π-Cation interactions as the origin of the weak absorption at 532 nm observed in tryptophan-containing polypeptides

We have previously reported that bovine serum albumin (BSA) and other proteins that do not contain prosthetic groups exhibited a weak light absorption in the visible, only detectable by pulsed laser-induced optoacoustic spectroscopy (LIOAS). Human serum albumin (HSA) exhibited signals 25% higher than those observed with BSA. Signals comparable to those obtained with BSA were observed with poly(L-Trp, L-Lys), poly(L-Trp, L-Arg) or poly(L-Trp, L-Orn) at pH 7.0. No signals were obtained when tryptophan was replaced by other amino acids or when free tryptophan or the tripeptide Lys-Trp-Lys was assayed (pH 7.0). Tryptophan in HCl 5 N produced LIOAS signals similar to those produced by tryptophan-containing copolymers. Moreover, the absorption peak could be observed in a UV-VIS spectrophotometer. Therefore, the LIOAS signals obtained with BSA, HSA, and tryptophan-containing random copolymers may be attributed to a new transition of the indole moiety of their tryptophan residues when "protonated". Tryptophan residues of proteins are known to participate in π-cation interactions, which are important in protein stability and function. As a matter of fact, HSA and BSA contain an internal tryptophan in close proximity to lysine and arginine residues and therefore suitable for π-cation interactions. The strength of this type of interaction strongly depends on distances and relative orientations of both amino acid residues. Accordingly, these interactions should be highly sensitive to conformational changes. Based on preliminary results that have shown that LIOAS signal at 532 nm depended on the aggregation state of BSA and/or on the oxidation state of its Cys-34, we postulate that the LIOAS signal observed with proteins and tryptophan-containing polypeptides are related to Trp-Lys or Trp-Arg interactions and that the intensity of the signal depends on the strength of such interactions.

Heterologous expression and characterization of recombinant phytochrome from the green alga Mougeotia scalaris

The full-length apoprotein (124 kDa) and the chromophore-binding N-terminal half (66 kDa) of the phytochrome of the unicellular green alga Mougeotia scalaris have been heterologously expressed in the methylotrophic yeast Pichia pastoris. Assembly with the tetrapyrrole phycocyanobilin (PCB) yielded absorption maxima (for the full-length protein) at 646 and 720 nm for red- and far-red absorbing forms of phytochrome (Pr and Pfr), respectively, whereas the maxima of the N-terminal 66 kDa domain are slightly blueshifted (639 and 714 nm, Pr and Pfr, respectively). Comparison with an action spectrum reported earlier gives evidence that in Mougeotia, as formerly reported for the green alga Mesotaenium caldariorum, PCB constitutes the genuine chromophore. The full-length protein, when converted into its Pfr form and kept in the dark, reverted rapidly into the Pr form (lifetimes of 1 and 24 min, ambient temperature), whereas the truncated chromopeptide (66 kDa construct) was more stable and converted into Pr with time constants of 18 and 250 min. Also, time-resolved analysis of the light-induced Pfr formation revealed clear differences between both recombinant chromoproteins in the various steps involved. The full-length phytochrome showed slower kinetics in the long milliseconds-to-seconds time domain (with dominant Pfr formation processes of ca 130 and 800 ms), whereas for the truncated phytochrome the major component of Pfr formation had a lifetime of 32 ms.

Time-resolved thermodynamic analysis of the oat phytochrome A phototransformation. A photothermal beam deflection study

The time-resolved enthalpy and the structural volume changes after excitation of native oat phytochrome A were studied in the micro- to milliseconds range by photothermal beam deflection (PBD), a technique that follows the time-resolved refractive index changes upon decay of the excited species. The first set of intermediates, I700(1) and I700(2), stores ca 83% of the energy of the first excited state, in agreement with previous optoacoustic data, whereas the second set stores only ca 18%. The temperature dependence of the amplitudes ratio for the optical absorbances of the (I700(1) + I700(2)) intermediates set is explained on the basis of the thermochromic equilibrium between Pr,657 and Pr,672, which also is in line with the present PBD data. These data were best fitted with a parallel mechanism (with equal yield in each branch) for the production of the first set of intermediates, I700(1) and I700(2), as well as the second set of intermediates, Ibl1 and Ibl2. Thus, the final steps toward Pfr should be largely driven by positive entropic changes brought about by protein movements, in line with previous resonance Raman data. For the production of the first set of intermediates (I700(1) and I700(2)) an expansion of 18 +/- 13 mL mol-1 was determined, and a further expansion > or = 7 mL mol-1 was estimated for the decay from I700(1) to the set of Ibl intermediates, indicating that the far red-absorbing form of phytochrome (Pfr) has a larger volume than the red-absorbing form of phytochrome. This is in agreement with previous chromatographic and circular dichroism data according to which Pfr shows a larger volume and the chromophore shows a higher accessibility, respectively, in the Pfr state.

Thermodynamics of the early steps in the photocycle of Natronobacterium pharaonis halorhodopsin. Influence of medium and of anion substitution

The enthalpy (delta H) and structural volume changes (delta V) associated with the formation and decay of the early intermediate K600 in the photocycle of Natronobacterium pharaonis halorhodopsin (pHR), an inward-directed anion pump, were obtained by laser-induced optoacoustic spectroscopy. A large expansion is associated with K600 formation, its value depending on the medium and on the anion (Cl-, NO3-, Br-, I-). A smaller expansion is associated with K600 decay to L520. A contraction is found for the same step in the case of the azide-loaded pHR which is an efficient outward-directed proton pump. Thus, the conformational changes in L520 determine the direction and sign of charge translocation. The linear correlation between delta H and delta V for chloride-loaded pHR observed upon mild medium variations is attributed to enthalpy-entropy compensation effects and allows the calculation of the free-energy changes, delta GK = (97 +/- 16) kJ/mol and delta GKL = -(2 +/- 2) kJ/mol. Different from other systems, delta S correlates negatively with delta V in the first steps of the pHR photocycle. Thus, the space around the anion becomes larger and more rigid during each of these two steps. The photocycle quantum yield was 0.52 for chloride-pHR as measured by laser flash photolysis.

Time-resolved thermodynamic changes photoinduced in 5,12-trans-locked bacteriorhodopsin. Evidence that retinal isomerization is required for protein activation

Structural volume changes upon excitation of isomerization-blocked 5,12-trans-locked bacteriorhodopsin (bR) (bacterio-opsin + 5-12-trans-locked retinal) were studied using photothermal methods. The very small prompt expansion detected using laser-induced optoacoustics (0.3 mL/mol of absorbed photons) is assigned to a charge reorganization in the chromophore protein pocket concomitant with the formation of the intermediate T5.12. The subsequent contraction associated with a 300 ns lifetime is assigned to protein movements required to reach the entire chromoprotein free energy minimum, after the 17 ps optical decay of T5.12. The volume changes comprise the entropy of medium rearrangement during T5.12 formation and decay. The slow changes detected in previous studies by atomic force microscopy might be explained by the slowing down of movements in films containing 5,12-trans-locked bR. Photothermal beam deflection data with the 5,12-trans-locked bR suspensions indicate no further changes in microseconds to hundreds of milliseconds. Thus, all the absorbed energy is either released to the solution as heat or used for entropy changes within the first 300 ns after the pulse, supporting the paradigm that isomerization is required for signal transduction in retinal proteins. Bacterio-opsin assembled with all-trans-retinal afforded (similar to data reported with wild-type bR) an expansion of 2.6 mL/mol (assigned to the production of KE) followed by a further expansion of 0.8 mL/mol (KE-->KL; KE, KL, early and late K's) involving no heat loss. For KL decay to L, a contraction of 6 mL/mol of phototransformed reconstituted all-trans bR was determined.

Resonance Raman spectroscopic study of the tryptic 39-kDa fragment of phytochrome

The 39-kDa fragment of oat phytochrome phyA, obtained by tryptic digestion at the amino acids 65 and 425, was studied by resonance Raman spectroscopy. The parent state P(r) reveals far-reaching similarities with that of the native phytochrome implying that the structures of the tetrapyrrole chromophore and its immediate protein environment are not affected by the proteolysis. However, the resonance Raman spectrum of the final product of the P(r) phototransformation, denoted as P(bl), is more closely related to that of the P(fr) precursor of the native phytochrome, i.e. meta-R(C), rather than to that of P(fr) itself. The resonance Raman spectra indicate a high conformational flexibility of the chromophore in P(bl) so that, unlike in P(fr), the tetrapyrrole rings C and D adopt a largely coplanar conformation. The protein interactions with ring D of the chromophore, which in the native phytochrome stabilize the specific chromophore structure of P(fr), cannot be established in the 39-kDa fragment due to the lack of the major C-terminal part of the protein. These findings, furthermore, support the view that the meta-R(C)-->P(fr) transition is associated with a coupling of chromophore and protein structural changes that represent crucial events for the photoactivation of phytochrome.

Photodecarboxylation of ketoprofen in aqueous solution. A time-resolved laser-induced optoacoustic study

The photodecarboxylation reaction of 2-(3-benzoylphenyl)propionate (ketoprofen anion, KP-) was studied in water and in 0.1 M phosphate buffer solutions in the pH range 5.7-11.0 by laser-induced optoacoustic spectroscopy (LIOAS, T range 9.5-31.6 degrees C). Upon exciting KP- with 355 nm laser pulses under anaerobic conditions, two components in the LIOAS signals with well-separated lifetimes were found (tau 1 < 20 ns; 250 < tau 2 < 500 ns) in the whole pH range, whereas a long-lived third component (4 < tau 3 < 10 microseconds) was only detected at pH < or = 6.1. The heat and structural volume changes accompanying the first step did not depend on pH or on the presence of buffer. The carbanion resulting from prompt decarboxylation within the nanosecond pulse (< 10 ns) drastically reduces its molar volume ([-18.9 +/- 2.0] cm3/mol) with respect to KP- and its enthalpy content is (256 +/- 10) kJ/mol. At acid pH (ca 6), a species is formed with a lifetime in the hundreds of ns. The enthalpy and structural volume change for this species with respect to KP- are (181 +/- 15) kJ/mol and (+0.6 +/- 2.0) cm3/mol, respectively. This species is most likely a neutral biradical formed by protonation of the decarboxylated carbanion, and decays to the final product 3-ethylbenzophenone in several microsecond. At basic pH (ca 11), direct formation of 3-ethylbenzophenone occurs in hundreds of ns involving a reaction with the solvent. The global decarboxylation reaction is endothermic ([45 +/- 15] kJ/mol) and shows an expansion of (+14.5 +/- 0.5) cm3/mol with respect to KP-. At low pH, the presence of buffer strongly affects the magnitude of the structural volume changes associated with intermolecular proton-transfer processes of the long-lived species due to reactions of the buffer anion with the decarboxylated ketoprofen anion.

Aspartate 75 mutation in sensory rhodopsin II from Natronobacterium pharaonis does not influence the production of the K-like intermediate, but strongly affects its relaxation pathway

The early steps in the photocycle of the aspartate 75-mutated sensory rhodopsin II from Natrobacterium pharaonis (pSRII-D75N) were studied by time-resolved laser-induced optoacoustic spectroscopy combined with quantum yield determinations by flash photolysis with optical detection. Similar to the case of pSRII-WT, excitation of pSRII-D75N produces in subnanosecond time a K-like intermediate. Different to the case of K in pSRII-WT, in pSRII-D75N there are two K states. K(E) decays into K(L) with a lifetime of 400 ns (independent of temperature in the range 6.5-52 degrees C) which is optically silent under the experimental conditions of our transient absorption experiments. This decay is concomitant with an expansion of 6.5 ml/mol of produced intermediate. This indicates a protein relaxation not affecting the chromophore absorption. For pSRII-D75N reconstituted into polar lipids from purple membrane, the mutation of Asp-75 by the neutral residue Asn affects neither the K(E) production yield (PhiK(e) 0.51 +/- 0.05) nor the energy stored by this intermediate (E(E)K(E) = 91 +/- 11 kJ/mol), nor the expansion upon its production (DeltaV(R,1) = 10 +/- 0.3 ml/mol). All these values are very similar to those previously determined for K with pSRII-WT in the same medium. The millisecond transient species is attributed to K(L) with a lifetime corresponding to that determined by electronic absorption spectroscopy for K(565). The determined energy content of the intermediates as well as the structural volume changes for the various steps afford the calculation of the free energy profile of the phototransformation during the pSRII-D75N photocycle. These data offer insights regarding the photocycle in pSRII-WT. Detergent solubilization of pSRII-D75N affects the sample properties to a larger extent than in the case of pSRII-WT.

Time-resolved absorption and photothermal measurements with recombinant sensory rhodopsin II from Natronobacterium pharaonis

Purified wild-type sensory rhodopsin II from Natronobacterium pharaonis (pSRII-WT) and its histidine-tagged analog (pSRII-His) were studied by laser-induced optoacoustic spectroscopy (LIOAS) and flash photolysis with optical detection. The samples were either dissolved in detergent or reconstituted into polar lipids from purple membrane (PML). The quantum yield for the formation of the long-lived state M(400) was determined as Phi(M) = 0.5 +/- 0.06 for both proteins. The structural volume change accompanying the production of K(510) as determined with LIOAS was DeltaV(R,1) </= 10 ml for both proteins, assuming Phi(K) >/= Phi(M), indicating that the His tag does not influence this early step of the photocycle. The medium has no influence on DeltaV(R,1), which is the largest so far measured for a retinal protein in this time range (<10 ns). This confirms the occurrence of conformational movements in pSRII for this step, as previously suggested by Fourier transform infrared spectroscopy. On the contrary, the decay of K(510) is an expansion in the detergent-dissolved sample and a contraction in PML. Assuming an efficiency of 1.0, DeltaV(R,2) = -3 ml/mol for pSRII-WT and -4.6 ml/mol for pSRII-His were calculated in PML, indicative of a small structural difference between the two proteins. The energy content of K(510) is also affected by the tag. It is E(K) = (88 +/- 13) for pSRII-WT and (134 +/- 11) kJ/mol for pSRII-His. A slight difference in the activation parameters for K(510) decay confirms an influence of the C-terminal His on this step. At variance with DeltaV(R,1), the opposite sign of DeltaV(R,2) in detergent and PML suggests the occurrence of solvation effects on the decay of K(510), which are probably due to a different interaction of the active site with the two dissolving media.

Protonation state and structural changes of the tetrapyrrole chromophore during the Pr --> Pfr phototransformation of phytochrome: a resonance Raman spectroscopic study

The photoconversion of phytochrome (phytochrome A from Avena satina) from the inactive (Pr) to the physiologically active form (Pfr) was studied by near-infrared Fourier transform resonance Raman spectroscopy at cryogenic temperatures, which allow us to trap the intermediate states. Nondeuterated and deuterated buffer solutions were used to determine the effect of H/D exchange on the resonance Raman spectra. For the first time, reliable spectra of the "bleached" intermediates meta-R(A) and meta-R(C) were obtained. The vibrational bands in the region 1300-1700 cm(-)(1), which is particularly indicative of structural changes in tetrapyrroles, were assigned on the basis of recent calculations of the Raman spectra of the chromophore in C-phycocyanin and model compounds [Kneip, C., Hildebrandt, P., Németh, K., Mark, F., Schaffner, K. (1999) Chem. Phys. Lett. 311, 479-485]. The experimental resonance Raman spectra Pr are compatible with the Raman spectra calculated for the protonated ZZZasa configuration, which hence is suggested to be the chromophore structure in this parent state of phytochrome. Furthermore, marker bands could be identified that are of high diagnostic value for monitoring structural changes in individual parts of the chromophore. Specifically, it could be shown that not only in the parent states Pr and Pfr but also in all intermediates the chromophore is protonated at the pyrroleninic nitrogen. The spectral changes observed for lumi-R confirm the view that the photoreaction of Pr is a Z --> E isomerization of the CD methine bridge. The subsequent thermal decay reaction to meta-R(A) includes relaxations of the CD methine bridge double bond, whereas the formation of meta-R(C) is accompanied by structural adaptations of the pyrrole rings B and C in the protein pocket. The far-reaching similarities between the chromophores of meta-R(A) and Pfr suggest that in the step meta-R(A) --> Pfr the ultimate structural changes of the protein matrix occur.

Differential effects of mutations in the chromophore pocket of recombinant phytochrome on chromoprotein assembly and Pr-to-Pfr photoconversion

Site-directed mutagenesis was performed with the chromophore-bearing N-terminal domain of oat phytochrome A apoprotein (amino acid residues 1-595). Except for Trp366, which was replaced by Phe (W366F), all the residues exchanged are in close proximity to the chromophore-binding Cys321 (i.e. P318A, P318K, H319L, S320K, H322L and the double mutant L323R/Q324D). The mutants were characterized by their absorption maxima, and the kinetics of chromophore-binding and the Pr-->Pfr conversion. The strongest effect of mutation on the chromoprotein assembly, leading to an almost complete loss of the chromophore binding capability, was found for the exchanges of His322 by Leu (H322L) and Pro318 by Lys (P318K), whereas a corresponding alanine mutant (P318A) showed wild-type behavior. The second histidine (H319) is also involved in chromophore fixation, as indicated by a slower assembly rate upon mutation (H319L). For the other mutants, an assembly process very similar to that of the wild-type protein was found. The light-induced Pr-->Pfr conversion kinetics is altered in the mutations H319L and S320K and in the double mutant L323R/Q324D, all of which exhibited a significantly faster I700 decay and accelerated Pfr formation. P318 is also involved in the Pr-->Pfr conversion, the millisecond steps (formation of Pfr) being significantly slower for P318A. Lacking sufficient amounts of W366F, assembly kinetics could not be determined in this case, while the fully assembled mutant underwent the Pr-->Pfr conversion with kinetics similar to wild-type protein.

Time-resolved absorption and photothermal measurements with sensory rhodopsin I from Halobacterium salinarum

An expansion accompanying the formation of the first intermediate in the photocycle of transducer-free sensory rhodopsin I (SRI) was determined by means of time-resolved laser-induced optoacoustic spectroscopy. For the native protein (SRI-WT), the absolute value of the expansion is approximately 5.5 mL and for the mutant SRI-D76N, approximately 1.5 mL per mol of phototransformed species (in 0.5 M NaCl), calculated by using the formation quantum yield for the first intermediate (S610) of Phi610 = 0.4 +/- 0.05 for SRI-WT and 0.5 +/- 0.05 for SRI-D76N, measured by laser-induced optoacoustic spectroscopy and by laser flash photolysis. The similarity in Phi610 and in the determined value of the energy level of S610, E610 = (142 +/- 12) kJ/mol for SRI-WT and SRI-D76N indicates that Asp76 is not directly involved in the first step of the phototransformation. The increase with pH of the magnitude of the structural volume change for the formation of S610 in SRI-WT and in SRI-D76N upon excitation with 580 nm indicates also that amino acids other than Asp76, and other than those related to the Schiff base, are involved in the process. The difference in structural volume changes as well as differences in the activation parameters for the S610 decay should be attributed to differences in the rigidity of the cavity surrounding the chromophore. Except for the decay of the first intermediate, which is faster than in the SRI-transducer complex, the rate constants of the photocycle for transducer-free SRI in detergent suspension are strongly retarded with respect to wild-type membranes (this comparison should be done with great care because the preparation of both samples is very different).

Structural volume changes upon photoisomerization of the bilirubin-albumin complex: a laser-induced optoacoustic study

The Z-->E photoisomerization of the 1:1 complexes of human serum albumin (HSA) and several bilirubins (BR-IX alpha, -III alpha, meso-IX alpha and a mixture of -IX alpha, -III alpha and XIII alpha) affords in every case an almost negligible structural volume change (delta VR approximately 0) within detection limits (i.e. less than 2-4 cm3/mol for this isomerization with very low quantum yield) as determined by laser-induced optoacoustic spectroscopy. Based on previous model studies of photoisomerizations in aqueous environment, this negligible small change is interpreted as indicating that the part of the molecule undergoing photoisomerization is not exposed to water but is located in a hydrophobic protein cavity that shields the molecule from the aqueous medium. The BR-protein interaction within this cavity seems to be very loose in view of the small structural volume change observed. The energy difference between the Z and E isomers of the BR-HSA complexes was estimated to be less than 4 kJ/mol, probably close to zero (delta H approximately 0).

Chromophore incorporation, Pr to Pfr kinetics, and Pfr thermal reversion of recombinant N-terminal fragments of phytochrome A and B chromoproteins

N-Terminal apoprotein fragments of oat phytochrome A (phyA) of 65 kDa (amino acids 1-595) and potato phyB of 66 kDa (1-596) were heterologously expressed in Escherichia coli and in the yeasts Saccharomyces cerevisiae and Pichia pastoris, and assembled with phytochromobilin (PthetaB; native chromophore) and phycocyanobilin (PCB). The phyA65 apoprotein from yeast showed a monoexponential assembly kinetics after an initial steep rise, whereas the corresponding apoprotein from E. coli showed only a slow monoexponential assembly. The phyB66 apoprotein incorporated either chromophore more slowly than the phyA65s, with biexponential kinetics. With all apoproteins, PthetaB was incorporated faster than PCB. The thermal stabilities of the Pfr forms of the N-terminal halves are similar to those known for the full-length recombinant phytochromes: oat phyA65 Pfr is highly stable, whereas potato phyB66 Pfr is rapidly converted into Pr. Thus, neither the C-terminal domain nor homodimer formation regulates this property. Rather, it is a characteristic of the phytochrome indicating its origin from mono- or dicots. The Pr to Pfr kinetics of the N-terminal phyA65 and phyB66 are different. The primary photoproduct I700 of phyA65-PCB decayed monoexponentially and the PthetaB analogue biexponentially, whereas the phyB66 I700 decayed monoexponentially irrespective of the chromophore incorporated. The formation of Pfr from Pr is faster with the N-terminal halves than with the full-length phytochromes, indicating an involvement of the C-terminal domain in the relatively slow protein conformational changes.

Raman spectroscopic and light-induced kinetic characterization of a recombinant phytochrome of the cyanobacterium Synechocystis

A phytochrome-encoding cDNA from the cyanobacterium Synechocystis has been heterologously expressed in Escherichia coli and reconstituted into functional chromoproteins by incubation with either phycocyanobilin (PCB) or phytochromobilin (PPhiB). These materials were studied by Raman spectroscopy and nanosecond flash photolysis. The Raman spectra suggest far-reaching similarities in chromophore configuration and conformation between the Pfr forms of Synechocystis phytochrome and the plant phytochromes (e.g. phyA from oat), but some differences, such as torsions around methine bridges and in hydrogen bonding interactions, in the Pr state. Synechocystis phytochrome (PCB) undergoes a multistep photoconversion reminiscent of the phyA Pr --> Pfr transformation but with different kinetics. The first process resolved is the decay of an intermediate with red-shifted absorption (relative to parent state) and a 25-micros lifetime. The next observable intermediate grows in with 300 (+/-25) micros and decays with 6-8 ms. The final state (Pfr) is formed biexponentially (450 ms, 1 s). When reconstituted with PPhiB, the first decay of this Synechocystis phytochrome is biexponential (5 and 25 micros). The growth of the second intermediate is slower (750 micros) than that in the PCB adduct whereas the decays of both species are similar. The formation of the Pfr form required fitting with three components (350 ms, 2.5 s, and 11 s). H/D Exchange in Synechocystis phytochrome (PCB) delays, by an isotope effect of 2.7, both growth (300 micros) and decay rates (6-8 ms) of the second intermediate. This effect is larger than values determined for phyA (ca. 1.2) and is characteristic of a rate-limiting proton transfer. The formation of the Pfr state of the PCB adduct of Synechocystis phytochrome shows a deuterium effect similar as phyA (ca. 1.2). Activation energies of the second intermediate in the range 0-18 degrees C are 44 (in H2O/buffer) and 48 kJ mol-1 (D2O), with essentially identical pre-exponential factors.

Effect of chromophore exchange on the resonance Raman spectra of recombinant phytochromes

The recombinant 65-kDa polypeptide of phyA oat phytochrome was expressed by yeast Pichia pastoris and assembled into two chromopeptides with the chromophores phytochromobilin (PphiB) and phycocyanobilin (PCB), respectively. The Pr and Pfr states of the two protein variants were characterized by resonance Raman (RR) spectroscopy and compared with native phyA oat phytochrome demonstrating that the deletion of the C-terminal half of phyA does not alter the structure of the chromophore site within the N-terminal half. Most of the RR spectral changes observed upon replacing PphiB by PCB can be attributed exclusively to altered vibrational mode compositions due to the different ring D substitutions (vinyl vs. ethyl), implying that the chromophore structures are largely the same for PphiB- and PCB-assembled phytochromes. Only in the Pr state may the RR spectral changes also reflect subtle differences of the PphiB and PCB conformations in the 65-kDa phyA, presumably brought about by the specific steric requirements of the vinyl and ethyl groups.

Raman spectroscopic analysis of isomers of biliverdin dimethyl ester

The constitutional isomers of biliverdin dimethyl ester, IX alpha and XIII alpha, were studied by resonance Raman spectroscopy. The far-reaching spectral similarities suggest that despite the different substitution patterns, the compositions of the normal modes are closely related. This conclusion does not hold only for the parent state (ZZZ, sss configuration) but also for the configurational isomers which were obtained upon double-bond photoisomerization. Based on a comparison of the resonance Raman spectra, a EZZ configuration is proposed for one of the two photoisomers of biliverdin dimethyl ester IX alpha, while a ZZE, ssa configuration has been assigned previously to the second isomer.

Volume and enthalpy changes after photoexcitation of bovine rhodopsin: laser-induced optoacoustic studies

Laser-induced optoacoustic measurements were performed with bovine rhodopsin in the temperature range 5-32 degrees C in its natural environment (i.e., in washed membranes) as well as solubilized in dodecyl-beta-D-maltoside. A signal deconvolution procedure using a simple sequential kinetic scheme for the photobaric time evolution revealed, in the case of the washed membranes, the presence of an intermediate with a 14-ns lifetime at 25 degrees C, of the same order as that reported for the BSI intermediate in solubilized rhodopsin (Hug, S. J., W. J. Lewis, C. M. Einterz, T. E. Thorgeirsson, and D. S. Kliger. 1990. Nanosecond photolysis of rhodopsin: evidence for a new, blue-shifted intermediate. Biochemistry. 29:1475-1485), with an energy content of (85 +/- 20) kJ/mol, and accompanied by an expansion of 26 +/- 3 ml/mol. The difference in energy content between BSI and the next transient lumi was estimated in only -1 +/- 5 kJ/mol, concomitant with an expansion of 9 +/- 3 ml/mol. Thus, this transition, which according to literature involves an equilibrium, should be controlled by an entropic change, rather than by an enthalpic difference. This is supported by the fact that both activation parameters for the decay of batho and BSI decrease upon solubilization. For detergent-solubilized rhodopsin, two time constants were enough to fit the sample signal. A short lifetime ascribable to BSI was not detected in this case. For the first intermediate (probably batho in equilibrium with BSI), an energy content of 50 +/- 20 kJ/mol and an expansion of 20 +/- 1 ml/mol, and for lumi an energy content of 11 +/- 20 kJ/mol and a further expansion of 11 +/- 2 ml/mol were determined. Thus, the intermediates of the membrane-embedded form of rhodopsin (in contrast to solubilized samples) are kept in a higher energy level, although the total expansion from rhodopsin to lumi is similar for both conditions (35 +/- 6 and 31 +/- 3 ml/mol). The expansions are interpreted as protein reorganization processes as a consequence of the photoisomerization of the chromophore. As a result, weak interactions are probably perturbed and the protein gains conformational flexibility.

Recombinant type A and B phytochromes from potato. Transient absorption spectroscopy

The cDNAs encoding full-length type A and B phytochromes (phyA and phyB, respectively) from potato were expressed in inducible yeast systems (Saccharomyces cerevisiae and Pichia pastoris). In addition, a deletion mutant of phyB (delta 1-74) was expressed. The apoproteins were reconstituted into chromoproteins by incorporation of the native chromophore, phytochromobilin (P phi B), and of phycocyanobilin (PCB). The incorporation of P phi B yielded chromoproteins with difference absorptions lambda max at 660 and 712 nm (Pr and Pfr, respectively) for phyA, and at 665 and 723 nm for phyB. All difference maxima of PCB phytochromes are blue-shifted by several nanometers with respect to those obtained with the P phi B chromophore. The deletion construct with PCB shows difference absorption maxima at 652 and 705 nm with the Pfr absorbance considerably reduced. Time-resolved kinetic analysis of a phyB-type phytochrome by nanosecond flash photolysis was performed for the first time. Recombinant full-length phyB afforded transient absorbance changes similar (but not identical) to those of phyA from Avena, whereas the kinetic behavior of these intermediates was very different. Contrary to phyA from Avena, the I700 intermediate from phyB reconstituted with either PCB or P phi B decayed following single exponential kinetics with a lifetime of 87 or 84 microseconds, respectively, at 10 degrees C. The formation of Pfr of PCB-containing recombinant phyB (phyB-PCB) could be fitted with three lifetimes of 9, 127, and 728 ms. The corresponding lifetimes of phyB-P phi B are 22.5, 343, and 2083 ms. Whereas for phyB-PCB all three millisecond lifetimes are related to the formation of Pfr, the 2 s component of phyB-P phi B is concomitant with a rapid recovery of Pr. For recombinant potato phyA and delta 1-74 phyB, no time-resolved data could be obtained due to the limited quantities available. As described for phytochromes of other dicotelydons, the Pfr forms of full-length phyA and PhyB of potato underwent rapid dark conversion to Pr.

Chromophore-protein interaction controls the complexity of the phytochrome photocycle

A new protocol for the preparation of recombinant phytochromes results in significantly higher yields which, for the first time, have made kinetic studies possible. Flash photolysis with nanosecond laser excitation reveals that, in recombinant and native phytochromes, the decay kinetics of the primary photoproducts I700i and the kinetics of the formation of the Pfr form are similar. Phycocyanobilin-containing recombinant phytochrome, however, shows only a monoexponential decay of the I700 intermediate with a time constant of approximately 90 microseconds, and a biexponential formation of the Pfr form, albeit with time constants (approximately 13 and 100 ms) somewhat shorter than those from native phytochrome. Thus the seemingly small structural modification of the chromophore (substitution of the native vinyl for an ethyl group) has a profound influence on the availability of protein conformational rearrangement pathways. The result is therefore of general interest in chromoprotein dynamics.

Influence of expression system on chromophore binding and preservation of spectral properties in recombinant phytochrome A

N-Terminal deletion mutants of the plant photoreceptor phytochrome, additionally truncated at two different positions at their C-terminal ends, were expressed both in Escherichia coli and in yeast (Pichia pastoris) and converted into chromoproteins upon chromophore incorporation. The start and end positions of the cDNA employed (phyA from oat) mimic the positions of tryptic cleavage (deletion of the first 64 amino acids, and stop codons after amino acid positions 425 or 595, generating 39-kDa and 59-kDa peptides, respectively. The absorption properties and photochromicity upon red/far-red irradiation of these mutants were compared with their tryptic counterparts derived from native oat phytochrome and with recombinant products possessing intact N-termini, but C-terminal positions identical to those of the corresponding tryptic fragments (45-kDa and 65-kDa peptides). All recombinant 65-kDa and 59kDa peptides bound the chromophore after expression and showed the appropriate absorption spectra of the Pr and the Pfr forms. The smaller chromopeptides (45-kDa and 39-kDa) behaved differently depending on the expression system employed. E. coli-derived peptides exhibited a phytochrome-like difference spectrum only when the intact N-terminus was present (45-kDa product). The recombinant 39-kDa peptide from E. coli was incapable of chromophore binding whereas the identical peptide sequence expressed by P. pastoris formed a chromoprotein with phycocyanobilin. This recombinant phytochrome fragment exhibited a difference spectrum (Pr-Pfr) with an even larger Pfr absorption band than the comparable tryptic 39-kDa fragment. Selectivity of chromophore incorporation and spectral properties suggest that interactions between protein domains of phytochrome control the protein folding and the Pr/Pfr absorption characteristics. Evidently, trypsin digestion down to the 39-kDa fragment affects protein conformation also in terms of Pfr conservation.

Fourier-transform resonance Raman spectroscopy of intermediates of the phytochrome photocycle

The parent states of the 124-kDa phytochrome (phy A from Avena sativa) and intermediates of its photocycle were studied by low-temperature Fourier-transform resonance Raman spectroscopy. Spectra of the primary photoproducts I700 and lumi-F and of the thermal intermediate meta-F have been obtained for the first time. The spectra of the stable photochromic forms of photochrome, Pr and Pfr, presented in this work are significantly better in signal-to-noise ratio and resolution than previously published spectra, demonstrating the distinct advantages of our experimental approach. The high spectral quality allows for the identification of subtle details of the vibrational band pattern so that the resonance Raman spectra, which have been measured from samples in H2O and D2O, constitute a solid basis for the structural analysis of the various forms of phytochrome. Notwithstanding the current uncertainty in the vibrational assignment of many resonance Raman bands, the spectral changes of the tetrapyrrole chromophore can plausibly be interpreted in terms of conformational changes at two different methine bridges, i.e., torsions around two single bonds and the E/Z isomerization of a double bond. Within the framework of this interpretation, which is based on a vibrational analysis of biliverdin dimethyl ester (Smith, K. Matysik, J., Hlldebrandt, P., & Mark, F. (1993) J. Phys. Chem. 97, 11887-11900), a consistent model is proposed to describe the molecular events in the chromophore during the photocycle. The involvement of a proton transfer in the primary photoprocess of Pr can safely be ruled out. However, previous conclusions concerning the chromophore protonation in the individual states appear premature at the present state of the vibrational assignment. In particular, the attribution of a broad band at 1100 cm-1 to the N-H out-of-plane bending of the protonated pyrrolenin nitrogen (Hildebrandt, P., Hoffmann, A., Lindemann, P., Heibel, G., Braslavsky, S. E., Schaffner, K., & Schrader, B. (1992) Biochemistry 32, 7957-7962) has now been found to be erroneous.

Photoinduced volume change and energy storage associated with the early transformations of the photoactive yellow protein from Ectothiorhodospira halophila

The photocycle of the photoactive yellow protein (PYP) isolated from Ectothiorhodospira halophila was analyzed by flash photolysis with absorption detection at low excitation photon densities and by temperature-dependent laser-induced optoacoustic spectroscopy (LIOAS). The quantum yield for the bleaching recovery of PYP, assumed to be identical to that for the phototransformation of PYP (pG), to the red-shifted intermediate, pR, was phi R = 0.35 +/- 0.05, much lower than the value of 0.64 reported in the literature. With this value and the LIOAS data, an energy content for pR of 120 kJ/mol was obtained, approximately 50% lower than for excited pG. Concomitant with the photochemical process, a volume contraction of 14 ml/photoconverted mol was observed, comparable with the contraction (11 ml/mol) determined for the bacteriorhodopsin monomer. The contraction in both cases is interpreted to arise from a protein reorganization around a phototransformed chromophore with a dipole moment different from that of the initial state. The deviations from linearity of the LIOAS data at photon densities > 0.3 photons per molecule are explained by absorption by pG and pR during the laser pulse duration (i.e., a four-level system, pG, pR, and their respective excited states). The data can be fitted either by a simple saturation process or by a photochromic equilibrium between pG and pR, similar to that established between the parent chromoprotein and the first intermediate(s) in other biological photoreceptors. This nonlinearity has important consequences for the interpretation of the data obtained from in vitro studies with powerful lasers.

Expression of phytochrome apoprotein from Avena sativa in Escherichia coli and formation of photoactive chromoproteins by assembly with phycocyanobilin

Phytochrome DNAs from oat (Avena sativa L.) encoding the full-length 124-kDa polypeptide, a 118-kDa fragment lacking the first 65 amino acids, and two N-terminal fragments of 65 kDa and 45 kDa were subcloned and expressed in Escherichia coli. Reducing the temperature to 25 degrees C during cell growth and the coexpression of chaperones improved the folding into a functional conformation for most of the polypeptides, and in one case the yield of polypeptides was also enhanced. A maximum yield of reconstitutable apoprotein was obtained by expressing the 65-kDa fragment consisting of 595 amino acids. The apoproteins could be assembled in the dark with phycocyanobilin into photoreversible chromoproteins. The yield of photoreversible pigment could be further increased by far-red/red irradiation cycles, indicating that the presence of the chromophore promotes the correct folding of the binding site. The chromoproteins with an intact N-terminal domain exhibit Pr and Pfr absorption bands, which are blue-shifted relative to the corresponding bands of native phytochrome due to the particular phycocyanobilin structure. The 118-kDa fragment, only lacking the 6-kDa N-terminus, exhibits a strong Pr band, but only a weak Pfr absorbance. This indicates an essential role of the front 6-kDa region of the protein in the formation of the far-red absorbing chromophore-protein complex. Otherwise, the C-terminal region seems to be less important for photoreversibility as indicated by the function of the shorter fragments.

Photoinduced volume changes associated with the early transformations of bacteriorhodopsin: a laser-induced optoacoustic spectroscopy study

Volume changes associated with the primary photochemistry of bacteriorhodopsin (BR) were measured by temperature-dependent laser-induced optoacoustic spectroscopy (LIOAS). Excitation was performed with 8-ns flashes establishing a photoequilibrium between the BR and the K states (BR<-->hvK). The concentration of K at the end of the laser pulse, which is an important parameter for the calculation of the volume change per molecule from the LIOAS data, was determined by flash photolysis with optical detection under the specific conditions (concentration, photon density) of the LIOAS experiment. Temperature-dependent measurements yielded a linear dependency of the ratio of the optoacoustic signals for BR and for a calorimetric reference (CoCl2) with the cubic thermal expansion coefficient beta of water. From the slope of this linear ratio a contraction of 11 cm3/mol was determined.

Effects of bound monoclonal antibodies on the decay of the phototransformation intermediates I700(1,2) from native Avena phytochrome

The kinetics of the microsecond phototransformation intermediates of 124 kDa Avena phytochrome (I700(1,2) were studied in the presence of bound monoclonal antibodies at various temperatures. A global analysis was applied to the decays at all wavelengths at each temperature in order to derive the rate constants and the decay-associated spectra of the three decay components. Monoclonal antibodies bound to specific epitopes altered the Arrhenius parameters of both I700(1,2) decay components. The strongest influence on these parameters was observed with OAT 8 (epitope between residues 624 and 686), which decreased by more than 50% the activation parameters of both components. This decrease is interpreted to result from an increased flexibility induced by this antibody in the ground state or in the transition state of bonds changing during the decay of both I700 transients. Thus, the OAT 8 epitope appears to be functionally important during the decay of the I700(1,2) intermediates. For the case of I700(1), bound OAT 23 and OAT 25 (epitopes between residues 1 and 66) reduced even further the relatively small flexibility of these bonds in the red light-absorbing form of phytochrome (Pr) without antibodies, as reflected by the high preexponential factors for its decay. This resulted also in higher activation energies for this decay in the presence of the antibodies. Thus, the amino-terminus should act as a rigid spacer of the chromophore cavity without affecting it during the microsecond transformation, because the Arrhenius parameters for these decays are similar to those for small phytochrome. The possible implications of the influence of the various antibodies on the bleaching remaining after the decay of I700(1,2) are discussed.

Fourier transform resonance Raman spectroscopy of phytochrome

The Pr and Pfr forms of phytochrome in H2O and D2O have been studied by Fourier transform resonance Raman spectroscopy with near-infrared excitation (1064 nm). It is demonstrated that this technique is a powerful method for analyzing the chromophore structures of photosensitive pigments. The high spectral quality allows discussion of vibrational assignments based on an empirical approach using previously published data obtained from model compounds. The reduction in intensity of a high-frequency band assigned to the ring-C/D methine bridge vibration is an indication for the non-coplanarity of the ring D in Pfr. The high intensity of a C-H out-of-plane vibration also supports this hypothesis. In Pr, a broad peak at approximately 1100 cm-1 is assigned to an out-of-plane vibration of a strongly hydrogen-bonded pyrrole C=NH+ group. It is missing in Pfr, suggesting deprotonation of the corresponding ring during the transformation from Pr to Pfr.

Carboxylated zinc-phthalocyanines--II. Dimerization and singlet molecular oxygen sensitization in hexadecyltrimethylammonium bromide micelles

The dimerization of the diamide of zinc-tetracarboxyphthalocyanine was studied spectroscopically in hexadecyltrimethylammonium bromide (CTAB) micelles at surfactant concentrations from 0.026 to 0.1 M and dye concentrations between 0.1 and 10 microM. The apparent dimerization constant in CTAB 0.1 M is 8.6 x 10(5) M-1, while the intramicellar dimerization constant is 1.8 x 10(3). The dimer absorption spectrum was also obtained. Singlet molecular oxygen sensitization was studied by steady state photolysis using 1,3-diphenylisobenzofurane as scavenger in 0.1 M CTAB. The usual sensitization mechanism is extended to include dimer reactions. Singlet molecular oxygen sensitization yields for monomer and dimer in the micelles are 0.7 and 0.1, respectively. With the reported values it is possible to calculate the average yield of singlet molecular oxygen production at any surfactant and dye concentrations.

Quantum yields of triplet and O2(1 delta g) formation of 4-thiouridine in water and acetonitrile

The quantum yield of triplet formation, phi T, and that of the photosensitized formation of singlet molecular oxygen, phi delta, were determined for a rare nucleoside, 4-thiouridine (4t-Urd), in water and in acetonitrile, using singlet molecular oxygen phosphorescence, laser-induced optoacoustics and time-resolved thermal lensing. These yields, phi T and phi delta, the latter in aerated solutions, were found to be, respectively, in water: 0.67 +/- 0.17 and 0.18 +/- 0.04 and in acetonitrile: 0.61 +/- 0.15 and 0.50 +/- 0.20. The fraction of the 4t-Urd triplet molecules quenched by oxygen leading to singlet molecular oxygen, S delta, was calculated to be between 0.7 and unity in both solvents, this value being indicative of a pi pi*character for the lowest triplet state of 4t-Urd.

Quantum yield of production of singlet molecular oxygen (1 delta g) in aqueous dispersions of small unilamellar lipid vesicles. A time-resolved near-IR phosphorescence study

The quantum yield of formation and kinetic behaviour of O2(1 delta g) in D2O dispersions of small unilamellar vesicles (SUVs) of dipalmitoyl phosphatidylcholine were studied by time-resolved detection of near-IR phosphorescence. At a SUV concentration of 26 nM, O2(1 delta g) is not quenched by the vesicles. It diffuses quickly through the lipid bilayer and a partition equilibrium of O2(1 delta g) between the lipid bilayer and the buffer is attained before decay occurs. In this equilibrium situation O2(1 delta g) is mostly located in the buffer phase, which permits the determination of absolute quantum yields for O2(1 delta g) production, phi delta, by comparison of the luminescence in the dispersions with that in neat D2O. The maximal phi delta values for the sensitizers incorporated in the SUV bilayer were 0.47 +/- 0.09 for the dipyridyl complex of zinc(II) phthalocyanine (ZnPc), 0.35 +/- 0.08 for porphycene, and 0.36 +/- 0.08 for 2,7,12,17-tetra-n-propylporphycene. These values are equal to those in neat organic solvents but lower than those previously obtained in SUVs by using chemical trapping agents. The high degree of organization of the environment around the sensitizers does not influence their efficiency of producing O2(1 delta g). While no concentration dependence is observed for ZnPc (at least up to a local concentration of 20 mM in the bilayer), phi delta for both porphycenes significantly decreases above a local concentration of 4 mM in the bilayer. This result is expected in view of previous observations on the concentration dependence of other photophysical parameters of the porphycenes in such microheterogeneous media.

Partial purification and initial characterization of phytochrome from the mossAtrichum undulatum P. Beauv. grown in the light

The extraction and partial purification of phytochrome from light-grownAtrichum undulatum P. Beauv., a chlorophyllous moss, is described. Polyethyleneimine and salt fractionation followed by hydroxyapatite and Affi-gel-blue chromatography were used to separate phytochrome from chlorophyll, and to purify the pigment. All steps were performed in the presence of Triton X-100 which improved the yield by a factor of about three. The protein has a molecular weight some-what larger than that ofAvena phytochrome (124 kDa), as determined by sodium dodecyl sulfate-polyacrylamide gel electrophoresis and immunoblot analysis. It cross-reacts with a monoclonal antibody against phytochrome from etiolated corn (Zea) and a polyclonal antibody against phytochrome from etiolated oat (Avena), and its photoreversibility is similar to that of phytochrome from greenAvena.