Conformational homogeneity and excited-state isomerization dynamics of the bilin chromophore in phytochrome Cph1 from resonance Raman intensities

The ground-state structure and excited-state isomerization dynamics of the P_r and P_fr forms of phytochrome Cph1 are investigated using resonance Raman intensity analysis. Electronic absorption and stimulated resonance Raman spectra of P_r and P_fr are presented; vibronic analysis of the Raman intensities and absorption spectra reveals that both conformers exist as a single, homogeneous population of molecules in the ground state. The homogeneous and inhomogeneous contributions to the overall electronic broadening are determined, and it is found that the broadening is largely homogeneous in nature, pointing to fast excited-state decay. Franck-Condon displacements derived from the Raman intensity analysis reveal the initial atomic motions in the excited state, including the highly displaced, nontotally symmetric torsional and C₁₅–H HOOP modes that appear because of symmetry-reducing distortions about the C₁₄–C₁₅ and C₁₅=C₁₆ bonds. P_fr is especially well primed for ultrafast isomerization and torsional Franck-Condon analysis predicts a <200 fs P_fr → P_r isomerization. This time is significantly faster than the observed 700 fs reaction time, indicating that the P_fr S₁ surface has a D-ring rotational barrier caused by steric interactions with the protein.     

Structure of the retinal chromophore in sensory rhodopsin I from resonance Raman spectroscopy

Sensory rhodopsin I (SR-I) is a retinal-containing pigment which functions as a phototaxis receptor in Halobacterium halobium. We have obtained resonance Raman vibrational spectra of the native membrane-bound form of SR587 and used these data to determine the structure of its retinal prosthetic group. The similar frequencies and intensities of the skeletal fingerprint modes in SR587, bacteriorhodopsin (BR568), and halorhodopsin (HR578) as well as the position of the dideuterio rocking mode when SR-I is regenerated with 12,14-D2 retinal (915 cm-1) demonstrate that the retinal chromophore has an all-trans configuration. The shift of the C = N stretching mode from 1628 cm-1 in H2O to 1620 cm-1 in D2O demonstrates that the chromophore in SR587 is bound to the protein by a protonated Schiff base linkage. The small shift of the 1195 cm-1 C14-C15 stretching mode in D2O establishes that the protonated Schiff base bond has an anti configuration. The low value of the Schiff base stretching frequency together with its small 8 cm-1 shift in D2O indicates that the Schiff base proton is weakly hydrogen bonded to its protein counterion. This suggests that the red shift in the absorption maximum of SR-I (587 nm) compared with HR (578 nm) and BR (568 nm) is due to a reduction of the electrostatic interaction between the protonated Schiff base group and its protein counterion.     

Molecular flow resonance Raman effect from retinal and rhodopsin.

We have performed resonance enhanced Raman measurements of retinal isomers in solution (all-trans, 11-cis, 9-cis, and 13-cis) and cetyltrimethylammonium bromide (CTAB) detergent extracts of bovine rhodopsin near physiological temperatures (17 degrees C). In order to measure these photolabile systems, we have developed a general technique which allows Raman measurements of any photosensitive material. This technique involves imposing a molecular velocity transverse to the Raman exciting laser beam sufficient to ensure that any given molecule moves through the beam so that it has little probability of absorbing a photon. We have also measured the resonance Raman spectra of crystals of the same retinal isomers. The data show that each isomer has a distinct and characteristic Raman spectra and that the spectrum of 11-cis-retinal is quite similar but not identical with that of rhodopsin and similarly for 9-cis-retinal compared with isorhodopsin. In agreement with previous work, the Raman data demonstrate that retinal and opsin are joined by a protonated Schiff base. Due to the fact that the Raman spectra of 11-cis-retinal (solution) and rhodopsin show bands near 998 and 1018 cm(-1), a spectral region previously assigned to C-Me stretching motions, it is suggested that 11-cis-retinal in solution is compased of a mixture of 12-s-trans and 12-s-cis, and that the conformation of rhodopsin is (perhaps distorted) 12-s-trans.     

Determination of retinal chromophore structure in bacteriorhodopsin with resonance Raman spectroscopy

The analysis of the vibrational spectrum of the retinal chromophore in bacteriorhodopsin with isotopic derivatives provides a powerful "structural dictionary" for the translation of vibrational frequencies and intensities into structural information. Of importance for the proton-pumping mechanism is the unambiguous determination of the configuration about the C13=C14 and C=N bonds, and the protonation state of the Schiff base nitrogen. Vibrational studies have shown that in light-adapted BR568 the Schiff base nitrogen is protonated and both the C13=C14 and C=N bonds are in a trans geometry. The formation of K625 involves the photochemical isomerization about only the C13=C14 bond which displaces the Schiff base proton into a different protein environment. Subsequent Schiff base deprotonation produces the M412 intermediate. Thermal reisomerization of the C13=C14 bond and reprotonation of the Schiff base occur in the M412------O640 transition, resetting the proton-pumping mechanism. The vibrational spectra can also be used to examine the conformation about the C--C single bonds. The frequency of the C14--C15 stretching vibration in BR568, K625, L550 and O640 argues that the C14--C15 conformation in these intermediates is s-trans. Conformational distortions of the chromophore have been identified in K625 and O640 through the observation of intense hydrogen out-of-plane wagging vibrations in the Raman spectra (see Fig. 2). These two intermediates are the direct products of chromophore isomerization. Thus it appears that following isomerization in a tight protein binding pocket, the chromophore cannot easily relax to a planar geometry. The analogous observation of intense hydrogen out-of-plane modes in the primary photoproduct in vision (Eyring et al., 1982) suggests that this may be a general phenomenon in protein-bound isomerizations. Future resonance Raman studies should provide even more details on how bacterio-opsin and retinal act in concert to produce an efficient light-energy convertor. Important unresolved questions involve the mechanism by which the protein catalyzes deprotonation of the L550 intermediate and the mechanism of the thermal conversion of M412 back to BR568. Also, it has been shown that under conditions of high ionic strength and/or low light intensity two protons are pumped per photocycle (Kuschmitz & Hess, 1981). How might this be accomplished?(ABSTRACT TRUNCATED AT 400 WORDS)     

Excited-state dynamics of all-trans protonated retinal Schiff base in CRABPII-based rhodopsin mimics

The rhodopsin mimic is a chemically synthetized complex with retinyl Schiff base (RSB) formed between protein and the retinal chromophore that can mimic the natural rhodopsin-like protein. The artificial rhodopsin mimic is more stable and designable than the natural protein and hence has wider uses in photon detection devices. The mimic structure RSB, like the case in the actual rhodopsin-like protein, undergoes isomerization and protonation throughout the photoreaction process. As a result, understanding the dynamics of the RSB in the photoreaction process is critical. In this study, the ultrafast transient absorption spectra of three mutants of the cellular retinoic acid-binding protein II-based rhodopsin mimic at acidic environment were recorded, from which the related excited-state dynamics of the all-trans protonated RSB (AT-PRSB) were investigated. The transient fluorescence spectra measurements are used to validate some of the dynamic features. We find that the excited-state dynamics of AT-PRSB in three mutants share a similar pattern that differs significantly from the dynamics of 15-cis PRSB of the rhodopsin mimic in neutral solution. By comparing the dynamics across the three mutants, we discovered that the aromatic residues near the β-ionone ring structure of the retinal may help stabilize the AT-PRSB and hence slow down its isomerization rate. The experimental results provide implications on designing a rhodopsin-like protein with significant infrared fluorescence, which can be particularly useful in the applications in biosensing or bioimaging in deeper tissues.     

All-trans retinal constitutes the functional chromophore in Chlamydomonas rhodopsin

Orientation of the green alga Chlamydomonas in light (phototaxis and stop responses) is controlled by a visual system with a rhodopsin as the functional photoreceptor. Here, we present evidence that in Chlamydomonas wild-type cells all-trans retinal is the predominant isomer and that it is present in amounts similar to that of the rhodopsin itself.

The ability of different retinal isomers and analog compounds to restore photosensitivity in blind Chlamydomonas cells (strain CC2359) was tested by means of flash-induced light scattering transients or by measuring phototaxis in a taxigraph. All-trans retinal reconstitutes behavioral light responses within one minute, whereas cis-isomers require at least 50 × longer incubation times, suggesting that the retinal binding site is specific for all-trans retinal. Experiments with 13-demethyl(dm)-retinal and short-chained analogs reveal that only chromophores with a β-methyl group and at least three double bonds in conjugation with the aldehyde mediate function. Because neither 13-dm-retinal, nor 9,12-phenylretinal restores a functional rhodopsin, a trans/13-cis isomerisation seems to take place in the course of the activation mechanism. We conclude that with respect to its chromophore, Chlamydomonas rhodopsin bears a closer resemblence to bacterial rhodopsins than to visual rhodopsins of higher animals.

     

Assignment of fingerprint vibrations in the resonance Raman spectra of rhodopsin, isorhodopsin, and bathorhodopsin: implications for chromophore structure and environment

13C- and 2H-labeled retinal derivatives have been used to assign normal modes in the 1100-1300-cm-1 fingerprint region of the resonance Raman spectra of rhodopsin, isorhodopsin, and bathorhodopsin. On the basis of the 13C shifts, C8-C9 stretching character is assigned at 1217 cm-1 in rhodopsin, at 1206 cm-1 in isorhodopsin, and at 1214 cm-1 in bathorhodopsin. C10-C11 stretching character is localized at 1098 cm-1 in rhodopsin, at 1154 cm-1 in isorhodopsin, and at 1166 cm-1 in bathorhodopsin. C14-C15 stretching character is found at 1190 cm-1 in rhodopsin, at 1206 cm-1 in isorhodopsin, and at 1210 cm-1 in bathorhodopsin. C12-C13 stretching character is much more delocalized, but the characteristic coupling with the C14H rock allows us to assign the "C12-C13 stretch" at approximately 1240 cm-1 in rhodopsin, isorhodopsin, and bathorhodopsin. The insensitivity of the C14-C15 stretching mode to N-deuteriation in all three pigments demonstrates that each contains a trans (anti) protonated Schiff base bond. The relatively high frequency of the C10-C11 mode of bathorhodopsin demonstrates that bathorhodopsin is s-trans about the C10-C11 single bond. This provides strong evidence against the model of bathorhodopsin proposed by Liu and Asato [Liu, R., & Asato, A. (1985) Proc. Natl. Acad. Sci. U.S.A. 82, 259], which suggests a C10-C11 s-cis structure. Comparison of the fingerprint modes of rhodopsin (1098, 1190, 1217, and 1239 cm-1) with those of the 11-cis-retinal protonated Schiff base in methanol (1093, 1190, 1217, and 1237 cm-1) shows that the frequencies of the C-C stretching modes are largely unperturbed by protein binding. In particular, the invariance of the C14-C15 stretching mode at 1190 cm-1 does not support the presence of a negative protein charge near C13 in rhodopsin. In contrast, the frequencies of the C8-C9 and C14-C15 stretches of bathorhodopsin and the C10-C11 and C14-C15 stretches of isorhodopsin are significantly altered by protein binding. The implications of these observations for the mechanism of wavelength regulation in visual pigments and energy storage in bathorhodopsin are discussed.     

Picosecond dynamics of G-protein coupled receptor activation in rhodopsin from time-resolved UV resonance Raman spectroscopy

The protein response to retinal chromophore isomerization in the visual pigment rhodopsin is studied using picosecond time-resolved UV resonance Raman spectroscopy. High signal-to-noise Raman spectra are obtained using a 1 kHz Ti:Sapphire laser apparatus that provides <3 ps visible (466 nm) pump and UV (233 nm) probe pulses. When there is no time delay between the pump and probe events, tryptophan modes W18, W16, and W3 exhibit decreased Raman scattering intensity. At longer pump-probe time delays of +5 and +20 ps, both tryptophan (W18, W16, W3, and W1) and tyrosine (Y1 + 2xY16a, Y7a, Y8a) peak intensities drop by up to 3%. These intensity changes are attributed to decreased hydrophobicity in the microenvironment near at least one tryptophan and one tyrosine residue that likely arise from weakened interaction with the beta-ionone ring of the chromophore following cis-to-trans isomerization. Examination of the crystal structure suggests that W265 and Y268 are responsible for these signals. These UV Raman spectral changes are nearly identical to those observed for the rhodopsin-to-Meta I transition, implying that impulsively driven protein motion by the isomerizing chromophore during the 200 fs primary transition drives key structural changes that lead to protein activation.     

Low-temperature solid-state 13C NMR studies of the retinal chromophore in rhodopsin

Magic angle sample spinning (MASS) 13C NMR spectra have been obtained of bovine rhodopsin regenerated with retinal prosthetic groups isotopically enriched with 13C at C-5 and C-14. In order to observe the 13C retinal chromophore resonances, it was necessary to employ low temperatures (-15-----35 degrees C) to restrict rotational diffusion of the protein. The isotropic chemical shift and principal values of the chemical shift tensor of the 13C-5 label indicate that the retinal chromophore is in the twisted 6-s-cis conformation in rhodopsin, in contrast to the planar 6-s-trans conformation found in bacteriorhodopsin. The 13C-14 isotropic shift and shift tensor principal values show that the Schiff base C = N bond is anti. Furthermore, the 13C-14 chemical shift (121.2 ppm) is within the range of values (120-123 ppm) exhibited by protonated (C = N anti) Schiff base model compounds, indicating that the C = N linkage is protonated. Our results are discussed with regard to the mechanism of wavelength regulation in rhodopsin.     

Structural analysis and dynamics of retinal chromophore in dark and meta I states of rhodopsin from 2H NMR of aligned membranes

Rhodopsin is a prototype for G protein-coupled receptors (GPCRs) that are implicated in many biological responses in humans. A site-directed (2)H NMR approach was used for structural analysis of retinal within its binding cavity in the dark and pre-activated meta I states. Retinal was labeled with (2)H at the C5, C9, or C13 methyl groups by total synthesis, and was used to regenerate the opsin apoprotein. Solid-state (2)H NMR spectra were acquired for aligned membranes in the low-temperature lipid gel phase versus the tilt angle to the magnetic field. Data reduction assumed a static uniaxial distribution, and gave the retinylidene methyl bond orientations plus the alignment disorder (mosaic spread). The dark-state (2)H NMR structure of 11-cis-retinal shows torsional twisting of the polyene chain and the beta-ionone ring. The ligand undergoes restricted motion, as evinced by order parameters of approximately 0.9 for the spinning C-C(2)H(3) groups, with off-axial fluctuations of approximately 15 degrees . Retinal is accommodated within the rhodopsin binding pocket with a negative pre-twist about the C11=C12 double bond that explains its rapid photochemistry and the trajectory of 11-cis to trans isomerization. In the cryo-trapped meta I state, the (2)H NMR structure shows a reduction of the polyene strain, while torsional twisting of the beta-ionone ring is maintained. Distortion of the retinal conformation is interpreted through substituent control of receptor activation. Steric hindrance between trans retinal and Trp265 can trigger formation of the subsequent activated meta II state. Our results are pertinent to quantum and molecular mechanics simulations of ligands bound to GPCRs, and illustrate how (2)H NMR can be applied to study their biological mechanisms of action.     

Mechanism of signal propagation upon retinal isomerization: insights from molecular dynamics simulations of rhodopsin restrained by normal modes

As one of the best studied members of the pharmaceutically relevant family of G-protein-coupled receptors, rhodopsin serves as a prototype for understanding the mechanism of G-protein-coupled receptor activation. Here, we aim at exploring functionally relevant conformational changes and signal transmission mechanisms involved in its photoactivation brought about through a cis-trans photoisomerization of retinal. For this exploration, we propose a molecular dynamics simulation protocol that utilizes normal modes derived from the anisotropic network model for proteins. Deformations along multiple low-frequency modes of motion are used to efficiently sample collective conformational changes in the presence of explicit membrane and water environment, consistent with interresidue interactions. We identify two highly stable regions in rhodopsin, one clustered near the chromophore, the other near the cytoplasmic ends of transmembrane helices H1, H2, and H7. Due to redistribution of interactions in the neighborhood of retinal upon stabilization of the trans form, local structural rearrangements in the adjoining H3-H6 residues are efficiently propagated to the cytoplasmic end of these particular helices. In the structures obtained by our simulations, all-trans retinal interacts with Cys¹⁶⁷ on H4 and Phe²⁰³ on H5, which were not accessible in the dark state, and exhibits stronger interactions with H5, while some of the contacts made (in the cis form) with H6 are lost.     

Halorhodopsin and sensory rhodopsin contain a C6-C7 s-trans retinal chromophore.

Halorhodopsin (HR) and sensory rhodopsin (SR) have been regenerated with retinal analogues that are covalently locked in the 6-s-cis or 6-s-trans conformations. Both pigments regenerate more completely with the locked 6-s-trans retinal and produce analogue pigments with absorption maxima (577 nm for HR and 592 nm for SR) nearly identical to those of the native pigments (577 and 587 nm). This indicates that HR and SR bind retinal in the 6-s-trans conformation. The opsin shift for the locked 6-s-trans analogue in HR is 1,200 cm-1 less than that for the native chromophore (5,400 cm-1). The opsin shift for the 6-s-trans analogue in SR is 1,100 cm-1 less than that for the native retinal (5,700 cm-1). This demonstrates that approximately 20% of the opsin shift in these pigments arises from a protein-induced change in the chromophore conformation from twisted 6-s-cis in solution to planar 6-s-trans in the protein. The reduced opsin shift observed for the locked 6-s-cis analogue pigments compared with the locked 6-s-trans pigments may be due to a positive electrostatic perturbation near C7.     

Transverse location of the retinal chromophore of rhodopsin in rod outer segment disc membranes

Diffusion-enhanced fluorescence energy transfer was used to study the structure of photoreceptor membranes from bovine retinal rod outer segments. The fluorescent energy donor was Tb³⁺ chelated to dipicolinate and the acceptor was the 11-cis retinal chromophore of rhodopsin in vesicles made from disc membranes. The rapid-diffusion limit for energy transfer was attained in these experiments because of the long excited state lifetime of the terbium donor (~2 ms). Under these conditions, energy transfer is very sensitive to a, the distance of closest approach between the donor and acceptor (Thomas et al., 1978). Vesicles containing terbium dipicolinate in their inner aqueous space were prepared by sonicating disc membranes in the presence of this chelate and chromatographing this mixture on a gel filtration column. The sidedness of rhodopsin in these vesicles was the same as in native disc membranes. The transfer efficiency from terbium to retinal in this sample was 43%. For an R₀ value of 46.7 Å and an average vesicle diameter of 650 Å, this corresponds to an a value of 22 Å from the inner aqueous space of the vesicle. The distance of closest approach from the external aqueous space, determined by adding terbium dipicolinate to a suspension of already formed vesicles, was found to be 28 Å. These values of a show that the retinal chromophore is far from both aqueous surfaces of the disc membrane. Hence, the transverse location of the retinal chromophore is near the center of the hydrophobic core of the disc membrane. These findings suggest that conformational changes induced by photoisomerization are transmitted through a distance of at least 20 Å within rhodopsin to trigger subsequent events in visual excitation.     

Deactivation of rhodopsin in the transition from the signaling state meta II to meta III involves a thermal isomerization of the retinal chromophore C[double bond]D

Light-induced isomerization of rhodopsin's retinal chromophore to the activating all-trans geometry initializes the formation of the active receptor state, Meta II. In the absence of peripheral regulatory proteins, the activity of Meta II is switched off spontaneously by two independent pathways: either by hydrolysis of the retinal Schiff base and dissociation of the light receptor into apoprotein opsin plus free retinal or by formation of Meta III, an inactive species with intact retinal protonated Schiff base absorbing at 470 nm. By FTIR spectroscopy on rhodopsin reconstituted with isotopically labeled chromophores in combination with quantum mechanical DFT calculations, we show that the deactivating step during formation of Meta III involves a thermal isomerization of the chromophore C[double bond]N, such that the chromophore in Meta III is all-trans-15-syn. This isomerization step is catalyzed by the protein environment and proceeds via Meta I, as suggested by its dependence on pH and on properties of the lipid/detergent environment of the protein. In the long term, Meta III decays likewise to opsin and free retinal by slow hydrolysis of the Schiff base.     

Activation of Chlamydomonas rhodopsin in vivo does not require isomerization of retinal

The unicellular eukaryote Chlamydomonas reinhardtii is a phototactic alga that swims toward or away from light, using rhodopsin as the photopigment. The activity of retinal analogues was tested in the mutant FN68, which has high phototactic sensitivity only after incubation with retinal or analogues of retinal. Analogues prevented from isomerizing about the 7-ene, 9-ene, 11-ene, 13-ene, or 15-ene (C = N+H) bonds retained full activity. Also, bleaching, protonation of the N, and a stable geometrically altered chromophore are not required for full activity. An attractive hypothesis is that charge redistribution in the excited state of retinal directly triggers the activity of rhodopsin.     

Structure of the retinal chromophore in the hRL intermediate of halorhodopsin from resonance raman spectroscopy

Time-resolved resonance Raman spectra of the hRL intermediate of halorhodopsin have been obtained. The structurally sensitive fingerprint region of the hRL spectrum is very similar to that of bacteriorhodopsin's L550 intermediate, which is known to have a 13-cis configuration. This indicates that hRL contains a 13-cis chromophore and that an all-trans----13-cis isomerization occurs in the halorhodopsin photocycle. hRL exhibits a Schiff base stretching mode at 1644 cm-1, which shifts to 1620 cm-1 in D2O. This demonstrates that the Schiff base linkage to the protein is protonated. The insensitivity of the C-C stretching mode frequencies to N-deuteriation suggests that the Schiff base configuration is anti. The 24 cm-1 shift of the Schiff base mode in D2O indicates that the Schiff base proton in hRL has a stronger hydrogen-bonding interaction with the protein than does hR578.