Raman microscope studies on the primary photochemistry of vertebrate visual pigments with absorption maxima from 430 to 502 nm

Raman microscope vibrational spectra have been recorded from single photoreceptor cells frozen at 77 K. Spectra of photostationary steady-state mixtures of visual pigments and their primary photoproducts were obtained from toad red rods (lambda max 502 nm), angelfish rods (lambda max 500 nm), gecko blue rods (lambda max 467 nm), and bullfrog green rods (lambda max 430 nm). All four photoproducts have enhanced low-wavenumber Raman lines at approximately 850, 875, and 915 cm-1 and show the anomalous decoupling of the 11- and 12-hydrogen out-of-plane (HOOP) wagging vibrations, as is observed in the bovine primary photoproduct. The low-wavenumber lines are enhanced in the resonance Raman spectrum by conformational distortion, and the uncoupling of the 11- and 12-hydrogen wags is caused by additional protein perturbations. The similarity of the HOOP modes in all four photoproducts indicates that the protein perturbations that uncouple the 11- and 12-hydrogen wags and that enhance the HOOP modes are very similar. Thus, these perturbations of the photoproduct Raman spectrum cannot be caused by the same protein-chromophore interactions that are responsible for wavelength regulation in these pigments.     

Resonance Raman spectroscopy of pyridoxal Schiff bases

Resonance Raman (RR) spectra are reported for amino acid and amine adducts of pyridoxal 5'-phosphate (PLP) and 5'-deoxypyridoxal (5'-dPL) in aqueous solution. For the valine adducts, a detailed study has been carried out on solutions at pH and pD 5, 9, and 13, values at which the pyridine and imine protons are successively ionized, and on the adducts formed from 15N-valine, alpha-deuterovaline, and N-methyl-PLP. Good quality spectra were obtained, despite the strong fluorescence of pyridoxal Schiff bases, by adding KI as a quencher, and by exciting the molecules on the blue side of their absorption bands: 406.7 nm (cw Kr+ laser) for the pH 5 and 9 species (lambda max = 409 and 414 nm), and 354.7 nm (pulsed YAG laser, third harmonic) for the pH 13 species (lambda max = 360 nm). A prominent band at 1646 cm-1 is assigned to the imine C=N stretch via its 13 cm-1 15N shift. A 12 cm-1 down-shift of the band in D2O confirms that the Schiff base linkage is protonated at pH 9. Deprotonation at pH 13 shifts VC = N from 1646 to 1629 cm-1, values typical of conjugated Schiff bases. The strongest band in the spectrum, at 1338 cm-1, shifts to 1347 cm-1 upon pyridine protonation at pH 5, and is assigned to a ring mode with a large component of phenolate C-O stretch. A shoulder on its low-frequency side is assigned to the C4-C4' stretch. Large enhancements of these modes can be understood qualitatively in terms of the dominant resonance structures contributing to the ground and resonant excited states. A number of weaker bands are observed, and assigned to pyridine ring modes. These modes gain significantly in intensity, while the exocyclic modes diminish, when the spectra are excited at 266 nm (YAG laser, fourth harmonic) in resonance with ring-localized electronic transitions.     

Absorption spectra of the hydroxycyclohexadienyl radicals of substrates for phenol hydroxylase

The absorption spectra of the hydroxycyclohexadienyl radicals formed upon the addition of OH radicals to six substrates for phenol hydroxylase have been determined using pulse radiolysis. Combining the radical spectra of thiophenol (lambda max, 390 nm; epsilon, 10,500 M-1 cm-1) and resorcinol (lambda max, 340 nm; epsilon, 4,100 M-1 cm-1) with their respective published spectra of enzyme-bound reduced flavin that is substituted in the C(4a) position of the dihydroflavin ring gave composite spectra that closely match the spectra formed concomitantly with the introduction of an oxygen atom into the substrates, the so-called Intermediate II species. A similar procedure for the substrates hydroquinone, 3-aminophenol, 3-chlorophenol, and 3-methylphenol yielded spectra that are also consistent with the known characteristics of their Intermediate II species. These spectral results give further support to the proposed biradical mechanism (Anderson, R.F., Patel, K. B., and Stratford, M. R. L. (1987) J. Biol. Chem. 262, 17475-17479) for the functioning of this class of flavoprotein hydroxylases.     

A pulse-radiolysis study of the reaction of hydrated electrons with N'-formylkynurenine and related compounds: electron-transfer reactions with nucleic acid components.

The reactivity of N'-formylkynurenine (FK) derivatives towards eaq has been investigated. The reduced transient species have been characterized (lambda max approximately 340, 440 nm, epsilon lambda max approximately 3000-1000 M-1 cm-1, pKa approximately 7.8). Owing to the strong FK electron affinity, electron-transfer reactions occur from purine (except guanine) and pyrimidine electron adducts to FK (k approximately 2-7 x 10(9) M-1 s-1). As some FK derivatives bind to DNA (or polynucleotides) the protective effect of complexation on FK-DNA (or polynucleotides) adduct formation has been investigated.     

Dynamics of the excited state of the primary electron donor in reaction centers of Rhodopseudomonas viridis as revealed by hole burning at 1.7K. Different conformational states

The spectra of absorbance changes (delta A) due to the formation of P+Q- (P, primary electron donor, Q, primary quinone acceptor) at 1.7K in Rhodopseudomonas viridis reaction centers (RCs) excited at 1014 nm has been shown to include, besides a progression of broad (170-190 cm-1) Gaussian vibronic bands separated by 150 cm-1, a 'narrow' structure near 1014 nm which can be simulated by a Lorentian zero-phonon hole (ZPH) and Lorentian one-mode (26.8 cm-1) phonon wings. The widths of ZPH of approximately 17 cm-1 for delta A reflecting the formation of P+Q- decaying in the ms time domain and of 6.8 +/- 0.4 cm-1 for P+Q- decaying in the min time domain at 1.7K, seems to correspond to different conformations of RCs with a relaxation time of P* of approximately 0.6 ps (in agreement with measurements in this time domain) and 1.6 +/- 0.1 ps, respectively. The comparison of the spectra of delta A in the region of the BL band for slow (min) and fast (ms) decaying components suggests a different mutual arrangement of P and BL for different conformations of RCs. It is assumed that the broad and narrow structures of the P band reflect the transitions to two configurations with different P-protein interactions. 'Narrow' structure of delta A spectrum with essentially the same phonon wings and ZPH (width of 3.8 +/- 0.4 cm-1) was observed within the P band when HL was photoreduced at 1.7K.     

Structure of apoproteins in insect lipophorin

The two polypeptide chains of cockroach and locust lipophorins were separated and their amino acid compositions were determined. Circular dichroic spectra of the lipophorins and apolipophorin from 190 to 250 nm showed a single trough at 218 nm and a peak at 194 nm. Infrared spectra of the lipophorins in D2O showed a strong peak at 1625 cm-1 and a weak shoulder at 1693 cm-1 corresponding to v (pi, 0) and nu (0, pi) of antiparallel pleated sheet. The resonance frequency splitting delta nu = nu (0, pi) -nu (pi, 0) was 68 cm-1, which was larger than that of ordinary globular proteins containing antiparallel pleated sheet. From circular dichroic and infrared spectra it was concluded that lipophorins contained polypeptides rich in antiparallel pleated sheet with longer unbroken extensions than the case for ordinary globular proteins. Partial proteolytic digestion study of lipophorins with trypsin, chymotrypsin, and subtilisin showed that the larger apolipophorin (AL1) was exposed to the surface of the particle and the smaller apolipophorin (AL2) lay protected from the attack of the enzymes. Crosslinked products between AL1 and AL2 were readily obtained when dimethylsuberimidate or dimethyladipimidate was added to the lipophorin solution, without giving lipophorin dimers, suggesting that the two chains were located within 11 A from each other. Such structural features of insect lipoprotein were compared with other insect lipophorins and the human serum low-density lipoprotein (LDL). Similarities between lipophorins and LDL were found in the molecular weight, amino acid compositions, and the secondary structure of major apoproteins.     

Excited-state structure and isomerization dynamics of the retinal chromophore in rhodopsin from resonance Raman intensities.

Resonance Raman excitation profiles have been measured for the bovine visual pigment rhodopsin using excitation wavelengths ranging from 457.9 to 647.1 nm. A complete Franck-Condon analysis of the absorption spectrum and resonance Raman excitation profiles has been performed using an excited-state, time-dependent wavepacket propagation technique. This has enabled us to determine the change in geometry upon electronic excitation of rhodopsin's 11-cis-retinal protonated Schiff base chromophore along 25 normal coordinates. Intense low-frequency Raman lines are observed at 98, 135, 249, 336, and 461 cm-1 whose intensities provide quantitative, mode-specific information about the excited-state torsional deformations that lead to isomerization. The dominant contribution to the width of the absorption band in rhodopsin results from Franck-Condon progressions in the 1,549 cm-1 ethylenic normal mode. The lack of vibronic structure in the absorption spectrum is shown to be caused by extensive progressions in low-frequency torsional modes and a large homogeneous linewidth (170 cm-1 half-width) together with thermal population of low-frequency modes and inhomogeneous site distribution effects. The resonance Raman cross-sections of rhodopsin are unusually weak because the excited-state wavepacket moves rapidly (approximately 35 fs) and permanently away from the Franck-Condon geometry along skeletal stretching and torsional coordinates.     

Interaction of anions with the active site of carboxypeptidase A

Studies of azide inhibition of peptide hydrolysis catalyzed by cobalt(II) carboxypeptidase A identify two anion binding sites. Azide binding to the first site (KI = 35 mM) inhibits peptide hydrolysis in a partial competitive mode while binding at the second site (KI = 1.5 M) results in competitive inhibition. The cobalt electronic absorption spectrum is insensitive to azide binding at the first site but shows marked changes upon azide binding to the second site. Thus, azide elicits a spectral change with new lambda max (epsilon M) values of 590 (330) and 540 nm (190) and a KD of 1.4 M, equal to the second kinetic KI value for the cobalt enzyme, indicating that anion binding at the weaker site involves an interaction with the active-site metal. Remarkably, in the presence of the C-terminal products of peptide or ester hydrolysis or carboxylate inhibitor analogues, anion (e.g., azide, cyanate, and thiocyanate) binding is strongly synergistic; thus, KD for azide decreases to 4 mM in the presence of L-phenylalanine. These ternary complexes have characteristic absorption, CD, MCD, and EPR spectra. The absorption spectra of azide/carboxylate inhibitor ternary complexes with Co(II)CPD display a near-UV band between 305 and 310 nm with epsilon M values around 900-1250 M-1 cm-1. The lambda max values are close to the those of the charge-transfer band of an aquo Co(II)-azide complex (310 nm), consistent with the presence of a metal azide bond in the enzyme complex.(ABSTRACT TRUNCATED AT 250 WORDS)     

Raman spectroscopic studies of the DNA cro binding site conformation, free and bound to cro protein.

Raman spectra of the DNA binding site for cro repressor protein were obtained in the presence and absence of bound cro protein. The 17 base pair fragment is a consensus sequence of the six cro binding sites in phage lambda, except that the second base to the right of the center of pseudosymmetry is altered. Analysis of the spectrum of the free DNA indicates that the molecule exists in a B-like conformation with deviations from the usual B form occurring mainly in the bands assigned to A-T vibrations. The spectrum of the bound DNA was obtained by subtracting the spectrum of free cro from the spectrum of the complex which was estimated to be 90% bound. The DNA undergoes significant structural changes upon binding to the protein; most notable of these changes is a destacking of the G-C bases reflected by increases in the 1240, 1262, and 1320 cm-1 bands. A decrease in the 1361 cm-1 band that occurs has also been assigned to a destacking in guanine bases. The appearance of a 705 cm-1 band and the decrease and downshift of the 670 cm-1 band are consistent with the appearance of A-like character in the A-T region of the binding site when the protein binds; however, the spectra indicate that the entire binding site remains in a distorted B-like conformation. We use the 705 cm-1 band to estimate A-like character because the 800-850 cm-1 region is obscured by interference from strong protein bands. Other shifts in both intensity and position cannot be assigned to characteristic changes in conformation and therefore must be attributed to the protein influencing the structure in a novel way.     

Photochemistry of the primary event in short-wavelength visual opsins at low temperature.

Two short-wavelength cone opsins, frog (Xenopus laevis) violet and mouse UV, were expressed in mammalian COS1 cells, purified in delipidated form, and studied using cryogenic UV-vis spectrophotometry. At room temperature, the X. laevis violet opsin has an absorption maximum at 426 nm when generated with 11-cis-retinal and an absorption maximum of 415 nm when generated with 9-cis-retinal. The frog short-wavelength opsin has two different batho intermediates, one stable at 30 K (lambda(max) approximately 446 nm) and the other at 70 K (lambda(max) approximately 475 nm). Chloride ions do not affect the absorption maximum of the violet opsin. At room temperature, mouse UV opsin has an absorption maximum of 357 nm, while at 70 K, the pigment exhibits a bathochromic shift to 403 nm with distinct vibronic structure and a strong secondary vibronic band at 380 nm. We have observed linear relationships when analyzing the energy difference between the initial and bathochromic intermediates and the normalized difference spectra of the batho-shifted intermediates of rod and cone opsins. We conclude that the binding sites of these pigments change from red to green to violet via systematic shifts in the position of the primary counterion relative to the protonated Schiff base. The mouse UV cone opsin does not fit this trend, and we conclude that wavelength selection in this pigment must operate via a different molecular mechanism. We discuss the possibility that the mouse UV chromophore is initially unprotonated.     

Regeneration of bovine and octopus opsins in situ with natural and artificial retinals

We consider the problem of color regulation in visual pigments for both bovine rhodopsin (lambda max = 500 nm) and octopus rhodopsin (lambda max = 475 nm). Both pigments have 11-cis-retinal (lambda max = 379 nm, in ethanol) as their chromophore. These rhodopsins were bleached in their native membranes, and the opsins were regenerated with natural and artificial chromophores. Both bovine and octopus opsins were regenerated with the 9-cis- and 11-cis-retinal isomers, but the octopus opsin was additionally regenerated with the 13-cis and all-trans isomers. Titration of the octopus opsin with 11-cis-retinal gave an extinction coefficient for octopus rhodopsin of 27,000 +/- 3000 M-1 cm-1 at 475 nm. The absorption maxima of bovine artificial pigments formed by regenerating opsin with the 11-cis dihydro series of chromophores support a color regulation model for bovine rhodopsin in which the chromophore-binding site of the protein has two negative charges: one directly hydrogen bonded to the Schiff base nitrogen and another near carbon-13. Formation of octopus artificial pigments with both all-trans and 11-cis dihydro chromophores leads to a similar model for octopus rhodopsin and metarhodopsin: there are two negative charges in the chromophore-binding site, one directly hydrogen bonded to the Schiff base nitrogen and a second near carbon-13. The interaction of this second charge with the chromophore in octopus rhodopsin is weaker than in bovine, while in metarhodopsin it is as strong as in bovine.     

Occurrence of a novel nucleotide, Zpp5'A2'p, in rat liver extracts

The nucleotide Zpp5'A2'p has been isolated from rat liver. Z stands for an unknown compound, probably a nucleoside. The preliminary structure of Zpp5'A2'p has been elucidated by treatment with phosphodiesterase and/or alkaline phosphatase and analysis of the products of the reaction by high pressure liquid chromatography. The following ultraviolet absorption spectral characteristics were determined at pH 7.0: Zpp5'A2'p (lambda max = 265 nm; A250/A260 = 0.76; A280/A260 = 0.83); Zp (lambda max = 280 nm; A250/A260 = 0.88; A280/A260 = 1.46). The molar extinction coefficient found for Zp, at 280 nm, was (7.5 + 0.9) X 10(3) M-1 cm-1. The base of Zp could correspond to an indole derivative.     

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)     

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.     

Detection and identification of intermediates in the reaction of L-serine with Escherichia coli tryptophan synthase via rapid-scanning ultraviolet-visible spectroscopy

Rapid-scanning stopped-flow (RSSF) UV-visible spectroscopy has been used to investigate the UV-visible absorption changes (300-550 nm) that occur in the spectrum of enzyme-bound pyridoxal 5'-phosphate during the reaction of L-serine with the alpha 2 beta 2 and beta 2 forms of Escherichia coli tryptophan synthase. In agreement with previous kinetic studies [Lane, A., & Kirschner, K. (1983) Eur. J. Biochem. 129, 561-570], the reaction with alpha 2 beta 2 was found to occur in three detectable relaxations (1/tau 1 greater than 1/tau 2 greater than 1/tau 3). The RSSF data reveal that during tau 1, the internal aldimine, E(PLP), with lambda max = 412 nm (pH 7.8), undergoes rapid conversion to two transient species, one with lambda max congruent to 420 nm and one with lambda max congruent to 460 nm. These species decay in a biphasic process (1/tau 2, 1/tau 3) to a complicated final spectrum with lambda max congruent to 350 nm and with a broad envelope of absorbance extending out to approximately 525 nm. Analysis of the time-resolved spectra establishes that the spectral changes in tau 2 are nearly identical with the spectral changes in tau 3. Kinetic isotope effects due to substitution of 2H for the alpha-1H of serine were found to increase the amount of the 420-nm transient and to decrease the amount of the species with lambda max congruent to 460 nm. These findings identify the serine Schiff base (the external aldimine) as the 420 nm absorbing, highly fluorescent transient; the species with lambda max congruent to 460 nm is the delocalized carbanion (quinoidal) species derived from abstraction of the alpha proton from the external aldimine. The reaction of L-serine with beta 2 consists of two relaxations (1/tau 1 beta greater than 1/tau 2 beta) and yields a quasi-stable species with lambda max = 420 nm, in good agreement with a previous report [Miles, E. W., Hatanaka, M., & Crawford, I. P. (1968) Biochemistry 7, 2742-2753]. Analysis of the RSSF spectra indicates that the same spectral change occurs in each phase of the reaction. The similarity of the spectral changes that occur in tau 2 and tau 3 of the alpha 2 beta 2 reaction is postulated to originate from the existence of two (slowly) interconverting forms of the enzyme.(ABSTRACT TRUNCATED AT 400 WORDS)     

Absorption spectra of radical forms of 2,4-dihydroxybenzoic acid, a substrate for p-hydroxybenzoate hydroxylase.

Combined optical and conductimetric measurements in aqueous solution indicate that at high pH (greater than or equal to 10).OH radicals react with the phenoxide form of 2,4-dihydroxybenzoic acid to form transiently phenoxyl radicals and a small amount of hydroxyeyclohexadienyl (HCHD) radicals by 150 ns. The respective yields of 88 and 12% of the total.OH radical yield were deduced from conductance and optical changes as well as from studies using a low potential reductant. The HCHD radical possesses a pKa of 8.0 +/- 0.1 and the constructed spectrum of the deprotonated forms of HCHD has a lambda max at 420 nm with a minimum extinction coefficient of approximately 7250 M-1 cm-1. The red shift in lambda max and increase in extinction coefficient compared to the revised spectral properties of the protonated form of the HCHD radical (lambda max at 390 nm with extinction coefficient of approximately 4500 M-1 cm-1), together with the pKa of the HCHD radical, provide an explanation for the pH-dependent spectral changes of the so-called highly absorbing intermediate II species, observed in the functioning of the enzyme p-hydroxybenzoate hydroxylase. These results add further to the evidence in support of the proposal that intermediate II is composed of species which absorb similarly to the flavin 4(a)-hydroxide and a form of the substrate/product such as the HCHD radical (Anderson, R. F., Patel, K. B., and Stratford, M. R. L. (1987) J. Biol. Chem. 262, 17475-17479).     

The photobleaching sequence of a short-wavelength visual pigment.

The photobleaching pathway of a short-wavelength cone opsin purified in delipidated form (lambda(max) = 425 nm) is reported. The batho intermediate of the violet cone opsin generated at 45 K has an absorption maximum at 450 nm. The batho intermediate thermally decays to the lumi intermediate (lambda(max) = 435 nm) at 200 K. The lumi intermediate decays to the meta I (lambda(max) = 420 nm) and meta II (lambda(max) = 388 nm) intermediates at 258 and 263 K, respectively. The meta II intermediate decays to free retinal and opsin at >270 K. At 45, 75, and 140 K, the photochemical excitation of the violet cone opsin at 425 nm generates the batho intermediate at high concentrations under moderate illumination. The batho intermediate spectra, generated via decomposing the photostationary state spectra at 45 and 140 K, are identical and have properties typical of batho intermediates of other visual pigments. Extended illumination of the violet cone opsin at 75 K, however, generates a red-shifted photostationary state (relative to both the dark and the batho intermediates) that has as absorption maximum at approximately 470 nm, and thermally reverts to form the normal batho intermediate when warmed to 140 K. We conclude that this red-shifted photostationary state is a metastable state, characterized by a higher-energy protein conformation that allows relaxation of the all-trans chromophore into a more planar conformation. FTIR spectroscopy of violet cone opsin indicates conclusively that the chromophore is protonated. A similar transformation of the rhodopsin binding site generates a model for the VCOP binding site that predicts roughly 75% of the observed blue shift of the violet cone pigment relative to rhodopsin. MNDO-PSDCI calculations indicate that secondary interactions involving the binding site residues are as important as the first-order chromophore protein interactions in mediating the wavelength maximum.     

Reversible denaturation of Aequorea green-fluorescent protein: physical separation and characterization of the renatured protein

The green-fluorescent protein (GFP) that functions as a bioluminescence energy transfer acceptor in the jellyfish Aequorea has been renatured with up to 90% yield following acid, base, or guanidine denaturation. Renaturation, following pH neutralization or simple dilution of guanidine, proceeds with a half-recovery time of less than 5 min as measured by the return of visible fluorescence. Residual unrenatured protein has been quantitatively removed by chromatography on Sephadex G-75. The chromatographed, renatured GFP has corrected fluorescence excitation and emission spectra identical with those of the native protein at pH 7.0 (excitation lambda max = 398 nm; emission lambda max = 508 nm) and also at pH 12.2 (excitation lambda max = 476 nm; emission lambda max = 505 nm). With its peak position red-shifted 78 nm at pH 12.2, the Aequorea GFP excitation spectrum more closely resembles the excitation spectra of Renilla (sea pansy) and Phialidium (hydromedusan) GFPs at neutral pH. Visible absorption spectra of the native and renatured Aequorea green-fluorescent proteins at pH 7.0 are also identical, suggesting that the chromophore binding site has returned to its native state. Small differences in far-UV absorption and circular dichroism spectra, however, indicate that the renatured protein has not fully regained its native secondary structure.     

Reconstitution of ancestral green visual pigments of zebrafish and molecular mechanism of their spectral differentiation

We previously reported that zebrafish have four tandemly duplicated green (RH2) opsin genes (RH2-1, RH2-2, RH2-3, and RH2-4). Absorption spectra vary widely among the four photopigments reconstituted with 11-cis retinal, with their peak absorption spectra (lambda(max)) being 467, 476, 488, and 505 nm, respectively. In this study, we inferred the ancestral amino acid (aa) sequences of the zebrafish RH2 opsins by likelihood-based Bayesian statistics and reconstituted the ancestral opsins by site-directed mutagenesis. The ancestral pigment (A1) to the four zebrafish RH2 pigments and that (A3) to RH2-3 and RH2-4 showed lambda(max) at 506 nm, while that (A2) to RH2-1 and RH2-2 showed a lambda(max) at 474 nm, indicating that a spectral shift had occurred toward the shorter wavelength on the evolutionary lineages A1 to A2 by 32 nm, A2 to RH2-1 by 7 nm, and A3 to RH2-3 by 18 nm. Pigment chimeras and site-directed mutagenesis revealed a large contribution (approximately 15 nm) of glutamic acid to glutamine substitution at residue 122 (E122Q) to the A1 to A2 and A3 to RH2-3 spectral shifts. However, the remaining spectral differences appeared to result from complex interactive effects of a number of aa replacements, each of which has only a minor spectral contribution (1-3 nm). The four zebrafish RH2 pigments cover nearly an entire range of lambda(max) distribution among vertebrate RH2 pigments and provide an excellent model to study spectral tuning mechanisms of RH2 in vertebrates.     

Transition dipole orientations in the early photolysis intermediates of rhodopsin.

The linear dichroism spectrum of rhodopsin in sonicated bovine disk membranes was measured 30, 60, 170, and 600 ns after room temperature photolysis with a linearly polarized, 7-ns laser pulse (lambda = 355 or 477 nm). A global exponential fitting procedure based on singular value decomposition was used to fit the linear dichroism data to two exponential processes which differed spectrally from one another and whose lifetimes were 42 +/- 7 ns and 225 +/- 40 ns. These results are interpreted in terms of a sequential model where bathorhodopsin (BATHO, lambda max = 543 nm) decays toward equilibrium with a blue shifted intermediate (BSI, lambda max = 478 nm). BSI then decays to lumirhodopsin (LUMI, lambda max = 492 nm). It has been suggested that two bathorhodopsins decay in parallel to their products. However, a Monte Carlo simulation of partial photolysis of solid-state visual pigment samples shows that one mechanism which creates populations of BATHO having different photolysis rates at 77 K may not be responsible for the two decay rates reported here at room temperature. The angle between the cis band and 498-nm band transition dipoles of rhodopsin is determined to be 38 degrees. The angles between both these transition dipoles and those of the long-wave-length bands of BATHO, BSI, and LUMI are also determined. It is shown that when BATHO is formed its transition dipole moves away from the original cis band transition dipole direction. The transition dipole then moves roughly twice as much towards the original cis band direction when BSI appears. Production of LUMI is associated with return of the transition dipole almost to the original orientation relative to the cis band, but with some displacement normal to the plane which contains the previous motions. The correlation between the lambda max of an intermediate and its transition dipole direction is discussed.