Formation of kinetically trapped nanoscopic unilamellar vesicles from metastable nanodiscs

Zwitterionic long-chain lipids (e.g., dimyristoyl phosphatidylcholine, DMPC) spontaneously form onion-like, thermodynamically stable structures in aqueous solutions (commonly known as multilamellar vesicles, or MLVs). It has also been reported that the addition of zwitterionic short-chain (i.e., dihexanoyl phosphatidylcholine, DHPC) and charged long-chain (i.e., dimyristoyl phosphatidylglycerol, DMPG) lipids to zwitterionic long-chain lipid solutions results in the formation of unilamellar vesicles (ULVs). Here, we report a kinetic study on lipid mixtures composed of DMPC, DHPC, and DMPG. Two membrane charge densities (i.e., [DMPG]/[DMPC] = 0.01 and 0.001) and two solution salinities (i.e., [NaCl] = 0 and 0.2 M) are investigated. Upon dilution of the high-concentration samples at 50 °C, thermodynamically stable MLVs are formed, in the case of both weakly charged and high salinity solution mixtures, implying that the electrostatic interactions between bilayers are insufficient to cause MLVs to unbind. Importantly, in the case of these samples small angle neutron scattering (SANS) data show that, initially, nanodiscs (also known as bicelles) or bilayered ribbons form at low temperatures (i.e., 10 °C), but transform into uniform size, nanoscopic ULVs after incubation at 10 °C for 20 h, indicating that the nanodisc is a metastable structure. The instability of nanodiscs may be attributed to low membrane rigidity due to a reduced charge density and high salinity. Moreover, the uniform-sized ULVs persist even after being heated to 50 °C, where thermodynamically stable MLVs are observed. This result clearly demonstrates that these ULVs are kinetically trapped, and that the mechanical properties (e.g., bending rigidity) of 10 °C nanodiscs favor the formation of nanoscopic ULVs over that of MLVs. From a practical point of view, this method of forming uniform-sized ULVs may lend itself to their mass production, thus making them economically feasible for medical applications that depend on monodisperse lipid-based systems for therapeutic and diagnostic purposes.     

Characterizing the Structure and Photocycle of PR 2D Crystals with CD and FTIR Spectroscopy†

We present here a study on proteorhodopsin (PR) 2D crystals with analytical ultracentrifugation, circular dichroism and Fourier transform infrared (FTIR) spectroscopy. The aim of our experiments was to test the activity of 2D crystal sample preparations and to gain further insight in PR structure, stability and function with these techniques. Our results demonstrate higher stability compared to detergent‐solubilized or reconstituted samples. For different pH values, low pH 2D crystals tend to form bigger aggregates and are less stable than at basic pH. The pH 9 sample shows a sharp phase transition during heat denaturation and there is also evidence for protein–protein interaction due to the close proximity of the proteins in the 2D crystals. In the FTIR measurements at cryogenic temperatures (77 K), we characterized the first step in the PR photocycle. At pH 9, the K intermediate could be observed and the samples showed no orientation effects. At pH 5, we could trap the K/L intermediate, characterized by its negative IR signal at 1741 cm^?1. In rapid‐scan FTIR experiments, we could also identify the M intermediate of the photocycle at basic pH. We conclude that the PR 2D crystals exhibit a fully functional photocycle and are therefore well suited for further studies on the proton transport mechanism of PR.     

His75-Asp97 cluster in green proteorhodopsin

The proteorhodopsin (PR) family found in bacteria near the ocean's surface consists of hundreds of PR variants color-tuned to their environment. PR contains a highly conserved single histidine at position 75, which is not found in most other retinal proteins. Using (13)C and (15)N MAS NMR, we were able to prove for green PR that His75 forms a pH-dependent H-bond with the primary proton acceptor Asp97, which explains its unusually high pK(a). The functional role of His75 has been studied using site-directed mutagenesis and time-resolved optical spectroscopy: Ultrafast vis-pump/vis-probe experiments on PR(H75N) showed that the primary reaction dynamics is retained, while flash photolysis experiments revealed an accelerated photocycle. Our data show the formation of a pH-dependent His-Asp cluster which might be typical for eubacterial retinal proteins. Despite its stabilizing function, His75 was found to slow the photocycle in wild-type PR. This means that PR was not optimized by evolution for fast proton transfer, which raises questions about its true function in vivo.     

pH-dependent transitions in xanthorhodopsin

Xanthorhodopsin (XR), the light-driven proton pump of the halophilic eubacterium Salinibacter ruber, exhibits substantial homology to bacteriorhodopsin (BR) of archaea and proteorhodopsin (PR) of marine bacteria, but unlike them contains a light-harvesting carotenoid antenna, salinixanthin, as well as retinal. We report here the pH-dependent properties of XR. The pKa of the retinal Schiff base is as high as in BR, i.e. > or =12.4. Deprotonation of the Schiff base and the ensuing alkaline denaturation cause large changes in the absorption bands of the carotenoid antenna, which lose intensity and become broader, making the spectrum similar to that of salinixanthin not bound to XR. A small redshift of the retinal chromophore band and increase of its extinction, as well as the pH-dependent amplitude of the M intermediate indicate that in detergent-solubilized XR the pKa of the Schiff base counterion and proton acceptor is about 6 (compared to 2.6 in BR, and 7.5 in PR). The protonation of the counterion is accompanied by a small blueshift of the carotenoid absorption bands. The pigment is stable in the dark upon acidification to pH 2. At pH < 2 a transition to a blueshifted species absorbing around 440 nm occurs, accompanied by loss of resolution of the carotenoid absorption bands. At pH < 3 illumination of XR with continuous light causes accumulation of long-lived photoproduct(s) with an absorption maximum around 400 nm. The photocycle of XR was examined between pH 4 and 10 in solubilized samples. The pH dependence of recovery of the initial state slows at both acid and alkaline pH, with pKas of 6.0 and 9.3. The decrease in the rates with pKa 6.0 is apparently caused by protonation of the counterion and proton acceptor, and that at high pH reflects the pKa of the internal proton donor, Glu94, at the times in the photocycle when this group equilibrates with the bulk.     

Accurate Prediction of Absorption Spectral Shifts of Proteorhodopsin Using a Fragment-Based Quantum Mechanical Method

Many experiments have been carried out to display different colors of Proteorhodopsin (PR) and its mutants, but the mechanism of color tuning of PR was not fully elucidated. In this study, we applied the Electrostatically Embedded Generalized Molecular Fractionation with Conjugate Caps (EE-GMFCC) method to the prediction of excitation energies of PRs. Excitation energies of 10 variants of Blue Proteorhodopsin (BPR-PR105Q) in residue 105GLN were calculated with the EE-GMFCC method at the TD-B3LYP/6-31G* level. The calculated results show good correlation with the experimental values of absorption wavelengths, although the experimental wavelength range among these systems is less than 50 nm. The ensemble-averaged electric fields along the polyene chain of retinal correlated well with EE-GMFCC calculated excitation energies for these 10 PRs, suggesting that electrostatic interactions from nearby residues are responsible for the color tuning. We also utilized the GMFCC method to decompose the excitation energy contribution per residue surrounding the chromophore. Our results show that residues ASP97 and ASP227 have the largest contribution to the absorption spectral shift of PR among the nearby residues of retinal. This work demonstrates that the EE-GMFCC method can be applied to accurately predict the absorption spectral shifts for biomacromolecules.     

Near‐Infrared Phosphorus‐Substituted Rhodamine with Emission Wavelength above 700 nm for Bioimaging

Phosphorus has been successfully fused into a classic rhodamine framework, in which it replaces the bridging oxygen atom to give a series of phosphorus‐substituted rhodamines (PRs). Because of the electron‐accepting properties of the phosphorus moiety, which is due to effective σ*–π* interactions and strengthened by the inductivity of phosphine oxide, PR exhibits extraordinary long‐wavelength fluorescence emission, elongating to the region above 700 nm, with bathochromic shifts of 140 and 40 nm relative to rhodamine and silicon‐substituted rhodamine, respectively. Other advantageous properties of the rhodamine family, including high molar extinction coefficient, considerable quantum efficiency, high water solubility, pH‐independent emission, great tolerance to photobleaching, and low cytotoxicity, stay intact in PR. Given these excellent properties, PR is desirable for NIR‐fluorescence imaging in vivo.     

Low-temperature spectroscopy of Met100Ala mutant of photoactive yellow protein

The trans-to-cis photoisomerization of the p-coumaroyl chromophore of photoactive yellow protein (PYP) triggers the photocycle. Met100, which is located in the vicinity of the chromophore, is a key residue for the cis-to-trans back-isomerization of the chromophore, which is a rate-determining reaction of the PYP photocycle. Here we characterized the photocycle of the Met100Ala mutant of PYP (M100A) by low temperature UV-visible spectroscopy. Irradiation of M100A at 80 K yielded a 380 nm species (M100A(BL)), while the corresponding intermediate of wild type (WT; PYP(BL)) is formed above 90 K. The amounts of redshifted intermediates produced from M100A (M100A(B') and M100A(L)) were substantially less than those from WT. While the near-UV intermediate (PYP(M)) is not formed from WT in glycerol samples at low temperature, M100A(M) was clearly observed above 190 K. These alterations of the photocycle of M100A were explained by the shift in the equilibrium between the intermediates. The carbonyl oxygen of the thioester linkage of the cis-chromophore in the photocycle intermediates is close to the phenyl ring of Phe96 (<3.5 A), which would be displaced by the mutation of Met100. These findings imply that the interaction between chromophore and amino acid residues near Met100 is altered during the early stage of the PYP photocycle.     

The influence of water on the photochemical reaction cycle of proteorhodopsin at low and high pH

Dried samples were prepared from suspension of proteorhodopsin. With HCl and NaOH the pH of the samples was adjusted below and above the pKa of the proton acceptor Asp-97, which was established earlier to be 7.1. Both types of samples were photoactive, and exhibited a truncated photocycle, compared to that measured in suspension. The photocycle of the low pH sample had a K like red shifted intermediate, decaying through an energized PR' intermediate to the ground state protein. The high pH sample had a more complex photocycle in which beside of the red shifted intermediate an M like intermediate could be identified, having a deprotonated Schiff-base. This blue shifted intermediate decays through an intermediate we designated PR', which is spectrally identical to the unphotolysed ground state. The humidity and temperature dependence of the photocycle in both cases was studied to understand the role of water in the function of the proteorhodopsin. The effects measured on proteorhodopsin were very similar to that measured earlier on bacteriorhodopsin.     

Proton transfer and associated molecular rearrangements in the photocycle of photoactive yellow protein: role of water molecular migration on the proton transfer reaction

The mechanism of the proton transfer and the concomitant molecular structural and hydrogen bond rearrangements after the photoisomerization of the chromophore in the photocycle of photoactive yellow protein are theoretically investigated by using the QM/MM method and molecular dynamics calculations. The free energy surface along this proton-transfer process is determined. This work suggests the important role of the water molecular migration into the moiety of chromophore, which facilitates proton transfer by the hydrogen bond rearrangement and the hydration of the pB' state.     

Photoisomerization in proteorhodopsin mutant D97N

The first steps of the photocycle of the D97N mutant of proteorhodopsin (PR) have been investigated by means of ultrafast transient absorption spectroscopy. A comparison with the primary dynamics of native PR and D85N mutant of bacteriorhodopsin is given. Upon photoexcitation of the covalently bound all-trans retinal the excited state decays biexponentially with time constants of 1.4 and 20 ps via a conical intersection, resulting in a 13-cis isomerized retinal. Neither of the two-deactivation channels is significantly preferred. The dynamics is slowed down in comparison with native PR at pH 9 and reaction rates are even lower than for native PR at pH 6, where the primary proton acceptor (Asp97) is protonated. Therefore, the ultrafast isomerization is not only controlled by the charge distribution within the retinal binding pocket. This study shows that in addition to direct electrostatics other effects have to be taken into account to explain the catalytic function of Asp97 in PR on the ultrafast isomerization reaction. This may include sterical interactions and/or bound water molecules within the retinal binding pocket.     

Initial photoinduced dynamics of the photoactive yellow protein.

The photoactive yellow protein (PYP) is the photoreceptor protein responsible for initiating the blue-light repellent response of the Halorhodospira halophila bacterium. Optical excitation of the intrinsic chromophore in PYP, p-coumaric acid, leads to the initiation of a photocycle that comprises several distinct intermediates. The dynamical processes responsible for the initiation of the PYP photocycle have been explored with several time-resolved techniques, which include ultrafast electronic and vibrational spectroscopies. Ultrafast electronic spectroscopies, such as pump-visible probe, pump-dump-visible probe, and fluorescence upconversion, are useful in identifying the timescales and connectivity of the transient intermediates, while ultrafast vibrational spectroscopies link these intermediates to dynamic structures. Herein, we present the use of these techniques for exploring the initial dynamics of PYP, and show how these techniques provide the basis for understanding the complex relationship between protein and chromophore, which ultimately results in biological function.     

Photoisomerization and proton transfer in photoactive yellow protein

The photoactive yellow protein (PYP) is a bacterial photosensor containing a para-coumaryl thioester chromophore that absorbs blue light, initiating a photocycle involving a series of conformational changes. Here, we present computational studies to resolve uncertainties and controversies concerning the correspondence between atomic structures and spectroscopic measurements on early photocycle intermediates. The initial nanoseconds of the PYP photocycle are examined using time-dependent density functional theory (TDDFT) to calculate the energy profiles for chromophore photoisomerization and proton transfer, and to calculate excitation energies to identify photocycle intermediates. The calculated potential energy surface for photoisomerization matches key, experimentally determined, spectral parameters. The calculated excitation energy of the photocycle intermediate cryogenically trapped in a crystal structure by Genick et al. [Genick, U. K.; Soltis, S. M.; Kuhn, P.; Canestrelli, I. L.; Getzoff, E. D. Nature 1998, 392, 206-209] supports its assignment to the PYP(B) (I(0)) intermediate. Differences between the time-resolved room temperature (298 K) spectrum of the PYP(B) intermediate and its low temperature (77 K) absorbance are attributed to a predominantly deprotonated chromophore in the former and protonated chromophore in the latter. This contrasts with the widely held belief that chromophore protonation does not occur until after the PYP(L) (I(1) or pR) intermediate. The structure of the chromophore in the PYP(L) intermediate is determined computationally and shown to be deprotonated, in agreement with experiment. Calculations based on our PYP(B) and PYP(L) models lead to insights concerning the PYP(BL) intermediate, observed only at low temperature. The results suggest that the proton is more mobile between Glu46 and the chromophore than previously realized. The findings presented here provide an example of the insights that theoretical studies can contribute to a unified analysis of experimental structures and spectra.     

Highlights on the recent advances in gold chemistry--a photophysical perspective

The presence of inter- and/or intra-molecular aurophilic interactions among the closed-shell gold(i) centres in various systems has been studied from various aspects, including synthetic, spectroscopic and theoretical approaches. The employment of different ligands can impose a significant influence on these factors and give rise to new complexes with interesting structural and photophysical properties. In this tutorial review, a number of recent examples are selected to illustrate the fascinating properties and chemistry, as well as versatility of gold(i) in these aspects and their potential applications to newcomers in this field. An emerging class of luminescent gold(iii) complexes is also described.     

Molecular Engineering Approaches Towards All-Organic White Light Emitting Materials

White light emitting (WLE) materials are of increasing interest owing to their promising applications in artificial lighting, display devices, molecular sensors, and switches. In this context, organic WLE materials cater to the interest of the scientific community owing to their promising features like color purity, long-term stability, solution processability, cost-effectiveness, and low toxicity. The typical method for the generation of white light is to combine three primary (red, green, and blue) or the two complementary (e.g., yellow and blue or red and cyan) emissive units covering the whole visible spectral window (400–800 nm). The judicious choice of molecular building blocks and connecting them through either strong covalent bonds or assembling through weak noncovalent interactions are the key to achieve enhanced emission spanning the entire visible region. In the present review article, molecular engineering approaches for the development of all-organic WLE materials are analyzed in view of different photophysical processes like fluorescence resonance energy transfer (FRET), excited-state intramolecular proton transfer (ESIPT), charge transfer (CT), monomer-excimer emission, triplet-state harvesting, etc. The key aspect of tuning the molecular fluorescence under the influence of pH, heat, and host–guest interactions is also discussed. The white light emission obtained from small organic molecules to supramolecular assemblies is presented, including polymers, micelles, and also employing covalent organic frameworks. The state-of-the-art knowledge in the field of organic WLE materials, challenges, and future scope are delineated.     

TIME-RESOLVED FOURIER TRANSFORM INFRARED SPECTROSCOPY OF THE BACTERIORHODOPSIN MUTANT TYR-185→E: ASP-96 REPROTONATES DURING O FORMATION; ASP-85 AND ASP-212 DEPROTONATE DURING O DECAY

The protonation state of key aspartic acid residues in the O intermediate of bacteriorhodopsin (bR) has been investigated by time-resolved Fourier transform infrared (FTIR) difference spectroscopy and site-directed mutagenesis. In an earlier study (Bousché et al., J. Biol Chem. 266, 11063-11067, 1991) we found that Asp-96 undergoes a deprotonation during the M-->N transition, confirming its role as a proton donor in the reprotonation pathway leading from the cytoplasm to the Schiff base. In addition, both Asp-85 and Asp-212, which protonate upon formation of the M intermediate, remain protonated in the N intermediate. In this study, we have utilized the mutant Tyr-185-->Phe (Y185F), which at high pH and salt concentrations exhibits a photocycle similar to wild type bR but has a much slower decay of the O intermediate. Y185F was expressed in native Halobacterium halobium and isolated as intact purple membrane fragments. Time-resolved FTIR difference spectra and visible difference spectra of this mutant were measured from hydrated multilayer films. A normal N intermediate in the photocycle of Y185F was identified on the basis of characteristic chromophore and protein vibrational bands. As N decays, bands characteristic of the all-trans O chromophore appear in the time-resolved FTIR difference spectra in the same time range as the appearance of a red-shifted photocycle intermediate absorbing near 640 nm. Based on our previous assignment of the carboxyl stretch bands to the four membrane embedded Asp groups: Asp-85, Asp-96, Asp-115 and Asp-212, we conclude that during O formation: (i) Asp-96 undergoes reprotonation. (ii) Asp-85 may undergo a small change in environment but remains protonated. (iii) Asp-212 remains partially protonated. In addition, reisomerization of the chromophore during the N-->O transition is accompanied by a major reversal of protein conformational changes which occurred during the earlier steps in the photocycle. These results are discussed in terms of a proposed mechanism for proton transport.     

Two Consecutive Polar Amino Acids at the End of Helix E are Important for Fast Turnover of the Archaerhodopsin Photocycle

Archaerhodopsins (ARs) is one of the members of microbial rhodopsins. Threonine 164 (T164) and serine 165 (S165) residues of the AR from Halorubrum sp. ejinoor (HeAR) are fully conserved in ARs, although they are far from the proton transfer channel and the retinal Schiff base, and are likely involved in a hydrogen‐bonding network at the end of the Helix E where most microbial rhodopsins assume a “bent structure”. In the present work, T164 and/or S165 were replaced with an alanine (A), and the photocycles of the mutants were analyzed with flash photolysis. The amino acid replacements caused profound changes to the photocycle of HeAR including prolonged photocycle, accelerated decay of M intermediate and appearance of additional two intermediates which were evident in T164A‐ and T164A/S165A‐HeAR photocyles. These results suggest that although T164 and S165 are located at the far end of the photoactive center, these two amino acid residues are important for maintaining the fast turnover of the HeAR photocycle. The underlying molecular mechanisms are discussed in relation to hydrogen‐bonding networks involving these two amino acids. Present study may arouse our interests to explore the functional role of the well‐conserved “bent structure” in different types of microbial rhodopsin.     

ABSORPTION AND PHOTOCHEMISTRY OF SENSORY RHODOPSIN—I: pH EFFECTS

Pyranine (8-hydroxyl-1,3,6-pyrene-trisulfonate) was used as a pH-probe to test whether there is a light-induced proton release to the bulk phase during the photochemical reaction cycle of sensory rhodopsin-I (SR-I). We conclude that the retinylidene Schiff-base proton is retained by SR-I-containing envelope vesicles during the SR-I photocycle under the conditions described here. Bacteriorhodopsin containing vesicles were used as a control to show that light-induced proton release can be observed under identical data acquisition parameters as those used for SR-I-containing vesicles. In addition, the effects of extravesicular pH on the absorption maximum (lambda max) and the SR-I photocycle were studied. SR-I properties are insensitive to pH in the range approximately 3 to approximately 8 with lambda max remaining at 587 nm. The lambda max shifts to 565 nm below pH 3.0 and to 552 nm at pH 10.8 with an apparent pKa of 8.5. Flash-induced absorbance changes of SR-I are described under neutral, alkaline and acidic conditions. The neutral, alkaline and acid SR-I forms each undergo similar photoreactions producing long-lived (> 500 ms decay half-time) blue-shifted intermediates. The UV/near-UV absorption of the photoproducts from neutral and alkaline SR-I indicate a deprotonated Schiff base, whereas acid SR-I produces a species with lambda max > 460 nm indicative of a protonated Schiff base.     

Deciphering the Spectral Tuning Mechanism in Proteorhodopsin: The Dominant Role of Electrostatics Instead of Chromophore Geometry

Proteorhodopsin (PR) is a photoactive proton pump found in marine bacteria. There are two phenotypes of PR exhibiting an environmental adaptation to the ocean's depth which tunes their maximum absorption: blue-absorbing proteorhodopsin (BPR) and green-absorbing proteorhodopsin (GPR). This blue/green color-shift is controlled by a glutamine to leucine substitution at position 105 which accounts for a 20 nm shift. Typically, spectral tuning in rhodopsins is rationalized by the external point charge model but the Q105L mutation is charge neutral. To study this tuning mechanism, we employed the hybrid QM/MM method with sampling from molecular dynamics. Our results reveal that the positive partial charge of glutamine near the C₁₄−C₁₅ bond of retinal shortens the effective conjugation length of the chromophore compared to the leucine residue. The derived mechanism can be applied to explain the color regulation in other retinal proteins and can serve as a guideline for rational design of spectral shifts.     

Array of aromatic amino acid side chains located near the chromophore of photoactive yellow protein

The role of the array of aromatic amino acid side chains located close to the chromophore binding loop of photoactive yellow protein (PYP) was studied using the alanine-substitution mutagenesis. Phe92, Tyr94, Phe96 and Tyr98 were replaced with alanine (F92A, Y94A, F96A and Y98A, respectively), then these mutants were characterized by UV-visible absorption spectra, circular dichroism (CD) spectra, thermal stability and photocycle kinetics. Absorption maxima of F92A, Y94A, F96A and Y98A were 444, 442, 439 and 447 nm, respectively, different to wild type (WT) at 446 nm. Far-UV CD spectra of mutants other than F92A were different from WT, indicating that Tyr94, Phe96 and Tyr98 maintain the native secondary structure of PYP. Mid-point temperatures of thermal denaturation of F92A, Y94A and F96A, estimated by the CD signal at 222 nm, were 5-10 degrees C lower than WT. Time constants of the photocycle estimated by flash-induced absorbance change were 0.36 s for WT and 1.4 s for Y98A, however, 100, 30 and 3000 times slower than WT for F92A, Y94A and F96A, respectively. Tyr98 is located in the loop region, whereas Phe92, Tyr94 and Phe96 are incorporated in the beta4 strand, showing that aromatic amino acid residues in the beta-sheet regulate the absorption spectrum, thermal stability and photocycle of PYP. Aromatic rings of Phe92, Tyr94 and Phe96 lie nearly perpendicular to the aromatic ring of Phe75 or chromophore. Possible weak hydrogen bonds between the aromatic ring hydrogen and pi-electrons of these residues are discussed.     

Distinguishing chromophore structures of photocycle intermediates of the photoreceptor PYP by transient fluorescence and energy transfer

The cinnamoyl chromophore is the light-activated switch of the photoreceptor photoactive yellow protein (PYP) and isomerizes during the functional cycle. The fluorescence of W119, the only tryptophan of PYP, is quenched by energy transfer to the chromophore. This depends on the chromophore's transition dipole moment orientation and spectrum, both of which change during the photocycle. The transient fluorescence of W119 thus serves as a sensitive kinetic monitor of the chromophore's structure and orientation and was used for the first time to investigate the photocycle kinetics. From these data and measurements of the ps-fluorescence decay with background illumination (470 nm) we determined the fluorescence lifetimes of W119 in the I(1) and I (1') intermediates. Two coexisting distinct chromophore structures were proposed for the I(1) photointermediate from time-resolved X-ray diffraction ( Ihee, H., et al. Proc. Natl. Acad. Sci. U.S.A., 2005, 102, 7145 ): one with two hydrogen bonds to E46 and Y42, and a second with only one H-bond to Y42 and a different orientation. Only for the first of these is the calculated fluorescence lifetime of 0.22 ns in good agreement with the observed one of 0.26 ns. The second structure has a predicted lifetime of 0.71 ns. Thus, we conclude that in solution only the first I(1) structure occurs. The high resolution structure of the I(1') intermediate, the decay product of I(1) at alkaline pH, is still unknown. We predict from the observed lifetime of 1.3 ns that the chromophore structure of I(1') is quite similar to that of the I(2) intermediate, and I(1') should thus be considered as the alkaline (deprotonated) form of I(2).