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

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

Femtosecond kinetics of photoconversion of the higher plant photoreceptor phytochrome carrying native and modified chromophores

The photoprocesses of native (phyA of oat), and of C-terminally truncated recombinant phytochromes, assembled instead of the native phytochromobilin with phycocyanobilin (PCB-65 kDa-phy) and iso-phycocyanobilin (iso-PCB-65 kDa-phy) chromophores, have been studied by femtosecond transient absorption spectroscopy in both their red absorbing phytochrome (P_r) and far-red absorbing phytochrome (P_fr) forms. Native P_r phytochrome shows an excitation wavelength dependence of the kinetics with three main picosecond components. The formation kinetics of the first ground-state intermediate I₇₀₀, absorbing at ∼690 nm, is mainly described by 28 ps or 40 ps components in native and PCB phytochrome, respectively, whereas additional ∼15 and 50 ps components describe conformational dynamics and equilibria among different local minima on the excited-state hypersurface. No significant amount of I₇₀₀ formation can be observed on our timescale for iso-PCB phytochrome. We suggest that iso-PCB-65 kDa-phy either interacts with the protein differently leading to a more twisted and/or less protonated configuration, or undergoes P_r to P_fr isomerization primarily via a different configurational pathway, largely circumventing I₇₀₀ as an intermediate. The isomerization process is accompanied by strong coherent oscillations due to wavepacket motion on the excited-state surface for both phytochrome forms. The femto- to (sub-)nanosecond kinetics of the P_fr forms is again quite similar for the native and the PCB phytochromes. After an ultrafast excited-state relaxation within ∼150 fs, the chromophores return to the first ground-state intermediate in 400-800 fs followed by two additional ground-state intermediates which are formed with 2-3 ps and ∼400 ps lifetimes. We call the first ground-state intermediate in native phytochrome I_fr·750, due to its pronounced absorption at that wavelength. The other intermediates are termed I_fr·675 and pseudo-P_r. The absorption spectrum of the latter already closely resembles the absorption of the P_r chromophore. PCB-65 kDa-phy shows a very similar kinetics, although many of the detailed spectral features in the transients seen in native phy are blurred, presumably due to wider inhomogeneous distribution of the chromophore conformation. Iso-PCB-65 kDa-phy shows similar features to the PCB-65 kDa-phy, with some additional blue-shift of the transient spectra of ∼10 nm. The sub-200 fs component is, however, absent, and the picosecond lifetimes are somewhat longer than in 124 kDa phytochrome or in PCB-65 kDa-phy. We interpret the data within the framework of two- and three-dimensional potential energy surface diagrams for the photoisomerization processes and the ground-state intermediates involved in the two photoconversions.     

Subpicosecond midinfrared spectroscopy of the Pfr reaction of phytochrome Agp1 from Agrobacterium tumefaciens

Phytochromes are light-sensing pigments found in plants and bacteria. For the first time, the P_fr photoreaction of a phytochrome has been subject to ultrafast infrared vibrational spectroscopy. Three time constants of 0.3 ps, 1.3 ps, and 4.0 ps were derived from the kinetics of structurally specific marker bands of the biliverdin chromophore of Agp1-BV from Agrobacterium tumefaciens after excitation at 765 nm. VIS-pump-VIS-probe experiments yield time constants of 0.44 ps and 3.3 ps for the underlying electronic-state dynamics. A reaction scheme is proposed including two kinetic steps on the S₁ excited-state surface and the cooling of a vibrationally hot P_fr ground state. It is concluded that the upper limit of the E-Z isomerization of the C₁₅ = C₁₆ methine bridge is given by the intermediate time constant of 1.3 ps. The reaction scheme is reminiscent of that of the corresponding P_r reaction of Agp1-BV as published earlier.     

Immunochemical and spectroscopic evidence for protein conformational changes in phytochrome transformations

Phytochrome was examined by immunochemical and spectroscopic techniques to detect differences between the protein moieties of red- and far red-absorbing phytochrome (P_r and P_fr). No differences in the reaction of P_r and P_fr with phytochrome antibody were discernible on Ouchterlony double diffusion plates. However, the microcomplement fixation assay showed a greater degree of antibody reaction with P_fr than with P_r, indicating some difference in the surface characteristics of the two forms. Circular dichroism spectroscopy between 300 and 200 nanometers revealed differences between P_r and P_fr which may reflect differences in the protein conformation. The circular dichroism spectrum of P_r showed a negative band at 285 nanometers which was not present in the spectrum of P_fr, and the large negative circular dichroism band at 222 nanometers with P_fr, associated with the α-helical content, was shifted 2 nanometers to shorter wave length with P_r although there was no change of magnitude of this band. The absorbancy of P_r and P_fr is very nearly the same in the 280 nanometer spectral region, but sensitive difference spectra between P_r and P_fr did reveal spectra which were similar to solvent perturbation spectra obtained by others with different proteins. In total, the experiments indicate that there are conformational differences between the protein moieties of P_r and P_fr but that these differences are rather slight from a standpoint of gross structure.     

Fluence-response curves and action spectra for the very low fluence and the low fluence response for the induction of kalanchoë seed germination

Germination of Kalanchoë blossfeldiana Poelln. seeds is absolutely light-requiring. Germination of one seed is the result of one out of three reactions, viz. the very low fluence response (VLFR), the low fluence response (LFR) and the high fluence response/high irradiance response. In order to demonstrate the involvement of phytochrome for both photoresponses, i.e. VLFR and LFR, action spectra for induction were determined. Fluence-response data are analyzed by means of probit analysis in order to calculate the seed population parameters, with special attention to μ, or the fluence for half-maximal induction, and B, the slope in the probit diagram. Laser light was used between 620 and 800 nanometers to analyze the VLFR. Phytochrome is responsible for both photoresponses: the VLFR action spectrum demonstrates an exponential decrease in apparent photoconversion cross-section (P_r → P_fr) up to about 800 nanometers. Assuming that P_r:P_fr-X and P_fr:P_fr-X are the effectors for the VLFR and the LFR, respectively, we estimate an average induction threshold of about 0.003% P_r:P_fr for the VLFR and about 1% P_fr:P_fr for the LFR among individuals of the seed population.     

Photoreversible association of phytochrome with membranes. II. Reciprocity tests and a model for the binding reaction

Abstract A series of fluence-response curves for the binding of phytochrome to membranes in the absence of divalent cations, as described by Watson & Smith (1982), were constructed to demonstrate that the response obeys the law of reciprocity. Analysis of the binding of P_fr (the far-red-absorbing form of phytochrome) showed that two P_fr molecules bind to the membrane for each P_r (the form with an absorption maximum in the red) photoconverted to P_fr in the intrinsic membrane-bound phytochrome pool. Using this stoichiometry we have been able to model the binding curve of Pr and match the binding data. P_r binding can be simulated if P_r binds only as a consequence of the binding of P_fr, i.e. when P_fr is part of a P_r: P_fr dimer. The enrichment of the membranes with P_fr as a result of the binding of P_fr was also accurately simulated. There is no binding cooperativity. Phytochrome binding is a low-fluence response and the possibility that it has physiological significance as a mediator of phytochrome action is discussed.     

Subpicosecond resonance Raman spectra of the early intermediates in the photocycle of bacteriorhodopsin

The resonance Raman spectra are presented for the species formed during the photocycle of bacteriorhodopsin (bR) on a timescale of 800-900 fs. In the ethylenic stretch region two intermediates were found with frequencies of 1,510 and 1,518 cm^-1, corresponding to species with optical absorption maxima at 660 and 625 nm, respectively. This leads to the assignment of the 1,518 cm^-1 band to the J₆₂₅ intermediate. In the fingerprint region, the appearance of a vibration at 1,195 cm^-1 strongly suggests that the isomerization indeed has taken place in a time less than the pulsewidth of our laser. This supports the previous proposals made on the basis of the optical spectra. The spectra are compared with those observed in tens of picoseconds up to nanoseconds.     

Phytochrome behaves as a dimer in vivo

Abstract It is well established that phytochrome exists as a dimer in vitro. A comparison of the relative photoequilibrium concentrations of P_rP_r, P_rP_fr and P_frP_fr, with the relative sizes of the P_fr-pools which undergo dark reversion in the intact plant, leads to the hypothesis that phytochrome also exists as a dimer in vivo, This hypothesis is in accordance with kinetic properties of the phytochrome system under continuous irradiation. Additional support for this view is provided by the observation that P_fr-destruction after a red light flash, which should favour the formation of P_rP_fr dimers, is paralleled by a decay of P_r, even if the presence of P_r cycled through P_fr can be excluded. Preliminary observations could indicate an interaction of the subunits of a phytochrome dimer during the process of phototransformation.     

First steps of retinal photoisomerization in proteorhodopsin

The early steps (<1 ns) in the photocycle of the detergent solubilized proton pump proteorhodopsin are analyzed by ultrafast spectroscopic techniques. A comparison to the first primary events in reconstituted proteorhodopsin as well as to the well known archaeal proton pump bacteriorhodopsin is given. A dynamic Stokes shift observed in fs-time-resolved fluorescence experiments allows a direct observation of early motions on the excited state potential energy surface. The initial dynamics is dominated by sequentially emerging stretching (<150 fs) and torsional (approximately 300 fs) modes of the retinal. The different protonation states of the primary proton acceptor Asp-97 drastically affect the reaction rate and the overall quantum efficiencies of the isomerization reactions, mainly evidenced for time scales above 1 ps. However, no major influence on the fast time scales (approximately 150 fs) could be seen, indicating that the movement out of the Franck-Condon region is fairly robust to electrostatic changes in the retinal binding pocket. Based on fs-time-resolved absorption and fluorescence spectra, ground and exited state contributions can be disentangled and allow to construct a reaction model that consistently explains pH-dependent effects in solubilized and reconstituted proteorhodopsin.     

The phytochrome system in light-grown Zea mays L.

The phytochrome system is analyzed in light-grown maize (Zea mays L.) plants, which were prevented from greening by application of the herbicide SAN 9789. The dark kinetics of phytochrome are not different in the first, second or third leaf. It is concluded that in light-grown maize plants phytochrome levels are regulated by P_r formation and P_fr and P_r destruction, rather than by P_frP_r dark reversion. P_r undergoes destruction after it has been cycled through P_fr. The consequences of this P_r destruction on the phytochrome system are discussed.Abbreviations SAN 9789 4-chloro-5-(methylamino)-2-(,,-trifluoro-m-tolyl)-3(2H) pyridazinone - P_fr far-red absorbing form of phytochrome - P_r red absorbing form of phytochrome - P_tot P_fr+P_r     

Photoperiodism and rhythmic response to light

Abstract. Seedlings of Pharhitis nil show a circadian rhythm in the capacity to flower in response to the timing of a second red light pulse given at various times after a first saturating exposure to red when this is given together with a benzyladeninc spray. There are also changes in the photon irradiance required for half maximum response to the second red pulse. The photochemical properties of phytochrome in the photoperiodically sensitive cotyledons were also shown to change rhythmically. Oscillations in both p_r→ P_fr and P_fr→ P_r photoconversion characteristics persisted over at least two circadian cycles with a periodicity of about 12 h. There were, however, no significant oscillations in either P_fr peak absorbance or in Δ(ΔA). The changes in sensitivity for the photoconversion of P_r→ P_fr did not parallel the much larger changes in sensitivity of the flowering response to red light. The amplitude of the P_r→ P_fr rhythm was at least as great as that for P_r→ P_fr, but the flowering response to far-red light was not rhythmic, nor was there any large change in sensitivity. The changes in photoconversion properties may reflect a basic biochemical oscillation which affects both photoreceptor properties and sensitivity to photoreceptor input. There was also a marked rhythm in the P_fr/P ratio that would be established by a saturating pulse of red light and this too may have affected the flowering response to such a pulse. Far-red light inhibited flowering when given at any time during the inductive night. After 14 h in darkness, P_fr could still be measured in the cotyledons and it was concluded that far-red light inhibited flowering by removing P_fr As red light also inhibited flowering at this time, there may be two pools of phytochrome with different kinetic properties.     

Phototransformation of the Red Light Sensor Cyanobacterial Phytochrome 2 from Synechocystis Species Depends on Its Tongue Motifs

Phytochromes are photoreceptors using a bilin tetrapyrrole as chromophore, which switch in canonical phytochromes between red (P_r) and far red (P_fr) light-absorbing states. Cph2 from Synechocystis sp., a noncanonical phytochrome, harbors besides a cyanobacteriochrome domain a second photosensory module, a P_r/P_fr-interconverting GAF-GAF bidomain (SynCph2(1-2)). As in the canonical phytochromes, a unique motif of the second GAF domain, the tongue region, seals the bilin-binding site in the GAF1 domain from solvent access. Time-resolved spectroscopy of the SynCph2(1-2) module shows four intermediates during P_r → P_fr phototransformation and three intermediates during P_fr → P_r back-conversion. A mutation in the tongue''s conserved PRXSF motif, S385A, affects the formation of late intermediate R3 and of a P_fr-like state but not the back-conversion to P_r via a lumi-F-like state. In contrast, a mutation in the likewise conserved WXE motif, W389A, changes the photocycle at intermediate R2 and causes an alternative red light-adapted state. Here, back-conversion to P_r proceeds via intermediates differing from SynCph2(1-2). Replacement of this tryptophan that is ∼15 Å distant from the chromophore by another aromatic amino acid, W389F, restores native P_r → P_fr phototransformation. These results indicate large scale conformational changes within the tongue region of GAF2 during the final processes of phototransformation. We propose that in early intermediates only the chromophore and its nearest surroundings are altered, whereas late changes during R2 formation depend on the distant WXE motifs of the tongue region. Ser-385 within the PRXSF motif affects only late intermediate R3, when refolding of the tongue and docking to the GAF1 domain are almost completed.     

Phytochrome decay in seedlings under continuous incandescent light

Summary Under continuous high intensity incandescent light the decay of phytochrome in Amaranthus seedlings deviates from the predicted first order rate characteristic of the P _fr/P _total ratio maintained. This deviation takes the form of a slower decay than would be predicted and is only observed at high intensities. Experiments are presented to test the hypothesis that this reduced rate of decay is the result of a high level of phytochrome intermediates maintained under high intensity incandescent light. Accumulation of intermediates under these conditions has been demonstrated using a quasi-continuous measuring spectrophotometer. They are weakly absorbing and their concentration increases with light intensity. Although they form P _fr in darkness, it is proposed that they do not decay. The model predicts that in a sample cuvette, where a light intensity gradient exists, there is more probability of a phytochrome molecule being presnet as P _fr at the back of the cuvette: the region of lowest light intensity. Under conditions which favour phytochrome decay, a preferential loss of phytochrome should result at the back of the cuvette and an increasingly higher proportion of the remaining phytochrome will consequently be measured as intermediate as the experiment progresses. The results confirm the hypothesis and in addition, after 60 min incandescent light, demonstrate an accumulation of intermediates which form P _fr with a longer half-life that at the begining of the experiment. Pisum epicotyl hooks show no such intermediate accumulation or preferential decay at the back of the cuvette, which is in agreement with the observed first order phytochrome decay under high intensity incandescent light. A scheme is presented explaining the results on the basis of the decay process.Abbreviations FR far-red light - R red light - P phytochrome - P _fr far-red-absorbing form of P - P _r red-absorbing form of P 321st communication of this Laboratory.     

Photochemical and Nonphotochemical Reactions of Phytochrome in vivo

The nonphotochemical reactions of phytochrome in the coleoptiles of dark-grown corn seedlings were studied at 3 temperatures: 14°, 24°, and 34°. The data obtained show that the destruction of P_fr is the only measurable reaction occurring; reversion of P_fr to P_r was not found. The Q₁₀'s (2.7 and 3.5) and zero order kinetics found for the destruction reaction are consistent with the hypothesis that the reaction is enzyme-mediated.

In vivo action spectra for phytochrome transformation in the coleoptiles of darkgrown corn seedlings were obtained which agree qualitatively with those obtained by other workers for phytochrome-mediated physiological responses and in vitro action spectra. In vivo conversion of phytochrome by blue light, as determined from spectrophotometric measurements of phytochrome itself, is reported. Action peaks for P_r were found at 667 mμ and in the blue in the region of 400 mμ, with a broad shoulder from 590 mμ to 640 mμ. Action peaks for P_fr were found at 725 mμ and in the blue in the region of 400 mμ with a minor peak at 670 mμ, and a broad shoulder from 590 mμ to 640 mμ. The ratio of the quantum efficiencies of P_r at 667 mμ and P_fr at 725 mμ (Φ_r667/Φ_fr725) was estimated to be 1.0.

     

Action spectra for light-induced germination in dormant lettuce seeds

Fluence response curves for red light-induced germination of thermodormant (TD) seeds of Lactuca sativa L. show two regions that differ in their light sensitivity. In the region of high sensitivity, the germination responses differ between seed batches and can be altered by dark storage or far red irradiation. Induction of germination in far red dormant (FRD) seeds requires far higher fluences. Action spectra for induction to 60% germination were determined for these various response types. Spectra for the regions of low sensitivity response are similar for TD and FRD seeds. In comparison, the action spectrum for the highly sensitive response in TD seeds is significantly shifted to longer wavelengths. Analogous differences exist in the action spectra for far red reversal of the red induced germination responses. Germination induction in the low sensitivity region shows repeated red-far red reversibility. Far red reversal of red induction in the high sensitivity region does not saturate even at the highest far red fluences available and requires increased red fluences for subsequent reinduction. A model quantitatively accounting for these observations is presented. It is pointed out that action spectra of processes involving photoreversible pigments with partly overlapping absorption spectra in general are not identical with the absorption spectra of the partners. They should depend upon the degree of phototransformation required to elicit a given physiological response. In the case of induction of lettuce seed germination the observed action spectra can be interpreted as reflecting different requirements for P _fr of the various response types. Our results do not necessitate the assumption of spectroscopically different forms of phytochrome in these seeds.Abbreviations TD thermodormant - FRD far red dormant - P phytochrome - P _r red absorbing form of P - P _fr far red absorbing form of P     

Domain interaction in cyanobacterial phytochromes as a prerequisite for spectral integrity

Two phytochromes, CphA and CphB, from the cyanobacterium Calothrix PCC7601, with similar size (768 and 766 amino acids) and domain structure, were investigated for the essential length of their protein moiety required to maintain the spectral integrity. Both proteins fold into PAS-, GAF-, PHY-, and Histidine-kinase (HK) domains. CphA binds a phycocyanobilin (PCB) chromophore at a “canonical” cysteine within the GAF domain, identically as in plant phytochromes. CphB binds biliverdin IXα at cysteine24, positioned in the N-terminal PAS domain. The C-terminally located HK and PHY domains, present in both proteins, were removed subsequently by introducing stop-codons at the corresponding DNA positions. The spectral properties of the resulting proteins were investigated. The full-length proteins absorb at (CphA) 663 and 707 nm (red-, far red-absorbing P _r and P _fr forms of phytochromes) and at (CphB) 704 and 750 nm. Removal of the HK domains had no effect on the absorbance maxima of the resulting PAS–GAF–PHY constructs (CphA: 663/707 nm, CphB: 704/750 nm, P _r/P _fr, respectively). Further deletion of the “PHY” domains caused a blue-shift of the P _r and P _fr absorption of CphA (λ _max: 658/698 nm) and increased the amount of unproperly folded apoprotein, seen by a reduced capability to bind the chromophore in photoconvertible manner. In CphB, however, it practically impaired the formation of P _fr, i.e., showing a very low oscillator strength absorption band, whereas the P _r form remains unchanged (702 nm). This finding clearly indicates a different interaction between domains in the “typical”, PCB binding and in the biliverdin-binding phytochromes, and demonstrates a loss of oscillator strength for the latter, most probably due to a strong conformational distortion of the chromophore in the CphB P _fr form. Proceedings of the XVIII Congress of the Italian Society of Pure and Applied Biophysics (SIBPA), Palermo, Sicily, September 2006.     

The active form of phytochrome: a new hypothesis based on phytochrome pelletability studies

Difficulties arising from the current dogma that the far-red absorbing form of phytochrome (P_fr) is the only active form are discussed.A new hypothesis is proposed in which phytochrome is held to be the photoreceptor for both low energy (pulse) and high energy (HIR) responses. There is a common basic mechanism of action involving interaction between phytochrome and a binding site within the cell. The phytochrome involvement in low energy responses exhibits an action spectrum for binding that matches the P_r absorption spectrum and reversibility by far-red irradiation. Upon prolonged irradiation the phytochrome-binding site interaction acquires different characteristics that are reminiscent of those displayed in HIR, e.g. dependence on sustained irradiation for continual binding, dependence of the degree of binding on irradiance and the similarity of the action spectrum with that of HIR action spectra, e.g. that for inhibition of lettuce hypocotyl lengthening.As expected on the basis of the new hypothesis the particulate fraction of phytochrome contains both P_r and P_fr. Arguments are advanced that the presence of P_r in pellets of particulate phytochrome cannot be accounted for by (i) the “induced fit” hypothesis, (ii) the “pigment cycling” hypothesis, and (iii) the “open phytochrome-receptor model”. We conclude that phytochrome molecules, after being sufficiently energized can interact with their intracellular binding sites irrespective of their chromophoric configuration.     

Developmental Physiology Apparent Dark Decay of Phytochrome Pfr in Fern Spores

Germination of spores of Dryopteris fllix-mas has been induced by two pulses of saturating red light, separated by a dark period of about 8 to 24 h. By chosing different wavelengths, different P_fr/P_tot levels could be established. Thus, by a “null method” the second pulse could be used as a “test pulse”, determining the actual P_fr level remaining from the “start pulse”, and thus providing information about an apparent Pf_r decay. It cannot be decided yet whether this apparent P_fr decay results from dark destruction or dark reversion. The apparent P_fr decay depends, as expected, on the temperature, being accelerated with increasing temperatures. Moreover, the later after sowing that the decay is tested, the faster it proceeds; a tentative interpretion is that newly synthesized P_r undergoes faster decay after phototransformation than that phytochrome pool present in the resting spores. A third factor that influences the apparent P_fr decay is the Pf_r/P_tot level established by the first pulse (start pulse). The lower this level, the slower the decay kinetics. This could be due to phytochrome biosynthesis partly compensating for P_fr destruction, and the relative contribution of this biosynthesis to the total effect increases with lower P_fr levels. Spores of D. paleacea yield virtually the same results. Whatever the real basis of the observed P_fr decay, i.e. destruction, reversion, or a combination of these reactions with biosynthesis, it can be concluded that modification of this P_fr decay by various factors is the basis of the effect of those factors on light-induced germination.     

Phytochrome in seeds of Amaranthus caudatus

Summary Dry seeds of Amaranthus caudatus show little or no photoreversible absorption changes, attributable to phytochrome. During imbibition phytochrome appears in two phases, one immediately after sowing and the second after about 8 hr. Experiments at different temperatures and under continuous illumination with red, far-red and blue light suggest that there are two pools of phytochrome. The first phase in the appearance of phytochrome could be due to the change in optical properties of the sample on hydration or to rehydration of inactive phytochrome, or both. The second phase probably represents phytochrome synthesis. It is absent at 0° and precedes the water uptake associated with germination by some 10 hr. This second pool of phytochrome does not accumulate in red and blue illuminated seeds indicating that the rate of P _fr decay is more rapid than the rate of phytochrome synthesis. The difference spectra of phytochrome in both 2 hr imbibed seeds and 72 hr old seedlings show peaks of absorption at 663 and 735 nm. The presence of P _fr in dark imbibed seeds and the process of inverse reversion of P _r to P _fr in darkness have been demonstrated. The results are discussed in relation to previous hypotheses for the mechanism of photocontrol of Amaranthus seed germination.     

Red/far-red modulation in vitro of enzyme activity in a membrane fraction from Phaseolus aureus

In a membrane fraction isolated from hypocotyls of Phaseolus aureus Roxb. the activity of a number of enzymes was regulated by red and far-red irradiation in vitro, provided that the tissue received a brief red light treatment before extraction. Other enzymes showed no photoregulation. There were two types of photocontrol, neither of which could be detected in the solute fraction, nor in extracts from completely etiolated material. One (Type I) was a red/far-red reversible regulation of the rate of enzyme activity, depending on the light given (in vivo or in vitro) before the assay was begun. The second (Type II) was a promotion of enzyme activity by red or far-red light given during the assay. The action spectra for type II responses do not coincide with either the phytochrome absorption or difference spectra. However, the effectiveness of red and far-red was correlated with the P_fr/P ratio present at the beginning of the assay, such that far-red was more efficient at high P_fr/P and red at low P_fr/P ratios. All enzymes that were regulated involved ATP. In samples that showed enzyme regulation, small changes in fluorescence yield of tryptophan and the covalent probe Fluram (Roche) accompanied the photoconversion of phytochrome, but no fluorescence changes could be measured after briefly incubating the membrane fraction with ATP. The results indicate that light may affect the interaction of ATP with the membrane fraction.Abbreviations F far-red light - P_r and P_fr phytochrome in the red and far-red absorbing forms - P_tot total phytochrome - R red light - RNP ribonucleoprotein