Coupling of protonation switches during rhodopsin activation

Recent studies of the activation mechanism of rhodopsin involving Fourier-transform infrared spectroscopy and a combination of chromophore modifications and site-directed mutagenesis reveal an allosteric coupling between two protonation switches. In particular, the ring and the 9-methyl group of the all-trans retinal chromophore serve to couple two proton-dependent activation steps: proton uptake by a cytoplasmic network between transmembrane (TM) helices 3 and 6 around the conserved ERY (Glu-Arg-Tyr) motif and disruption of a salt bridge between the retinal protonated Schiff base (PSB) and a protein counterion in the TM core of the receptor. Retinal analogs lacking the ring or 9-methyl group are only partial agonists--the conformational equilibrium between inactive Meta I and active Meta II photoproduct states is shifted to Meta I. An artificial pigment was engineered, in which the ring of retinal was removed and the PSB salt bridge was weakened by fluorination of C14 of the retinal polyene. These modifications abolished allosteric coupling of the proton switches and resulted in a stabilized Meta I state with a deprotonated Schiff base (Meta I(SB)). This state had a partial Meta II-like conformation due to disruption of the PSB salt bridge, but still lacked the cytoplasmic proton uptake reaction characteristic of the final transition to Meta II. As activation of native rhodopsin is known to involve deprotonation of the retinal Schiff base prior to formation of Meta II, this Meta I(SB) state may serve as a model for the structural characterization of a key transient species in the activation pathway of a prototypical G protein-coupled receptor.     

Modulating rhodopsin receptor activation by altering the pKa of the retinal Schiff base

The visual pigment rhodopsin is a seven-transmembrane (7-TM) G protein-coupled receptor (GPCR). Activation of rhodopsin involves two pH-dependent steps: proton uptake at a conserved cytoplasmic motif between TM helices 3 and 6, and disruption of a salt bridge between a protonated Schiff base (PSB) and its carboxylate counterion in the transmembrane core of the receptor. Formation of an artificial pigment with a retinal chromophore fluorinated at C14 decreases the intrinsic pKa of the PSB and thereby destabilizes this salt bridge. Using Fourier transform infrared difference and UV-visible spectroscopy, we characterized the pH-dependent equilibrium between the active photoproduct Meta II and its inactive precursor, Meta I, in the 14-fluoro (14-F) analogue pigment. The 14-F chromophore decreases the enthalpy change of the Meta I-to-Meta II transition and shifts the Meta I/Meta II equilibrium toward Meta II. Combining C14 fluorination with deletion of the retinal beta-ionone ring to form a 14-F acyclic artificial pigment uncouples disruption of the Schiff base salt bridge from transition to Meta II and in particular from the cytoplasmic proton uptake reaction, as confirmed by combining the 14-F acyclic chromophore with the E134Q mutant. The 14-F acyclic analogue formed a stable Meta I state with a deprotonated Schiff base and an at least partially protonated protein counterion. The combination of retinal modification and site-directed mutagenesis reveals that disruption of the protonated Schiff base salt bridge is the most important step thermodynamically in the transition from Meta I to Meta II. This finding is particularly important since deprotonation of the retinal PSB is known to precede the transition to the active state in rhodopsin activation and is consistent with models of agonist-dependent activation of other GPCRs.     

Activity switches of rhodopsin

Rhodopsin, the visual pigment of the rod photoreceptor cell contains as its light-sensitive cofactor 11-cis retinal, which is bound by a protonated Schiff base between its aldehyde group and the Lys296 side chain of the apoprotein. Light activation is achieved by 11-cis to all-trans isomerization and subsequent thermal relaxation into the active, G protein-binding metarhodopsin II state. Metarhodopsin II decays via two parallel pathways, which both involve hydrolysis of the Schiff base eventually to opsin and released all-trans retinal. Subsequently, rhodopsin's dark state is regenerated by a complicated retinal metabolism, termed the retinoid cycle. Unlike other retinal proteins, such as bacteriorhodopsin, this regeneration cycle cannot be short cut by light, because blue illumination of active metarhodopsin II does not lead back to the ground state but to the formation of largely inactive metarhodopsin III. In this review, mechanistic details of activating and deactivating pathways of rhodopsin, particularly concerning the roles of the retinal, are compared. Based on static and time-resolved UV/Vis and FTIR spectroscopic data, we discuss a model of the light-induced deactivation. We describe properties and photoreactions of metarhodopsin III and suggest potential roles of this intermediate for vision.     

MAGIC ANGLE SPINNING NMR STUDIES ON THE METARHODOPSIN II INTERMEDIATE OF BOVINE RHODOPSIN: EVIDENCE FOR AN UNPROTONATED SCHIFF BASE

Magic angle spinning (MAS)13C-NMR spectra of the metarhodopsin II intermediate have been obtained using bovine rhodopsin regenerated with retinal 13C-labeled at the C-13 and C-15 positions to investigate the protonation state of the retinal Schiff base linkage. The 13C-labeled rhodopsin was reconstituted into 1,2-dipalmitoleoylphosphatidylcholine bilayers to increase the amount of meta II trapped at low temperature. Both the 13C-15 (159.2 ppm) and 13C-13 (144.0 ppm) isotropic chemical shifts are characteristic of an unprotonated Schiff base, while the 13C-15 shift is significantly different from that of retinal (191 ppm) or a tetrahedral carbinolamine group (70-90 ppm) previously proposed as an intermediate in the hydrolysis of the Schiff base at the meta II stage. This rules out the possibility that meta II non-covalently binds retinal or is a carbinolamine intermediate and provides convincing evidence that Schiff base deprotonation occurs in the meta I-meta II transition, an event that is likely to be important in triggering the activation of transducin.     

All-trans-N-retinylidenetryptamine Schiff base in surfactant solubilized water pools in heptane—a fluorescence study

All-trns-N-retinylidenetryptamine Schiff base was incorporated into aerosol-OT (AOT, sodium bis(2-ethylhexyl)sulphosuccinate)/heptane reverse micelles. This micellar system was used as a model to study the retinal-tryptophan interactions in retinal proteins. The retinylidene Schiff base remains stable in the presence of reverse micelle-solubilized water pools. Partition coefficient and microviscosity measurements show that the Schiff base is located in the micellar interphase. The results are discussed in terms of the interaction between the retinylidene chromophore and the active site environment of rhodopsin and bacteriorhodopsin. In the present model, the quencher and emitting units are covalently attached, and are separated by two carbon spacer units. The fluorescence emission data obtained for the micelle-intercalated Schiff base chromophore are compared with the fluorescence of the native protein and intermediates in the photochemical cycle of bacteriofhodopsin. A comparison of the data obtained for tryptamine and the Schiff base with the results available for bacteriorhodopsin and bacterioopsin reveals that there is a large degree of quenching on intercalation of the retinylidene chromophore in the vicinity of the fluorophore. Evidence provided by this model suggests that energy transfer to retinal can occur from tryptophan residues located in the retinal pocket in the native protein. Thus the retinylidene unit can act as a quencher of the energy of tryptophan, the nature and extent of which may depend on the conformation and relative orientation of the protein-bound fluorophore.     

Structural and functional properties of metarhodopsin III: recent spectroscopic studies on deactivation pathways of rhodopsin

The activation of rhodopsin has been the focus of researchers over the past decades, revealing many aspects of the activation pathways of this prototypical G protein-coupled receptor on a molecular level, starting with the light-dependent isomerization of its retinal chromophore from 11-cis to all-trans and leading eventually to the large scale helix movements in the transition to the active receptor state, Meta II. Comparatively little is known, however, on the deactivation pathways of the light receptor, which represent essential steps in maintaining a functional photoreceptor cell. Rhodopsin's active receptor species, Meta II, decays by two fundamentally different pathways, either forming the apoprotein opsin by release of the activating all-trans retinal ligand from its binding pocket, or by a thermal isomerization of this ligand to a less activating species in the transition to metarhodopsin III (Meta III). Both decay products, opsin and Meta III, are largely inactive under physiological conditions, yet they do not restore the complete inactivity of the dark state. Although some properties of Meta III have been described already in the 1960s, its molecular nature and the pathways of its formation have remained rather obscure. In this review, we focus on recent studies from our laboratories, which have provided a major progress in our understanding of the Meta III deactivation pathway and its potential physiological roles. Using Fourier-transform infrared (FTIR) difference spectroscopy in combination with a variety of other spectroscopic and biochemical techniques and quantum chemical calculations, we have developed a general picture of the interplay between the retinal ligand and the receptor protein, which is compared to similar reaction mechanisms in invertebrate photoreceptors and microbial retinal proteins.     

Primary events in dim light vision: a chemical and spectroscopic approach toward understanding protein/chromophore interactions in rhodopsin

The visual pigment rhodopsin (bovine) is a 40 kDa protein consisting of 348 amino acids, and is a prototypical member of the subfamily A of G protein-coupled receptors (GPCRs). This remarkably efficient light-activated protein (quantum yield = 0.67) binds the chromophore 11-cis-retinal covalently by attachment to Lys296 through a protonated Schiff base. The 11-cis geometry of the retinylidene chromophore keeps the partially active opsin protein locked in its inactive state (inverse agonist). Several retinal analogs with defined configurations and stereochemistry have been incorporated into the apoprotein to give rhodopsin analogs. These incorporation results along with the spectroscopic properties of the rhodopsin analogs clarify the mode of entry of the chromophore into the apoprotein and the biologically relevant conformation of the chromophore in the rhodopsin binding site. In addition, difference UV, CD, and photoaffinity labeling studies with a 3-diazo-4-oxo analog of 11-cis-retinal have been used to chart the movement of the retinylidene chromophore through the various intermediate stages of visual transduction.     

Light Dynamics of the Retinal-Disease-Relevant G90D Bovine Rhodopsin Mutant

The RHO gene encodes the G-protein-coupled receptor (GPCR) rhodopsin. Numerous mutations associated with impaired visual cycle have been reported; the G90D mutation leads to a constitutively active mutant form of rhodopsin that causes CSNB disease. We report on the structural investigation of the retinal configuration and conformation in the binding pocket in the dark and light-activated state by solution and MAS-NMR spectroscopy. We found two long-lived dark states for the G90D mutant with the 11-cis retinal bound as Schiff base in both populations. The second minor population in the dark state is attributed to a slight shift in conformation of the covalently bound 11-cis retinal caused by the mutation-induced distortion on the salt bridge formation in the binding pocket. Time-resolved UV/Vis spectroscopy was used to monitor the functional dynamics of the G90D mutant rhodopsin for all relevant time scales of the photocycle. The G90D mutant retains its conformational heterogeneity during the photocycle.     

Alpha-retinals as rhodopsin chromophores--preference for the 9-Z configuration and partial agonist activity

The visual pigment rhodopsin, the photosensory element of the rod photoreceptor cell in the vertebrate retina, shows in combination with an endogenous ligand, 11-Z retinal, an astonishing photochemical performance. It exhibits an unprecedented quantum yield (0.67) in a highly defined and ultrafast photoisomerization process. This triggers the conformational changes leading to the active state Meta(rhodopsin) II. Retinal is covalently bound to Lys-296 of the protein opsin in a protonated Schiff base. The resulting positive charge delocalization over the terminal part of the polyene chain of retinal creates a conjugation defect that upon photoexcitation moves to the opposite end of the polyene. Shortening the polyene as in 4,5-dehydro,5,6-dihydro (alpha), 5,6-dihydro or 7,8-dihydro-analogs might facilitate photoisomerization of a 9-Z and a 11-Z bond. Here we describe pigment analogs generated with bovine opsin and 11-Z or 9-Z 4,5-dehydro,5,6-dihydro-retinal that were further characterized by UV-Vis and FTIR spectroscopy. The preference of opsin for native 11-Z retinal over the 9-Z isomer is reversed in 4,5-dehydro,5,6-dihydro-retinal. 9-Z 4,5-dehydro,5,6-dihydro-retinal readily generated a photosensitive pigment. This modification has no effect on the quantum yield, but affects the Batho<-->blueshifted intermediate (BSI) equilibrium and leads to a strong decrease in the G-protein activation rate because of a downshift of the pK(a) of the Meta I<-->Meta II equilibrium.     

Rhodopsin regeneration is accelerated via noncovalent 11-cis retinal-opsin complex--a role of retinal binding pocket of opsin

The regeneration of bovine rhodopsin from its apoprotein opsin and the prosthetic group 11-cis retinal involves the formation of a retinylidene Schiff base with the epsilon-amino group of the active lysine residue of opsin. The pH dependence of a Schiff base formation in solution follows a typical bell-shaped profile because of the pH dependence of the formation and the following dehydration of a 1-aminoethanol intermediate. Unexpectedly, however, we find that the formation of rhodopsin from 11-cis retinal and opsin does not depend on pH over a wide pH range. These results are interpreted by the Matsumoto and Yoshizawa (Nature 258 [1975] 523) model of rhodopsin regeneration in which the 11-cis retinal chromophore binds first to opsin through the beta-ionone ring, followed by the slow formation of the retinylidene Schiff base in a restricted space. We find the second-order rate constant of the rhodopsin formation is 6100+/-300 mol(-1) s(-1) at 25 degrees C over the pH range 5-10. The second-order rate constant is much greater than that of a model Schiff base in solution by a factor of more than 10(7). A previous report by Pajares and Rando (J Biol Chem 264 [1989] 6804) suggests that the lysyl epsilon-NH(2) group of opsin is protonated when the beta-ionone ring binding site is unoccupied. The acceleration of the Schiff base formation in rhodopsin is explained by stabilization of the deprotonated form of the lysyl epsilon-NH(2) group which might be induced when the beta-ionone ring binding site is occupied through the noncovalent binding of 11-cis retinal to opsin at the initial stage of rhodopsin regeneration, followed by the proximity and orientation effect rendered by the formation of noncovalent 11-cis retinal-opsin complex.     

Light Dynamics of the Retinal‐Disease‐Relevant G90D Bovine Rhodopsin Mutant

The RHO gene encodes the G‐protein‐coupled receptor (GPCR) rhodopsin. Numerous mutations associated with impaired visual cycle have been reported; the G90D mutation leads to a constitutively active mutant form of rhodopsin that causes CSNB disease. We report on the structural investigation of the retinal configuration and conformation in the binding pocket in the dark and light‐activated state by solution and MAS‐NMR spectroscopy. We found two long‐lived dark states for the G90D mutant with the 11‐cis retinal bound as Schiff base in both populations. The second minor population in the dark state is attributed to a slight shift in conformation of the covalently bound 11‐cis retinal caused by the mutation‐induced distortion on the salt bridge formation in the binding pocket. Time‐resolved UV/Vis spectroscopy was used to monitor the functional dynamics of the G90D mutant rhodopsin for all relevant time scales of the photocycle. The G90D mutant retains its conformational heterogeneity during the photocycle.     

Interaction of chromophore, 11-<Emphasis Type="Italic">cis</Emphasis>-retinal,with amino acid residues of the visual pigment rhodopsin in the region of protonated Schiff base: A molecular dynamics study

A molecular dynamics study of the dark adapted visual pigment rhodopsin molecule was carried out. The interaction of the chromophore group, 11-cis-retinal, with the nearest amino acid residues in the chromophore center of the molecule, namely, in the region of the protonated Schiff base linkage, was analyzed. Most likely, the interaction of the CH=NH bond with the negatively charged amino acid residue Glu113 cannot be described as a simple electrostatic interaction of two oppositely charged groups. One can propose that not only Glu113 but also Glu181 and Ser186 are involved in stabilization of the protonated Schiff base linkage. Accord-ing to calculations, Glu181 interacts, as the counter-ion, with the Schiff base indirectly via Ser186. The intramolecular mechanisms of protonated Schiff base stabilization in rhodopsin are discussed. Published in Russian in Izvestiya Akademii Nauk. Seriya Khimicheskaya, No. 1, pp. 19–27, January, 2007.     

Absorption studies of neutral retinal Schiff base chromophores

The neutral retinal Schiff base is connected to opsin in UV sensing pigments and in the blue-shifted meta-II signaling state of the rhodopsin photocycle. We have designed and synthesized two model systems for this neutral chromophore and have measured their gas-phase absorption spectra in the electrostatic storage ring ELISA with a photofragmentation technique. By comparison to the absorption spectrum of the protonated retinal Schiff base in vacuo, we found that the blue shift caused by deprotonation of the Schiff base is more than 200 nm. The absorption properties of the UV absorbing proteins are thus largely determined by the intrinsic properties of the chromophore. The effect of approaching a positive charge to the Schiff base was also studied, as well as the susceptibility of the protonated and unprotonated chromophores to experience spectral shifts in different solvents.     

Mechanism of G-protein activation by rhodopsin

Rhodopsin is a member of the family of G-protein-coupled receptors (GPCRs), and is an excellent molecular switch for converting light signals into electrical response of the rod photoreceptor cells. Light initiates cis-trans isomerization of the retinal chromophore of rhodopsin and leads to the formation of several thermolabile intermediates during the bleaching process. Recent investigations have identified spectrally distinguishable two intermediate states that can interact with the retinal G-protein, transducin, and have elucidated the functional sharing of these intermediates. The initial contact with GDP-bound G-protein occurs in the meta-Ib intermediate state, which has a protonated Schiff base as its chromophore. The meta-Ib intermediate in the complex with the G-protein converts to the meta-II intermediate with releasing GDP from the alpha-subunit of the G protein. Meta-II has a de-protonated Schiff base chromophore and induces binding of GTP to the alpha-subunit of the G-protein. Thus, the GDP-GTP exchange reaction, namely G-protein activation, by rhodopsin proceeds through at least two steps, with conformational changes in both rhodopsin and the G-protein.     

7,8-dihydro retinals outperform the native retinals in conferring photosensitivity to visual opsin

The visual pigment rhodopsin presents an astonishing photochemical performance. It exhibits an unprecedented quantum yield (0.67) in a highly defined and ultrafast photoisomerization process. This triggers the conformational changes leading to the active state Meta II of this G protein-coupled receptor. The responsible ligand, retinal, is covalently bound to Lys-296 of the protein in a protonated Schiff base. The resulting positive charge delocalization over the terminal part of the polyene chain of retinal creates a conjugation defect that upon photoexcitation moves to the opposite end of the polyene. Shortening the polyene as in 5,6-dihydro- or 7,8-dihydro analogues might facilitate photoisomerization of a 9-Z and an 11-Z bond. Here we describe pigment analogues generated with bovine opsin and 11-Z 7,8-dihydro retinal or 9-Z 7,8-dihydro retinal. Both isomers readily generate photosensitive pigments that differ remarkably in spectral properties from the native pigments. In addition, in spite of the more flexible 7,8 single bond, both analogue pigments exhibit strikingly efficient photoisomerization while largely maintaining the activity toward the G-protein. These results bear upon the activation of ligand-gated signal transducers such as G protein-coupled receptors.     

Recent bioorganic studies on rhodopsin and visual transduction

Rhodopsin, the pigment responsible for vision in animals, insect and fish is a typical G protein (guanyl-nucleotide binding protein) consisting of seven transmembrane alpha helices and their interconnecting extramembrane loops. In the case of bovine rhodopsin, the best studied of the visual pigments, the chromophore is 11-cis retinal attached to the terminal amino group of Lys296 through a protonated Schiff base linkage. Photoaffinity labeling with a 3-diazo-4-oxo-retinoid shows that C-3 of the ionone ring moiety is close to Trp265 in helix F (VI) in dark inactivated rhodopsin. Irradiation causes a cis to trans isomerization of the 11-cis double bond giving rise to the highly strained intermediate bathorhodopsin. This undergoes a series of thermal relaxation through lumi-, meta-I and meta-II intermediates after which the retinal chromophore is expelled from the opsin binding pocket. Photoaffinity labeling performed with 3-diazo-4-oxoretinal at -196 degrees C for batho-, -80 degrees C for lumi-, -40 degrees C for meta-I, and 0 degrees C for meta-II rhodopsin showed that in bathorhodopsin the ring is still close to Trp265. However, in lumi-, meta-I and meta-II intermediates crosslinking occurs unexpectedly at A169 in helix D (IV). This shows that large movements in the helical arrangements and a flip over of the ring moiety accompanies the transduction (or bleaching) process. These changes in retinal/opsin interactions are necessarily accompanied by movements of the extramembrane loops, which in turn lead to activation of the G protein residing in the cytoplasmic side. Of the numerous G protein coupled receptors, this is the first time that the outline of transduction pathway has been clarified.     

Protein design: reengineering cellular retinoic acid binding protein II into a rhodopsin protein mimic

Rational redesign of the binding pocket of Cellular Retinoic Acid Binding Protein II (CRABPII) has provided a mutant that can bind retinal as a protonated Schiff base, mimicking the binding observed in rhodopsin. The reengineering was accomplished through a series of choreographed manipulations to ultimately orient the reactive species (the epsilon-amino group of Lys132 and the carbonyl of retinal) in the proper geometry for imine formation. The guiding principle was to achieve the appropriate Bürgi-Dunitz trajectory for the reaction to ensue. Through crystallographic analysis of protein mutants incapable of forming the requisite Schiff base, a highly ordered water molecule was identified as a key culprit in orienting retinal in a nonconstructive manner. Removal of the ordered water, along with placing reinforcing mutations to favor the desired orientation of retinal, led to a triple mutant CRABPII protein capable of nanomolar binding of retinal as a protonated Schiff base. The high-resolution crystal structure of all-trans-retinal bound to the CRABPII triple mutant (1.2 A resolution) unequivocally illustrates the imine formed between retinal and the protein.     

ORIENTATION OF AROMATIC RESIDUES IN RHODOPSIN. ROTATION OF ONE TRYPTOPHAN UPON THE META I→META II TRANSITION AFTER ILLUMINATION

Abstract— Linear dichroism measurements have been performed in the visible and the UV on suspensions of intact retinal rod outer segments, isolated from frog and from cattle retinas and oriented by a magnetic field. In the UV a sharp double peaked signal is observed around 290 nm. It is characteristic of a tryptophan residue having its ¹L_b transition oriented preferentially perpendicular to the membrane plane. Only one tryptophan residue per rhodopsin molecule seems to be involved, and this is insufficient to account for the diamagnetic anisotropy of the rods which causes their orientation. Upon bleaching one observes a rotation of this tryptophan coupled to the Meta I →Meta II transition, and the rotation is reversed in the next step Meta II → Meta III. The correlation with other spectral changes suggests that this tryptophan is in close relation with the retinal chromophore.     

STRUCTURE OF HYPSORHODOPSIN: ANALYSIS BY FOURIER TRANSFORM INFRARED SPECTROSCOPY AT 10 K

Abstract— Vibrational bands of hypsorhodopsin in the difference Fourier transform infrared spectra were identified as the bands which arose after formation of isorhodopsin by successive irradiations of bovine rhodopsin at 10 K with >500 nm light, and also as the bands disappeared upon conversion to bathorhodopsin by warming. The chromophore bands were assigned by the bands which shifted upon deuterium substitution of the polyene chain of the retinylidene chromophore. The presence of chromophore bands which shift by D₂O exchange clearly shows that the Schiff base chromophore of hypsorhodopsin is protonated. The amide I bands and several other protein bands of hypsorhodopsin appeared at the same frequencies as those of bathorhodopsin, but they are different from those of rhodopsin and isorhodopsin. Furthermore, like bathorhodopsin, hypsorhodopsin displays the C_l—H out-of-plane bending mode which is weakly coupled with C₁₂-_-–H out-of-plane mode. These facts show that hypsorhodopsin has a chromophore conformation and chromophore-opsin interaction more similar to bathorhodopsin than to rhodopsin and isorhodopsin.     

Constraints of opsin structure on the ligand-binding site: studies with ring-fused retinals

Ring-fused retinal analogs were designed to examine the hula-twist mode of the photoisomerization of the 9-cis retinylidene chromophore. Two 9-cis retinal analogs, the C11-C13 five-membered ring-fused and the C12-C14 five-membered ring-fused retinal derivatives, formed the pigments with opsin. The C11-C13 ring-fused analog was isomerized to a relaxed all-trans chromophore (lambda(max) > 400 nm) at even -269 degrees C and the Schiff base was kept protonated at 0 degrees C. The C12-C14 ring-fused analog was converted photochemically to a bathorhodopsin-like chromophore (lambda(max) = 583 nm) at -196 degrees C, which was further converted to the deprotonated Schiff base at 0 degrees C. The model-building study suggested that the analogs do not form pigments in the retinal-binding site of rhodopsin but form pigments with opsin structures, which have larger binding space generated by the movement of transmembrane helices. The molecular dynamics simulation of the isomerization of the analog chromophores provided a twisted C11-C12 double bond for the C12-C14 ring-fused analog and all relaxed double bonds with a highly twisted C10-C11 bond for the C11-C13 ring-fused analog. The structural model of the C11-C13 ring-fused analog chromophore showed a characteristic flip of the cyclohexenyl moiety toward transmembrane segments 3 and 4. The structural models suggested that hula twist is a primary process for the photoisomerization of the analog chromophores.