initiates the primary photochemical reaction in the chromophore. Picosecond time-resolved spectroscopy of 11-cis locked rhodopsin analogs revealed that the cis-trans isomerization of the chromophore is the primary reaction in rhodopsin. Then, generation of femtosecond laser pulses in the 1990s made it possible to follow the process of isomerization in real time. Formation of photorhodopsin within 200 fsec was observed by a transient absorption (pump–probe) experiment, which also revealed that the photoisomerization in rhodopsin is a vibrationally coherent process. Femtosecond fluorescence spectroscopy directly captured excited-state dynamics of rhodopsin, so that both coherent reaction process and unreacted excited state were observed. Faster photoreaction of the chromophore in rhodopsin than that in solution implies that the protein environment facilitates the efficient isomerization process. Such contributions of the protein residues have been monitored by infrared spectroscopy of rhodopsin, bathorhodopsin, and isorhodopsin (9-cis rhodopsin) at low temperatures. The crystal structure of bovine rhodopsin recently reported will lead to better understanding of the mechanism in future.     

The photophysics of green fluorescent protein: influence of the key amino acids at positions 65, 203, and 222

The three amino acids S65, T203, and E222 crucially determine the photophysical behavior of wild-type green fluorescent protein. We investigate the impact of four point mutations at these positions and their respective combinations on green fluorescent protein's photophysics using absorption spectroscopy, as well as steady-state and time-resolved fluorescence spectroscopy. Our results highlight the influence of the protein's hydrogen-bonding network on the equilibrium between the different chromophore states and on the efficiency of the excited-state proton transfer. The mutagenic approach allows us to separate different mechanisms responsible for fluorescence quenching, some of which were previously discussed theoretically. Our results will be useful for the development of new strategies for the generation of autofluorescent proteins with specific photophysical properties. One example presented here is a variant exhibiting uncommon blue fluorescence.     

水葫芦及菠菜光合作用原初光反应的超快光谱研究

采用相同的分离技术,从水葫芦(Eichhornia crassipes(Mart)Solms.)和菠菜(Spinacia oleracea L.)叶片中提取叶绿体.利用吸收光谱和低温荧光光谱及皮秒荧光单光子计数技术对它们的光谱性质和光系统Ⅱ荧光寿命进行了研究.这两种叶绿体吸收光谱相似,暗示着它们都能高效吸收不同波长的光子.低温荧光光谱显示,水葫芦叶绿体两个光系统之间激发能分配平衡状态差,表明不利于该植物叶绿体高效利用吸收的光子能.采用三指数动力学模型对测定的光系统Ⅱ荧光衰减曲线拟合,水葫芦叶绿体光系统Ⅱ荧光衰减寿命分别是:138,521和1 494 ps;菠菜叶绿体荧光寿命分别是:197,465和1 459ps.并且归属了荧光组分,慢速度荧光衰减是由叶绿素堆积造成的,中等速度荧光衰减源于PSⅡ反应中心重新结合电荷组分,快速度荧光衰减归属于PSⅡ反应中心组分.基于20ps模型计算的水葫芦和菠菜叶绿体PSⅡ反应中心激发能转能效率分别是87%和91%.该结果与转能效率为100%的观点不一致.实验结果支持PSⅡ反应中心电荷分裂20 ps时间常数模型.根据转能效率,水葫芦生长速度不大于菠菜生长速度,但是,水葫芦叶绿体中含有丰富的胡萝卜素成分,其单位质量叶绿体吸收光能大于单位质量菠菜叶绿体吸收的量.实验结果还暗示植物叶绿体体系传能高效,接近于100%.     

Energy transfer kinetics of phycoerythrocyanin trimer from cyanobacterium Anabaena variabilis (II)

The excitation energy transfer processes in trimeric PEC have been studied by using steady-state and time-resolved fluorescence spectra techniques in detail. The results indicate that the energy transfer processes should take place between α₈₄-PVB and β₈₄-or β₁₅₅-PCB chromophores with the time constants 34.7 ps and 175–200 ps individually; in contrast with monomeric PEC, from time-resolved fluorescence anisotropic spectrum technique, the decay constant of 45 ps which was assigned to the energy transfer time among three β₈₄-PCB chromophores was observed and the energy levels of β₈₄-and/or β₁₅₅-PCB chromophores were confirmed to turn over in trimeric PEC. Project supported by the National Natural Science Foundation of China (Grant No. 39670065).     

Picosecond time-resolved fluorescence study of chlorophyll organisation and excitation energy distribution in chloroplasts from wild-type barley and a mutant lacking chlorophyll b.

Picosecond time-resolved fluorescence spectroscopy has been used to investigate the fluorescence emission from wild-type barley chloroplasts and from chloroplasts of the barley mutant, chlorina f-2, which lacks the light-harvesting chlorophyll a/b-protein complex. Cation-controlled regulation of the distribution of excitation energy was studied in isolated chloroplasts at the Fo and Fm levels. It was found that: (a) The fluorescence decay curves were distinctly non-exponential, even at low excitation intensities (less than 2 x 10(14) photons . cm(-2). (b) The fluorescence decay curves could, however, be described by a dual exponential decay law. The wild-type barley chloroplasts gave a short-lived fluorescence component of approximately 140 ps and a long-lived component of 600 ps (Fo) or 1300 ps (Fm) in the presence of Mg2+; in comparison, the mutant barley yielded a short-lived fluorescence component of approx. 50 ps and a long-lived component of 194 ps (Fo) and 424 ps (Fm). (c) The absence of the light-harvesting chlorophyll a/b-protein complex in the mutant results in a low fluorescence quantum yield which is unaffected by the cation composition of the medium. (d) The fluorescence yield changes seen in steady-state experiments on closing Photosystem II reaction centres (Fm/Fo) or on the addition of MgCl2 (+Mg2+/-Mg2+) were in overall agreement with those calculated from the time-resolved fluorescence measurements. The results suggest that the short-lived fluorescence component is partly attributable to the chlorophyll a antenna of Photosystem I, and, in part, to those light-harvesting-Photosystem II pigment combinations which are strongly coupled to the Photosystem I antenna chlorophyll. The long-lived fluorescence component can be ascribed to the light-harvesting-Photosystem II pigment combinations not coupled with the antenna of Photosystem I. In the case of the mutant, the two components appear to be the separate emissions from the Photosystem I and Photosystem II antenna chlorophylls.     

Ultrafast energy transfer pathways in R-phycoerythrin from Polysiphonia urceolata

Energy transfer (ET) processes between chromophores in R-phycoerythrin (R-PE) from Polysiphonia urceolata were studied by use of ultrafast spectroscopic methods. Several primary ET pathways were elaborated. A fluorescence decay component with a time constant of several hundred picoseconds observed by streak camera is tentatively assigned to the reversible formation of exciton traps between α84 and β84 pigment pairs. In order to investigate much faster ET processes in R-PE, a noncollinear optical parametric amplifier based femtosecond time-resolved transient fluorescence spectrometer was employed. The results reveal that the ET between α84 and β84 pigment pair has a time constant of 1-2?ps; the energy migration between α84 and β84 pairs within the R-PE trimer has a time constant of 30-40?ps. We also demonstrated an ET process from phycourobilin to phycoerythrobilin with a time constant as fast as 2.5-3.0?ps, which was directly observed in fluorescence kinetics by selective excitation of the phycourobilin molecules acting as the energy donor.     

Determination of the excitation migration time in Photosystem II consequences for the membrane organization and charge separation parameters

The fluorescence decay kinetics of Photosystem II (PSII) membranes from spinach with open reaction centers (RCs), were compared after exciting at 420 and 484 nm. These wavelengths lead to preferential excitation of chlorophyll (Chl) a and Chl b, respectively, which causes different initial excited-state populations in the inner and outer antenna system. The non-exponential fluorescence decay appears to be 4.3+/-1.8 ps slower upon 484 nm excitation for preparations that contain on average 2.45 LHCII (light-harvesting complex II) trimers per reaction center. Using a recently introduced coarse-grained model it can be concluded that the average migration time of an electronic excitation towards the RC contributes approximately 23% to the overall average trapping time. The migration time appears to be approximately two times faster than expected based on previous ultrafast transient absorption and fluorescence measurements. It is concluded that excitation energy transfer in PSII follows specific energy transfer pathways that require an optimized organization of the antenna complexes with respect to each other. Within the context of the coarse-grained model it can be calculated that the rate of primary charge separation of the RC is (5.5+/-0.4 ps)(-1), the rate of secondary charge separation is (137+/-5 ps)(-1) and the drop in free energy upon primary charge separation is 826+/-30 cm(-1). These parameters are in rather good agreement with recently published results on isolated core complexes [Y. Miloslavina, M. Szczepaniak, M.G. Muller, J. Sander, M. Nowaczyk, M. R?gner, A.R. Holzwarth, Charge separation kinetics in intact Photosystem II core particles is trap-limited. A picosecond fluorescence study, Biochemistry 45 (2006) 2436-2442].