Fluorescent derivatives of the GFP chromophore give a new insight into the GFP fluorescence process

The photophysical properties of synthetic compounds derived from the imidazolidinone chromophore of the green fluorescent protein were determined. Various electron-withdrawing or electron-donating substituents were introduced to mimic the effect of the chromophore surroundings in the protein. The absorption and emission spectra as well as the fluorescence quantum yields in dioxane and glycerol were shown to be highly dependent on the electronic properties of the substituents. We propose a kinetic scheme that takes into account the temperature-dependent twisting of the excited molecule. If the activation energy is low, the molecule most often undergoes an excited-state intramolecular twisting that leads it to the ground state through an avoided crossing between the S(1) and S(0) energy surfaces. For a high activation energy, the torsional motion within the compounds is limited and the ground-state recovery will occur preferentially by fluorescence emission. The excellent correlation between the fluorescence quantum yields and the calculated activation energies to torsion points to the above-mentioned avoided crossing as the main nonradiative deactivation channel in these compounds. Finally, our results are discussed with regard to the chromophore in green fluorescent protein and some of its mutants.     

On the linkages between chromophore and protein in biliproteins, VII. Amino acid sequence in the chromophore regions of C-phycoerythrin from Pseudanabaena W 1173 and Phormidium persicinum.

Bilipeptides from all chromophore regions were prepared by trypsin digestion of C-phycoerythrin from Pseudanabaena W 1173 and Phormidium persicinum. Analytical separation and quantitative determination of bilipeptides was achieved by isoelectric focusing, preparative isolation by gel chromatography and ion-exchange chromatography. Amino acid analysis revealed cysteine as the only amino acid common to all chromopeptides. Amino acid sequences were determined by Edman degradation and the dansyl-Edman technique. Sequences are different in all 5 and 6 chromophore regions, respectively. Possible homologies are discussed. A thioether linkage between ring A of the chromophore and cysteine was found in the bilipeptides (as before in biliproteins). A second linkage (serine ester) was found in only one peptide (CM 4.I from Pseudanabaena W 1173). This peptide absorbs as cation at a longer wavelength (559 nm) than the other bilipeptides (542 - 550 nm).     

Enhanced Photolysis of Nucleic Acid Monomers by Pyrophosphate in the Simulated Primitive Soup

In our simulation of the photochemistry of the primitive soup, it was found that yield of chromophore loss of some nucleic acid bases, nucleosides and nucleotides [NA] undergoing ultraviolet radiation by medium pressure mercury lamp [MPML] was enhanced by pyrophosphate and triphosphate whether O2 is present or not. The yield of chromophore loss of guanosine, uracil, 5 CMP, and the derivatives of adenine and thymine was observed to rise with the increase of molar concentration of pyrophosphate in N2-saturated systems. In air-saturated samples, increase in yield of chromophore loss was observed when the concentration of pyrophosphate reaches 5×10-4 M, relative yield of chromophore loss (CLrel) coming to maximum in the range from 0.01 to 0.1 M, followed by a slight decline with the further increase of pyrophosphate concentration. The enhancement of photolysis of NA by pyrophosphate was due to the interaction between NA and pyrophosphate radicals photoionized by UV quanta of wavelength less than about 210 nm in the emission spectrum of a MPML. The relevance of this phenomenon to the origin of life has been discussed as well.     

Depth of immersion of fluorescent chromophores in biomembranes studied by quenching with nitroxide radical

A novel method has been developed for measuring depth of immersion of a fluorescent chromophore in biological matrices, such as biomembranes. The method is based on dynamic quenching of chromophore fluorescence by a nitroxide probe freely diffused in solution. Theoretical considerations and experimental evidences relating to the method are discussed. The proposed method was applied to investigation of lecithin liposomes and membranes from Bacillus subtilis modified by the photochrome-fluorescent probe 4,4'-dimethylaminocyanostilbene.     

Properties of the dark and signaling states of photoactive yellow protein probed by solution phase hydrogen/deuterium exchange and mass spectrometry

The perturbations on conversion from the dark state to the signaling state in photoactive yellow protein have been determined by solution-phase hydrogen/deuterium exchange and mass spectrometry. Both the wild type and M100A mutant are used in this study, with the mutant providing over 90% conversion to the bleached state under steady-state illumination. We found perturbations in both the wild type and the mutant on illumination, consistent with a more flexible structure in the long-lived signaling (I2') state. In the case of the wild type, the conformational changes detected are mainly around the chromophore region. With the M100A mutant, differences in H/D exchange between the light and dark are more extensive as compared to wild type; not only are the chromophore surroundings affected, but significant increases in deuterium uptake in the N-terminus and central beta-sheet are observed as well. On the basis of the data obtained from this study and previous findings, a sequence of events that leads to the perturbation of PYP following chromophore photoisomerization is proposed.     

Structural characterization of a thiazoline-containing chromophore in an orange fluorescent protein, monomeric Kusabira Orange

Monomeric Kusabira Orange (mKO) is a green fluorescent protein (GFP)-like protein that emits orange light at a peak of 559 nm. We analyzed its X-ray structure at 1.65 A and found a novel three-ring chromophore that developed autocatalytically from a Cys65-Tyr66-Glu67 tripeptide in which the side chain of Cys65 formed the third 2-hydroxy-3-thiazoline ring. As a result, the chromophore contained the CNCOH group at the 2-position of the imidazolinone moiety such that the conjugated pi-electron system of the chromophore was more extended than that of GFP but less extended than that of the Discosoma sp. red fluorescent protein (DsRed). Since a sulfur atom has potent nucleophilic character, the third 3-thiazoline ring is rapidly and completely cyclized. Furthermore, our structure reveals the presence of a pi-pi stacking interaction between His197 and the chromophore as well as a pi-cation interaction between Arg69 and the chromophore. These structural findings are sufficient to account for the orange emission, pH tolerance, and photostability of mKO.     

Molecular dynamics simulations of enhanced green fluorescent proteins: effects of F64L,S65T and T203Y mutations on the ground-state proton equilibria

Molecular dynamics simulations with the Amber force field are carried out to study two mutants of the green fluorescent protein (GFP), namely EGFP (F64L/S65T) and T203Y-EGFP (E(2)GFP). Those variants display an opposite equilibrium between the structural A and B states, associated with neutral and anionic protonation forms of the chromophore. Configurations of those two states are simulated for each variant and the energetics of their equilibrium in the two mutants is studied by evaluating the change in the relative free energy of A and B states (DeltaG(AB)) upon T203Y mutation. The resulting DeltaDeltaG(AB) agrees with the value inferred from absorption measurements. A comparison of the hydrogen bond network around the chromophore rationalizes the different population of state A and B in EGFP and E(2)GFP. On the basis of structural and energetic considerations, a mechanism for destabilization of the neutral chromophore in S65T mutants is proposed. Simulations of the B state of the S65T variant and of WT GFP are also performed for comparison and to test the force field parameters of the chromophore derived for the present calculations. Possible paths of proton transfer leading to nonfluorescent states of the chromophore are discussed in light of the photodynamical behavior of GFP, as revealed by fluorescence correlation spectroscopy and single-molecule experiments.     

Spectroscopic characterization of the photocycle intermediates of photoactive yellow protein.

The absorption spectra of photocycle intermediates of photoactive yellow protein mutants were compared with those of the corresponding intermediates of wild type to probe which amino acid residues interact with the chromophore in the intermediate states. B and H intermediates were produced by irradiation and trapped at 80 K, and L intermediates at 193 K. The absorption spectra of these intermediates produced from R52Q were identical to those from wild type, whereas those from E46Q and T50V were 7-15 nm red-shifted as those in the dark states. The absorption spectra of M intermediates were measured by flash photolysis at room temperature. Those of Y42F, T50V, and R52Q were identical to that of wild type, whereas that of E46Q was 11 nm red-shifted. Assuming that the intermediates of mutants have a structure comparable to that of wild type, these findings suggest the following: Glu46 interacts with the chromophore throughout the photocycle, interaction between the chromophore and Thr50 as well as Tyr42 is lost upon the formation of M intermediate, and Arg52 never interacts with the chromophore directly. The hydrogen-bonding network around the phenolic oxygen of the chromophore would be thus maintained until L intermediate decays, and the global conformational change would take place by the loss of the hydrogen bond between the chromophore and Tyr42. This model conflicts with some of the results of previous crystallographic studies, suggesting that the reaction mechanism in the crystal may be different from that in solution.     

The inhibitory mechanism of in vitro protein phosphorylation by a nonprotein chromophore removed from neocarzinostatin

The inhibitory effect of a nonprotein chromophore removed from neocarzinostatin on protein phosphorylation by nuclear protein kinase in vitro has been studied. Low levels of the chromophore greatly inhibited protein phosphorylation in vitro. This inhibition, however, was not selectively dependent on the indicated kinases and their different phosphate acceptors (histones and non-histone protein). In contrast, the protein component (apoprotein) of neocarzinostatin did not affect the phosphorylation even at a concentration of 400-times higher than that of the chromophore. Moreover, apoprotein suppressed the chromophore-induced inhibition of protein phosphorylation in vitro in proportion to the apoprotein concentrations. Kinetic and analytical experiments suggest that the chromophore-induced inhibition of protein phosphorylation seems to be due to the binding of the chromophore to the kinases. In addition, we found that ultraviolet irradiation as well as methanol extraction can release the chromophore from neocarzinostatin, but it exhibits no inhibitory activity of DNA synthesis in growing cells. The fact that the chromophore-induced inhibition of protein phosphorylation in vitro was not sensitive to ultraviolet irradiation, which rapidly inactivated the ability of the chromophore to induce DNA degradation in vitro, suggests that there are different actions involved in the two inhibitions induced by the chromophore which is removed from neocarzinostatin.     

Factors affecting the estimation of the relative amount of chromophore and chromophore area by the two-wavelength method of Patau and Ornstein.

Factors influencing the calculation of the relative amount of chromophore and the chromophore area by the two-wavelength method are examined. The study was carried out with the help of models and further tested on Feulgen stained preparations. Except for certain restrictions the difference between the chromophore area as calculated from the two transmissions measurements and the chromophore area obtained by planimetry can be used as a guide for determining the proper measuring conditions, including the choise of the two wavelengths.     

Factors affecting the estimation of the relative amount of chromophore and chromophore area by the two-wavelength method of patau and ornstein

Summary Factors influencing the calculation of the relative amount of chromophore and the chromophore area by the two-wavelength method are examined. The study was carried out with the help of models and further tested on Feulgen stained preparations. Except for certain restrictions the difference between the chromophore area as calculated from the two transmissions measurements and the chromophore area obtained by planimetry can be used as a guide for determining the proper measuring conditions, including the choise of the two wavelengths.     

Resonance Raman study of the pink membrane photochemically prepared from the deionized blue membrane of H. halobium.

We report here the Resonance Raman spectrum of a 'pink' membrane (lambda max approximately 495 nm) photochemically generated from the deionized 'blue' membrane (Chang et al., 1985). Comparison of the Raman spectrum of the pink membrane with that of the model compounds, as well as the chromophore extraction data, indicate that the chromophore in the pink membrane is in the 9-cis configuration. The Schiff base peak at approximately 1,652 cm-1 shifts to approximately 1,622 cm-1 upon deuteration of the pink membrane, showing that the chromophore is bound to the bacterio-opsin by a protonated Schiff base linkage. The location of the Schiff base peak, as well as the 30 cm-1 shift that it undergoes upon deuteration, are quite different from the corresponding values for the native bacteriorhodopsin, suggesting differences in the local environment for the Schiff base in these pigments.     

Structural changes of pharaonis phoborhodopsin upon photoisomerization of the retinal chromophore: infrared spectral comparison with bacteriorhodopsin

Archaeal rhodopsins possess a retinal molecule as their chromophores, and their light energy and light signal conversions are triggered by all-trans to 13-cis isomerization of the retinal chromophore. Relaxation through structural changes of the protein then leads to functional processes, proton pump in bacteriorhodopsin and transducer activation in sensory rhodopsins. In the present paper, low-temperature Fourier transform infrared spectroscopy is applied to phoborhodopsin from Natronobacterium pharaonis (ppR), a photoreceptor for the negative phototaxis of the bacteria, and infrared spectral changes before and after photoisomerization are compared with those of bacteriorhodopsin (BR) at 77 K. Spectral comparison of the C--C stretching vibrations of the retinal chromophore shows that chromophore conformation of the polyene chain is similar between ppR and BR. This fact implies that the unique chromophore-protein interaction in ppR, such as the blue-shifted absorption spectrum with vibrational fine structure, originates from both ends, the beta-ionone ring and the Schiff base regions. In fact, less planer ring structure and stronger hydrogen bond of the Schiff base were suggested for ppR. Similar frequency changes upon photoisomerization are observed for the C==N stretch of the retinal Schiff base and the stretch of the neighboring threonine side chain (Thr79 in ppR and Thr89 in BR), suggesting that photoisomerization in ppR is driven by the motion of the Schiff base like BR. Nevertheless, the structure of the K state after photoisomerization is different between ppR and BR. In BR, chromophore distortion is localized in the Schiff base region, as shown in its hydrogen out-of-plane vibrations. In contrast, more extended structural changes take place in ppR in view of chromophore distortion and protein structural changes. Such structure of the K intermediate of ppR is probably correlated with its high thermal stability. In fact, almost identical infrared spectra are obtained between 77 and 170 K in ppR. Unique chromophore-protein interaction and photoisomerization processes in ppR are discussed on the basis of the present infrared spectral comparison with BR.     

Structural changes during the formation of early intermediates in the bacteriorhodopsin photocycle

Early intermediates of bacteriorhodopsin's photocycle were modeled by means of ab initio quantum mechanical/molecular mechanical and molecular dynamics simulations. The photoisomerization of the retinal chromophore and the formation of photoproducts corresponding to the early intermediates were simulated by molecular dynamics simulations. By means of the quantum mechanical/molecular mechanical method, the resulting structures were refined and the respective excitation energies were calculated. Two sequential intermediates were found with absorption maxima that exhibit red shifts from the resting state. The intermediates were therefore assigned to the K and KL states. In K, the conformation of the retinal chromophore is strongly deformed, and the N--H bond of the Schiff base points almost perpendicular to the membrane normal toward Asp-212. The strongly deformed conformation of the chromophore and weakened interaction of the Schiff base with the surrounding polar groups are the means by which the absorbed energy is stored. During the K-to-KL transition, the chromophore undergoes further conformational changes that result in the formation of a hydrogen bond between the N--H group of the Schiff base and Thr-89 as well as other rearrangements of the hydrogen-bond network in the vicinity of the Schiff base, which are suggested to play a key role in the proton transfer process in the later phase of the photocycle.     

The retinal conformation and its environment in rhodopsin in light of a new 2.2 A crystal structure

A new high-resolution structure is reported for bovine rhodopsin, the visual pigment in rod photoreceptor cells. Substantial improvement of the resolution limit to 2.2 A has been achieved by new crystallization conditions, which also reduce significantly the probability of merohedral twinning in the crystals. The new structure completely resolves the polypeptide chain and provides further details of the chromophore binding site including the configuration about the C6-C7 single bond of the 11-cis-retinal Schiff base. Based on both an earlier structure and the new improved model of the protein, a theoretical study of the chromophore geometry has been carried out using combined quantum mechanics/force field molecular dynamics. The consistency between the experimental and calculated chromophore structures is found to be significantly improved for the 2.2 A model, including the angle of the negatively twisted 6-s-cis-bond. Importantly, the new crystal structure refinement reveals significant negative pre-twist of the C11-C12 double bond and this is also supported by the theoretical calculation although the latter converges to a smaller value. Bond alternation along the unsaturated chain is significant, but weaker in the calculated structure than the one obtained from the X-ray data. Other differences between the experimental and theoretical structures in the chromophore binding site are discussed with respect to the unique spectral properties and excited state reactivity of the chromophore.     

Resonance Raman studies of the HOOP modes in octopus bathorhodopsin with deuterium-labeled retinal chromophores

Resonance Raman spectra of the hydrogen out-of-plane (HOOP) vibrational modes in the retinal chromophore of octopus bathorhodopsin with deuterium label(s) along the polyene chain have been obtained. In clear contrast with bovine bathorhodopsin's HOOP modes, there are only two major HOOP bands at 887 and 940 cm-1 for octopus bathorhodopsin. On the basis of their isotopic shifts upon deuterium labeling, we have assigned the band at 887 cm-1 to C10H and C14H HOOP modes, and the band at 940 cm-1 to C11H = C12H Au-like HOOP mode. Except for a 26 cm-1 downward shift, the C11H = C12H Au-like wag appears to be little disturbed in octopus bathorhodopsin from the chromophore in solution since its changes upon deuterium labeling are close to those found in solution model-compound studies. We found also that the C10H and C14H HOOP wags are also similar to those in the model-compound studies. However, we have found that the interaction between the C7H and C8H HOOP internal coordinates of the chromophore in octopus bathorhodopsin is different from that of the chromophore in solution. The intensity of the C11H = C12H and the other HOOP modes suggests that the chromophore of octopus bathorhodopsin is somewhat torsionally distorted from a planar trans geometry. Importantly, a twist about C11 = C12 double bond is inferred. Such a twist breaks the local symmetry, resulting in the observation of the normally Raman-forbidden C11H = C12H Au-like HOOP mode. The twisted nature of the chromophore, semiquantitatively discussed here, likely affects the lambda max of the chromophore and its enthalpy.(ABSTRACT TRUNCATED AT 250 WORDS)     

A protein dynamics study of photosystem II: the effects of protein conformation on reaction center function

Molecular dynamics simulations have been performed to study photosystem II structure and function. Structural information obtained from simulations was combined with ab initio computations of chromophore excited states. In contrast to calculations based on the x-ray structure, the molecular-dynamics-based calculations accurately predicted the experimental absorbance spectrum. In addition, our calculations correctly assigned the energy levels of reaction-center (RC) chromophores, as well as the lowest-energy antenna chlorophyll. The primary and secondary quinone electron acceptors, Q_A and Q_B, exhibited independent changes in position over the duration of the simulation. Q_B fluctuated between two binding sites similar to the proximal and distal sites previously observed in light- and dark-adapted RC from purple bacteria. Kinetic models were used to characterize the relative influence of chromophore geometry, site energies, and electron transport rates on RC efficiency. The fluctuating energy levels of antenna chromophores had a larger impact on quantum yield than did their relative positions. Variations in electron transport rates had the most significant effect and were sufficient to explain the experimentally observed multi-component decay of excitation in photosystem II. The implications of our results are discussed in the context of competing evolutionary selection pressures for RC structure and function.     

含Dsred类似生色团的红色荧光蛋白的发展及应用

自从绿色荧光蛋白(GFP)被发现以来,荧光蛋白在生物医学领域已经成为一种重要的荧光成像工具．随着红色荧光蛋白DsRed的出现,各种优化的DsRed突变体和远红荧光蛋白也不断涌现．其中荧光蛋白生色团的形成机制对改建更优的荧光蛋白变种影响很大,对于红色荧光蛋白而言,大多数的红色荧光蛋白的生色团类型为DsRed类似生色团,在此基础上又出现了Far-red DsRed类似生色团．目前,含DsRed类似生色团的荧光蛋白主要有单体红色荧光蛋白、光转换荧光蛋白、斯托克斯红移蛋白、荧光计时器等．这些优化的荧光蛋白作为分子探针可以实现对活细胞、细胞器或胞内分子的时空标记和追踪,已经在生物工程学、细胞生物学、基础医学领域得到广泛应用．本文综述了含DsRed类似生色团的荧光蛋白的研究进展及其应用,以及由此发展起来的远红荧光蛋白在活体显微成像技术中的应用,并展望了荧光探针技术研究的新方向．     

Resonance raman spectroscopy of an ultraviolet-sensitive insect rhodopsin

We present the first visual pigment resonance Raman spectra from the UV-sensitive eyes of an insect, Ascalaphus macaronius (owlfly). This pigment contains 11-cis-retinal as the chromophore. Raman data have been obtained for the acid metarhodopsin at 10 degrees C in both H2O and D2O. The C = N stretching mode at 1660 cm-1 in H2O shifts to 1631 cm-1 upon deuteriation of the sample, clearly showing a protonated Schiff base linkage between the chromophore and the protein. The structure-sensitive fingerprint region shows similarities to the all-trans-protonated Schiff base of model retinal chromophores, as well as to the octopus acid metarhodopsin and bovine metarhodopsin I. Although spectra measured at -100 degrees C with 406.7-nm excitation, to enhance scattering from rhodopsin (lambda max 345 nm), contain a significant contribution from a small amount of contaminants [cytochrome(s) and/or accessory pigment] in the sample, the C = N stretch at 1664 cm-1 suggests a protonated Schiff base linkage between the chromophore and the protein in rhodopsin as well. For comparison, this mode also appears at approximately 1660 cm-1 in both the vertebrate (bovine) and the invertebrate (octopus) rhodopsins. These data are particularly interesting since the absorption maximum of 345 nm for rhodopsin might be expected to originate from an unprotonated Schiff base linkage. That the Schiff base linkage in the owlfly rhodopsin, like in bovine and in octopus, is protonated suggests that a charged chromophore is essential to visual transduction.     

Cyanobacterial phytochrome-like PixJ1 holoprotein shows novel reversible photoconversion between blue- and green-absorbing forms

The gene, pixJ1 (formerly pisJ1), is predicted to encode a phytochrome-like photoreceptor that is essential for positive phototaxis in the unicellular cyanobacterium Synechocystis sp. PCC 6803 [Yoshihara et al. (2000) Plant Cell Physiol. 41: 1299]. The PixJ1 protein was overexpressed as a fusion with a poly-histidine tag (His-PixJ1) and isolated from Synechocystis cells. A zinc-fluorescence assay suggested that a linear tetrapyrrole was covalently attached to the His-PixJ1 protein as a chromophore. His-PixJ1 showed novel photoreversible conversion between a blue light-absorbing form (Pb, lambdaAmax=425-435 nm) and a green light-absorbing form (Pg, lambdaAmax=535 nm). Dark incubation led Pg to revert to Pb, indicative of stability of the Pb form in darkness. Red or far-red light irradiation, which is effective for photochemical conversion of the known phytochromes, produced no change in the spectra of Pb and Pg forms. Site-directed mutagenesis revealed that a Cys-His motif in the second GAF domain of PixJ1 is responsible for binding of the chromophore. Possible chromophore species are discussed with regard to the novel photoconversion spectrum.