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This study presents an accurate biexponential weighted stochastic conjugate direction (WSCD) method for the quantitative T2-mapping reconstruction of magnetic resonance images (MRIs), and this approach was compared with the non-negative-least-squares Gauss-Newton (GN) numerical optimization method in terms of accuracy and goodness of fit of the reconstructed images from simulated data and ruptured Achilles tendon (AT) MRIs. Reconstructions with WSCD and GN were obtained from data simulating the signal intensity from biexponential decay and from 58 MR studies of postrupture, surgically repaired ATs. Both methods were assessed in terms of accuracy (closeness of the means of calculated and true simulated T2 values) and goodness of fit (magnitude of mean squared error (MSE)). The lack of significant deviation in correct T2 values for the WSCD method was demonstrated for SNR ≥ 20 and for GN-SNR ≥ 380. The MSEs for WSCD and GN were 287.52 ± 224.11 and 2553.91 ± 1932.31, respectively. The WSCD reconstruction method was better than the GN method in terms of accuracy and goodness of fit.

Recombinant phytochromes Agp1 and Agp2 from Agrobacterium tumefaciens are used as model phytochromes for biochemical and biophysical studies. In biliverdin binding phytochromes the site for covalent attachment of the chromophore lies in the N-terminal region of the protein, different from plant phytochromes. The issue which stereochemistry the chromophore adopts in the so-called Pr and Pfr forms is addressed by using a series of locked chromophores which form spectrally characteristic adducts with Agp1 and Agp2. Studies on light-induced conformational changes of Agp1 give an insight into how the intrinsic histidine kinase is modulated by light. Comparison of the crystal structure of an Agp1 fragment with other phytochrome crystal structures supports the idea that a light induced rearrangement of subunits within the homodimer modulates the activity of the kinase.

Ppr is a unique bacteriophytochrome that bleaches rather than forming a far-red-shifted Pfr state upon red light activation. Ppr is also unusual in that it has a blue light photoreceptor domain, PYP, which is N-terminally fused to the bacteriophytochrome domain (Bph). When both photoreceptors are activated by light, the fast phase of Bph recovery (1 min lifetime) corresponds to the formation of an intramolecular long-lived complex between the activated PYP domain and the Bph domain (lifetime of 2-3 days). Since this state is unusually long-lived as compared to other intermediates in the photocycle of both PYP and Bph, we interpret this as formation of a metastable complex between activated PYP and Bph domains that takes days to relax. In the metastable complex, the PYP domain is locked in its activated UV absorbing state and the Bph domain is in a slightly red-shifted state (from 701 to 702 nm), which is photochemically inactive to red or white light. The amount of metastable complex formed increases with the degree of prior activation of PYP, reaching a maximum of 50% when PYP is fully activated compared to 0% when no PYP is activated. The saturation of complex formation at 50% is believed to be due to light-induced heterogeneity within the Ppr dimer. UV irradiation (365 nm) of the metastable complex state photoreverses the activated PYP and the red-shifted Bph to the initial dark state within seconds. We therefore postulate that Ppr functions as a UV-red light sensor and describe the different Ppr states that can be obtained depending on the light quality. Both red and white light upregulate the autokinase activity, while it is downregulated in the dark. The physiological state of Ppr is most likely a mixture of three different states, dark, metastable complex, and red light-activated, with fractional populations whose amounts depend on the light quality of the environment and that regulate the extent of phosphorylation by the kinase.

Light-induced structural changes at the entrance of the chromophore pocket of Agp1 phytochrome were investigated by using a thiol-reactive fluorescein derivative that is covalently attached to the genuine chromophore binding site (Cys-20) and serves as a polarity probe. In the apoprotein, the absorption spectrum of bound fluorescein is red-shifted with respect to that of the free label suggesting that the probe enters the hydrophobic chromophore pocket. Assembly of this construct with the chromophores phycocyanobilin or biliverdin is associated with a blue-shift of the fluorescein absorption band indicating the displacement of the probe out of the pocket. The probe does not affect the photochromic and kinetic properties of the noncovalent bilin adducts. Upon photoconversion to Pfr, the probe spectrum undergoes again a bathochromic shift and a strong rise in CD indicating a more hydrophobic and asymmetric environment. We propose that the environmental changes of the probe reflect conformational changes at the entrance of the chromophore pocket and are indicative for rearrangements of the chromophore ring A. Flash photolysis measurements showed that the absorption changes of the probe are kinetically coupled to the formation of Meta-R(C) and Pfr. In the biliverdin adduct, an additional component occurs that probably reflects a transition between two Meta-RC substates. Analogous results to that of the noncovalent phycocyanobilin adduct were obtained with the mutant V249C in which probe and chromophore are covalently attached. The conformational changes of the chromophore are correlated to proton transfer to the protein surface.

The functional role of the covalent attachment of the bilin chromophores biliverdin (BV) and phycocyanobilin (PCB) was investigated for phytochrome Agp1 from Agrobacterium tumefaciens using circular dichroism (CD) and transient absorption spectroscopy. Covalent and noncovalent adducts with these chromophores were prepared by using wild-type (WT) Agp1 (covalent BV and noncovalent PCB binding), mutant C20A in which the covalent BV binding site is eliminated, and mutant V249C in which the covalent PCB binding site is introduced. While the CD spectra of the P(r) forms of all these photochromic adducts are qualitatively the same, the CD spectrum of the P(fr) form of the covalent PCB adduct is unique in having a positive rotational strength in the Q-band which we assign to the Z-E isomerization of the C-D methine bridge. In the three other adducts, the Q-band CD in the P(fr) state is almost zero, suggesting that upon photoconversion a negative contribution from an out-of-plane rotation of the A ring of the chromophore compensates for the positive contribution from ring D. The contribution from ring A is absent or strongly reduced in the shorter pi-conjugation system of the covalent PCB adduct. The results from CD spectroscopy are consistent with a uniform geometry of the bilin chromophore in the covalent and noncovalent adducts. Transient absorption spectroscopy showed that the spectral changes and the kinetics of the P(r) to P(fr) photoconversion are not substantially affected by the covalent attachment of BV and PCB. The kinetics in the BV and PCB adducts mainly differ in the formation of P(fr) that is accelerated by 2 orders of magnitude in the PCB adducts, whereas the sequence of spectral transitions and the associated proton transfer processes are quite similar. We conclude that the P(r) to P(fr) photoconversion in the BV and PCB adducts of Agp1 involves the same relaxation processes and is thus governed by specific protein-cofactor interactions rather than by the chemical structure of the chromophore or the mode of attachment. The strongly reduced photostability of the noncovalent BV adduct suggests that covalent attachment in native Agp1 phytochrome prevents irreversible photobleaching and stabilizes the chromophore. The N-terminal peptide segment including amino acids 2-19 is essential for covalent attachment of the chromophore but dispensable for the spectral and kinetic properties of Agp1.

The bacteriophytochrome Agp1 was reconstituted with a locked 5Zs-biliverdin in which the C(4)=C(5) and C(5)-C(6) bonds of the methine bridge between rings A and B are fixed in the Z and syn configuration/conformation, respectively. In Agp1-5Zs the photoconversion proceeds via the Lumi-R intermediate to Meta-R(A), but the following millisecond-transition to Meta-R(C) is blocked. Consistently, no transient proton release was detected. The photoconversion of Agp1-5Zs is apparently arrested in a Meta-R(A)-like intermediate, since the subsequent syn to anti rotation around the C(5)-C(6) bond is prevented by the lock. The Meta-R(A)-like photoproduct was characterized by its distinctive CD spectrum suggesting a reorientation of ring D.

The effect of ionic strength on the conformational equilibrium between the I(2) intermediate and the signaling state I(2)' of the photoreceptor PYP and on the rate of recovery to the dark state were investigated by time-resolved absorption and fluorescence spectroscopy. With increasing salt concentration up to approximately 600 mM, the recovery rate k(3) decreases and the I(2)/I(2)' equilibrium (K) shifts in the direction of I(2)'. At higher ionic strength both effects reverse. Experiments with mono-(KCl, NaBr) and divalent (MgCl(2), MgSO(4)) salts show that the low salt effect depends on the ionic strength and not on the cation or anion species. These observations can be described over the entire ionic strength range by considering the activity coefficients of an interdomain salt bridge. At low ionic strength the activity coefficient decreases due to counterion screening whereas at high ionic strength binding of water by the salt leads to an increase in the activity coefficient. From the initial slopes of the plots of log k(3) and log K versus the square root of the ionic strength, the product of the charges of the interacting groups was found to be -1.3 +/- 0.2, suggesting a monovalent ion pair. The conserved salt bridge K110/E12 connecting the beta-sheet of the PAS core and the N-terminal domain is a prime candidate for this ion pair. To test this hypothesis, the mutants K110A and E12A were prepared. In K110A the salt dependence of the I(2)/I(2)' equilibrium was eliminated and of the recovery rate was greatly reduced below approximately 600 mM. Moreover, at low salt the recovery rate was six times slower than in wild-type. In E12A significant salt dependence remained, which is attributed to the formation of a novel salt bridge between K110 and E9. At high salt reversal occurs in both mutants suggesting that salting out stabilizes the more compact I(2) structure. However, chaotropic anions like SCN shift the I(2)/I(2)' equilibrium toward the partially unfolded I(2)' form. The salt linkage K110/E12 stabilizes the photoreceptor in the inactive state in the dark and is broken in the light-induced formation of the signaling state, allowing the N-terminal domain to detach from the beta-scaffold PAS core.

The mutants H250A and D197A of Agp1 phytochrome from Agrobacterium tumefaciens were prepared and investigated by different spectroscopic and biochemical methods. Asp-197 and His-250 are highly conserved amino acids and are part of the hydrogen-bonding network that involves the chromophore. Both substitutions cause a destabilization of the protonated chromophore in the Pr state as revealed by resonance Raman and UV-visible absorption spectroscopy. Titration experiments demonstrate a lowering of the pK(a) from 11.1 (wild type) to 8.8 in H250A and 7.2 in D197A. Photoconversion of the mutants does not lead to the Pfr state. H250A is arrested in a meta-Rc-like state in which the chromophore is deprotonated. For H250A and the wild-type protein, deprotonation of the chromophore in meta-Rc is coupled to the release of a proton to the external medium, whereas the subsequent proton re-uptake, linked to the formation of the Pfr state in the wild-type protein, is not observed for H250A. No transient proton exchange with the external medium occurs in D197A, suggesting that Asp-197 may be the proton release group. Both mutants do not undergo the photo-induced protein structural changes that in the wild-type protein are detectable by size exclusion chromatography. These conformational changes are, therefore, attributed to the meta-Rc --> Pfr transition and most likely coupled to the transient proton re-uptake. The present results demonstrate that Asp-197 and His-250 are essential for stabilizing the protonated chromophore structure in the parent Pr state, which is required for the primary photochemical process, and for the complete photo-induced conversion to the Pfr state.

The signaling state of the photoreceptor photoactive yellow protein is the long-lived intermediate I(2)'. The pH dependence of the equilibrium between the transient photocycle intermediates I(2) and I(2)' was investigated. The formation of I(2)' from I(2) is accompanied by a major conformational change. The kinetics and intermediates of the photocycle and of the photoreversal were measured by transient absorption spectroscopy from pH 4.6 to 8.4. Singular value decomposition (SVD) analysis of the data at pH 7 showed the presence of three spectrally distinguishable species: I(1), I(2), and I(2)'. Their spectra were determined using the extrapolated difference method. I(2) and I(2)' have electronic absorption spectra, with maxima at 370 +/- 5 and 350 +/- 5 nm, respectively. Formation of the signaling state is thus associated with a change in the environment of the protonated chromophore. The time courses of the I(1), I(2), and I(2)' intermediates were determined from the wavelength-dependent transient absorbance changes at each pH, assuming that their spectra are pH-independent. After the formation of I(2)' ( approximately 2 ms), these three intermediates are in equilibrium and decay together to the initial dark state. The equilibrium between I(2) and I(2)' is pH dependent with a pK(a) of 6.4 and with I(2)' the main species above this pK(a). Measurements of the pH dependence of the photoreversal kinetics with a second flash of 355 nm at a delay of 20 ms confirm this pK(a) value. I(2) and I(2)' are photoreversed with reversal times of approximately 55 micros and several hundred microseconds, respectively. The corresponding signal amplitudes are pH dependent with a pK(a) of approximately 6.1. Photoreversal from I(2)' dominates above the pK(a). The transient accumulation of I(2)', the active state of photoactive yellow protein, is thus controlled by the proton concentration. The rate constant k(3) for the recovery to the initial dark state also has a pK(a) of approximately 6.3. This equality of the equilibrium and kinetic pK(a) values is not accidental and suggests that k(3) is proportional to [I(2)'].

Since the habitat of Halorhodospira halophila is distinctly alkaline, we investigated the kinetics and intermediates of the photocycle and photoreversal of the photoreceptor photoactive yellow protein (PYP) from pH 8 to 11. SVD analysis of the transient absorption time traces in a broad wavelength range (330-510 nm) shows the presence of three spectrally distinct species (I1, I1', and I2') at pH 10. The spectrum of I1' was obtained in two different ways. The maximal absorption is at 425 nm. I1' probably has a deprotonated chromophore and may be regarded as the alkaline form of I2'. At pH 10, the I1 intermediate decays in approximately 330 micros in part to I1' before I1 and I1' decay further to I2' in approximately 1 ms. From the rise of I2' (approximately 1 ms) to the end of the photocycle, the three intermediates (I1, I1', and I2') remain in equilibrium and decay together to P in approximately 830 ms. Assuming that the spectra of I1, I1', and I2' are pH-independent, their time courses were determined. On the millisecond to second time scale, they are in a pH-dependent equilibrium with a pKa of approximately 9.9. With an increase in pH, the I1 and I1' populations increase at the expense of the amount of I2'. The apparent rate constant for the recovery of P slows with an increase in pH with a pKa of approximately 9.7. The equal pH dependence of this rate and the equilibrium concentrations follows, if we assume that the equilibration rates between the intermediates are much faster than the recovery rate and that the recovery occurs from I2'. The pKa of approximately 9.9 is assigned to the deprotonation of the phenol of the surface-exposed chromophore in the I1'-I2' equilibrium. The I1-I1' equilibrium is pH-independent. Photoreversal experiments at pH 10 with the second flash at 355 nm indicate the presence of only one I2-like intermediate, which we assign on the basis of its lambda(max) value to I2'. After the rapid unresolved photoisomerization to I2'(trans), the reversal pathway back to P involves two sequential steps (60 micros and 3 ms). The amplitude spectra show that I1'(trans) and I1(trans) intermediates participate in this reversal.

Light-induced activation of the photoreceptors phytochrome and photoactive yellow protein (PYP) is accompanied by protonation changes of the respective chromophores and key residues in the protein moiety. For both systems, proton exchange with the external medium could be observed with pH electrode measurements and with UV-visible absorption spectroscopy using appropriate pH indicator dyes. From these signals, the stoichiometry of proton release and uptake, respectively, was determined by different calibration procedures which will be presented and discussed. Kinetic information on these processes is only available from time-resolved measurements with pH indicator dyes. Vibrational spectroscopy methods such as Fourier transform infrared spectroscopy and resonance Raman scattering provided information on the protonation state of individual functional groups suggesting that internal proton transfer processes are involved as well. Deuterium kinetic isotope effects that occurred in the Pr --> Pfr phototransformation of the bacteriophytochromes Cph1 and Agp1 were consistent with proton transfer reactions as rate-limiting steps. In contrast, the apparent rate constants in the photocycle of PYP exhibited only small kinetic isotope effects that could not be interpreted conclusively. Possible mechanisms of proton transfer in the activation of phytochrome and PYP will be discussed.

We investigated the photocycle of mutants Y98Q and Y98F of the photoactive yellow protein (PYP) from Halorhodospira halophila. Y98 is located in the beta4-beta5 loop and is thought to interact with R52 in the alpha3-alpha4 loop thereby stabilizing this region. Y98 is conserved in all known PYP species, except in Ppr and Ppd where it is replaced by F. We find that replacement of Y98 by F has no significant effect on the photocycle kinetics. However, major changes were observed with the Y98Q mutant. Our results indicate a requirement for an aromatic ring at position 98, especially for recovery and a normal I1/I2 equilibrium. The ring of Y98 could stabilize the beta4-beta5 loop. Alternatively, the Y98 ring could transiently interact with the isomerized chromophore ring, thereby stabilizing the I2 intermediate in the I1/I2 equilibrium. For Y98Q, the decay of the signaling state I2' was slowed by a factor of approximately 40, and the rise of the I2 and I2' intermediates was slowed by a factor of 2-3. Moreover, the I1 intermediate is in a pH-dependent equilibrium with I2/I2' with the ratio of the I1 and I2 populations close to one at pH 7 and 50 mM KCl. From pH 5.5 to 8, the equilibrium shifts toward I1, with a pKa of approximately 6.3. Above pH 8, the populations of I1 and I2/I2' decrease due to an equilibrium between I1 and an additional species I1' which absorbs at approximately 425 nm (pKa approximately 9.8) and which we believe to be an I2-like form with a surface-exposed deprotonated chromophore. The I1/I2/I2' equilibrium was found to be strongly dependent on the KCl concentration, with salt stabilizing the signaling state I2' up to 600 mM KCl. This salt-induced transition to I2' was analyzed and interpreted as ion binding to a specific site. Moreover, from analysis of the amplitude spectra, we conclude that KCl exerts its major effect on the I2 to I2' transition, i.e., the global conformational change leading to the signaling state I2' and the exposure of a hydrophobic surface patch. In wild type and Y98F, the I1/I2 equilibrium is more on the side of I2/I2' as compared to Y98Q but is also salt-dependent at pH 7. The I2 to I2' transition appears to be controlled by an ionic lock, possibly involving the salt bridge between K110 on the beta-scaffold and E12 on the N-terminal cap. Salt binding would break the salt bridge and weaken the interaction between the two domains, facilitating the release of the N-terminal domain from the beta-scaffold in the formation of I2'.

The Pr --> Pfr phototransformation of the bacteriophytochrome Agp1 from Agrobacterium tumefaciens and the structures of the biliverdin chromophore in the parent states and the cryogenically trapped intermediate Meta-R(C) were investigated with resonance Raman spectroscopy and flash photolysis. Strong similarities with the resonance Raman spectra of plant phytochrome A indicate that in Agp1 the methine bridge isomerization state of the chromophore is ZZZasa in Pr and ZZEssa in Pfr, with all pyrrole nitrogens being protonated. Photoexcitation of Pr is followed by (at least) three thermal relaxation components in the formation of Pfr with time constants of 230 micros and 3.1 and 260 ms. H2O/D2O exchange reveals kinetic isotope effects of 1.9, 2.6, and 1.3 for the respective transitions that are accompanied by changes of the amplitudes. The second and the third relaxation correspond to the formation and decay of Meta-R(C), respectively. Resonance Raman measurements of Meta-R(C) indicate that the chromophore adopts a deprotonated ZZE configuration. Measurements with a pH indicator dye show that formation and decay of Meta-R(C) are associated with proton release and uptake, respectively. The stoichiometry of the proton release corresponds to one proton per photoconverted molecule. The coupling of transient chromophore deprotonation and proton release, which is likely to be an essential element in the Pr --> Pfr photocon-version mechanism of phytochromes in general, may play a crucial role for the structural changes in the final step of the Pfr formation that switch between the active and the inactive state of the photoreceptor.

We investigated the kinetics of photoreversal from the I(1) and I(2) intermediates of photoactive yellow protein (PYP) by time-resolved optical absorption spectroscopy with double flash excitation. A first flash, at 430 nm, initiated the photocycle. After a variable time delay, the I(1) intermediate was photoreversed by a second flash, at 500 nm, or a mixture of I(2) and I(2)' intermediates was photoreversed by a second flash, at 355 nm. By varying the delay from 1 micros to 3 s, we were able to selectively excite the intermediates I(1), I(2), and I(2)'. The photoreversal kinetics of I(2) and I(2)' at 21 different delays and two wavelengths (340 and 450 nm) required two exponentials for a global fit with time constants of tau(1) = 57 +/- 5 micros and tau(2) = 380 +/- 40 micros (pH 6, 20 degrees C). These were assigned to photoreversal from sequential I(2) and I(2)' intermediates, respectively. The good agreement of the delay dependence of the two amplitudes, A(1) and A(2), with the time dependence of the I(2) and I(2)' populations provided strong evidence for the sequential model. The persistence of A(1) beyond delay times of 5 ms and its decay, together with A(2) around 500 ms, suggest moreover that I(2) and I(2)' are in thermal equilibrium. The wavelength dependence of the photoreversal kinetics was measured at 26 wavelengths from 510 to 330 nm at the two fixed delays of 1 and 10 ms. These data also required two exponentials for a global fit with tau(1) = 59 +/- 5 micros and tau(2) = 400 +/- 40 micros, in good agreement with the delay results. Photoreversal from I(2)' is slower than from I(2), since, in addition to chromophore protonation, the global conformational change has to be reversed. Our data thus provide a first estimate of about 59 micros for deprotonation and 400 micros for the structural change, which also occurs in the thermal decay of the signaling state but is obscured there since reisomerization is rate-limiting. The first step in photoreversal is rapid cis-trans isomerization of the chromophore, which we could not resolve, but which was detected by the instantaneous increase in absorbance between 330 and 380 nm. In agreement with this observation, the spectrum of the I(2)'(trans) intermediate, derived from the A(2) amplitude spectrum, has a much larger extinction coefficient than the spectrum of the I(2)'(cis) intermediate. With a first flash, at 430 nm, and a second flash, at 500 nm, we observed efficient photoreversal of the I(1) intermediate at a delay of 20 micros when most molecules in the cycle are in I(1). We conclude that each of the three intermediates studied can be reversed by a laser flash. Depending on the progression of the photocycle, reversal becomes slower with the time delay, thus mirroring the individual steps of the forward photocycle.

The absorption and CD spectra of wild-type PYP, apo-PYP, and the mutants, E46Q and M100A, were measured between 250 and 550 nm. At neutral pH, the two very weak absorption bands of wild-type PYP at 307 and 318 nm (epsilon(max) = 600 +/- 100 M(-1) cm(-1) at 318 nm) are associated with quite strong positive CD bands (Deltaepsilon(max) approximately 6.8 M(-1) cm(-1)). Both sets of bands are absent in the apoprotein. On the basis of this evidence, we assign these optical signals to the n --> pi* transition of the oxygen of the carbonyl group of the 4-hydroxycinnamic acid chromophore, which is expected to be electric dipole forbidden but magnetic dipole allowed. The progression of narrow bands at 307 and 318 nm with a shoulder in the CD around 329 nm is due to vibrational fine structure with a frequency of about 1050 +/- 50 cm(-1). This is the carbonyl stretch frequency in the electronically excited state and is well-known from the vibrational structure in the CD spectra of carbonyl compounds. The positive sign of the CD in the near UV is in accordance with the octant rule and the high-resolution X-ray structure, if we assume that the NH group of cysteine 69 to which the carbonyl is hydrogen bonded is the principle perturbant. Similar absorption and CD spectra were observed in the range of 300-340 nm for the mutants E46Q and M100A at neutral pH. Protonation of the trans chromophore by lowering the pH in the dark (without photoisomerization) broadens the 307 and 318 nm CD bands in the mutant E46Q but does not significantly affect their positions or alter their sign. For the long-lived I(2) photointermediate of the mutant M100A with protonated cis chromophore, we observed that the sign of the rotational strength in the 310-320 nm range is negative (i.e., opposite to that in the dark state with trans chromophore). This suggests that the light-induced isomerization of the chromophore, which leads to breaking of the hydrogen bond with the backbone amide of C69, brings the carbonyl into a new protein environment with different asymmetry than in the unbleached protein. The observed change in sign is mainly due to this effect, but a change in chromophore twist may also contribute. Thus, the 318 nm CD signal is a sensitive marker for the environment of the chromophore carbonyl, which samples various environments and configurations during the photocycle.

The kinetics and mechanism of the autocatalytic assembly of holo-Cph1 phytochrome (from Synechocystis) from the apoprotein and the bilin chromophores phycocyanobilin (PCB) and phycoerythrobilin (PEB) were investigated by stopped flow and circular dichroism. At 1:1 stoichiometry, pH 7.9, and 10 degrees C, SVD analysis of the kinetic data for PCB revealed three spectral components involving three transitions with time constants tau(1) approximately 150 ms, tau(2) approximately 2.5 s, and tau(3) approximately 50 s. Tau(1) was associated with a major red shift and transfer of oscillator strength from the Soret region to the 680 nm region. When the sulfhydryl group of cysteine 259 was blocked with iodoacetamide, preventing the formation of a covalent adduct, a noncovalent red-shifted complex (680 nm) was formed with a time constant of 200 ms. Tau(1) could thus be assigned to the formation of a noncovalent complex. The absorption changes during tau(1) are due to the formation of the extended conformation of the linear tetrapyrrole and to its protonation in the binding pocket. From the concentration and pH dependence of the kinetics we obtained a value of 1.5 microM for the K(D) of this noncovalent complex and a value of 8.4 for the pK(a) of the proton donor. The tau(2) component was associated with a blue shift of about 25 nm and was attributed to the formation of the covalent bond (P(r)), accompanied with the loss of the 3-3' double bond to ring A. Tau(3) was due to photoconversion to P(fr). For PEB, which is not photochromic, the formation of the noncovalent complex is faster (tau(1) = 70 ms), but the covalent bond formation is about 80 times slower (tau(2) = 200 s) than with the natural chromophore PCB. The CD spectra of the PCB adduct in the 250-800 nm range show that the chromophore geometries in P(r) and P(fr) are similar to those in plant phytochrome. The opposite rotational strengths of P(r) and P(fr) in the longest wavelength band suggest that the photoisomerization induces a reversal of the chirality. The Cph1 complex with noncovalently bound PCB was still photochromic when cysteine 259 was blocked with IAA or with the bulkier IAF. The covalent linkage to cysteine 259 is thus not required for photoconversion. The CD spectra of the noncovalently bound PCB in P(r)- and P(fr)-like states are qualitatively similar to those of the covalent adducts, suggesting analogous structures in the binding pocket. The noncovalent interactions with the binding pocket are apparently sufficient to hold the chromophore in the appropriate geometry for photoisomerization.

The kinetics of the photocycle of PYP and its mutants E46Q and E46A were investigated as a function of pH. E46 is the putative donor of the chromophore which becomes protonated in the I(2) intermediate. For E46Q we find that I(2) is in a pH-dependent equilibrium with its precursor I(1)' with a pK(a) of 8.15 and n = 1. From this result and from experiments with pH indicator dyes, we conclude that in the I(1)' to I(2) transition one proton is taken up from the external medium. The pK(a) of 8.15 is that of the surface-exposed chromophore in the equilibrium between I(1)' and I(2) and is close to that of the phenolate group of p-hydroxycinnamic acid. The pH-dependent I(1)'/I(2) equilibrium with associated H(+) uptake is reminiscent of the M(I)/M(II) equilibrium in the formation of the signaling state of rhodopsin. Well above this pK(a) no I(2) is formed and I(1)' returns in a pH-independent manner to the initial state P. The decay rate for the return to P via I(2) is between pH 4 and pH 8, exactly proportional to the hydroxide concentration (first order), and the deprotonation of the chromophore in this transition occurs by hydroxide uptake. Well above the pK(a) of 8.15 the apparent rate constant for the return to P is constant due to the branching from I(1)'. Complementary measurements with the pH indicator dye cresol red at pH 8.3 show that the remaining PYP molecules that still cycle via I(2) take up one proton in the formation of I(2). Together, these observations provide compelling evidence that during the photocycle the chromophore in E46Q is protonated and deprotonated from the external medium. For the yellow form of the mutant E46A the apparent rate constant for the return to P is also linear in [OH(-)] below about pH 8.3 and constant above about pH 9.5, with a pK(a) value of 8.8 for I(1)', suggesting a similar mechanism of chromophore protonation/deprotonation as in E46Q. For wild type qualitatively similar observations were made: the amplitude of I(2) decreased at alkaline pH, I(1)' and I(2) were in equilibrium, and I(1)' decayed together with the return to P. Chromophore hydrolysis prevented, however, an accurate determination of the pK(a) of I(1)'. We estimate that its value is above 11. The ground state P is in the dark in a pH-dependent equilibrium with a low-pH bleached form P(bl) with protonated chromophore. The pK(a) values for these equilibria are 4.8 and 7.9 for E46Q and E46A, respectively. When the pH is close to these pK(a)'s, the kinetics of the photocycle contains additional components in the millisecond time range. Using pH-jump stopped-flow experiments, we show that these contributions are due to the relaxation of the P/P(bl) equilibrium which is perturbed by the rapid decrease in the P concentration caused by the flash excitation of P. The condition for the occurrence of this effect is that the relaxation time of the P/P(bl) equilibrium is faster than the photocycle time.

We investigated the dimerization of phytochrome Cph1 from the cyanobacterium Synechocystis by fluorescence resonance energy transfer (FRET). As donor we used the chromophore analogue phycoerythrobilin (PEB) and as acceptor either the natural chromophore phycocyanobilin (PCB; hetero transfer) or PEB (homo transfer). Both chromophores bind in a 1:1 stoichiometry to apo-monomers expressed in Escherichia coli. Energy transfer was characterized by time-resolved fluorescence intensity and anisotropy decay after excitation of PEB by picosecond pulses from a tunable Ti-sapphire laser system. ApoCph1 was first assembled with PEB at a low stoichiometry of 0.1. The remaining sites were then sequentially titrated with PCB. In the course of this titration, the mean lifetime of PEB decreased from 3.33 to 1.25 ns in the P(r) form of Cph1, whereas the anisotropy decay was unaffected. In the P(fr)/P(r) photoequilibrium (about 65% P(fr)), the mean lifetime decreased significantly less, to 1.67 ns. These observations provide strong support for inter-chromophore hetero energy transfer in mixed PEB/PCB dimers. The reduced energy transfer in P(fr) may be due to a structural difference but is at least in part due to the difference in spectral overlap, which was 4.1 x 10(-13) and 1.6 x 10(-13) cm(3) M(-1) in P(r) and P(fr), respectively. From the changes in the mean lifetime, rates of hetero energy transfer of 0.68 and 0.37 ns(-1) were calculated for the P(r) form and the P(fr)/P(r) photoequilibrium, respectively. Sequential titration of apo Cph1 with PEB alone to full occupancy did not affect the intensity decay but led to a substantial increase in depolarization. This is the experimental signature of homo energy transfer. Values for the rate of energy transfer k(HT) (0.47 ns(-1)) and the angle 2theta between the transition dipole moment directions (2theta = 45 +/- 5 degrees) were determined from an analysis of the concentration dependence of the anisotropy at five different PEB/Cph1 stoichiometries. The independently determined rates of hetero and homo energy transfer are thus of comparable magnitude and consistent with the energy transfer interpretation. Using these results and exploiting the 2-fold symmetry of the dimer, the chromophore-chromophore distance R(DA) was calculated and found to be in the range 49 A < R(DA) < 63 A. Further evidence for energy transfer in Cph1 dimers was obtained from dilution experiments with PEB/PEB dimers: the lifetime was unchanged, but the anisotropy increased as the dimers dissociated with increasing dilution. These experiments allowed a rough estimate of 5 +/- 3 microM for the dimer dissociation constant. With the deletion mutant Cph1Delta2 that lacks the carboxy terminal histidine kinase domain less energy transfer was observed suggesting that in this mutant dimerization is much weaker. The carboxy terminal domain of Cph1 that is involved in intersubunit trans-phosphorylation and signal transduction thus plays a dominant role in the dimerization. The FRET method provides a sensitive assay to monitor the association of Cph1 monomers.

We studied the kinetics of proton uptake and release by photoactive yellow protein (PYP) from Ectothiorhodospira halophila in wild type and the E46Q and E46A mutants by transient absorption spectroscopy with the pH-indicator dyes bromocresol purple or cresol red in unbuffered solution. In parallel, we investigated the kinetics of chromophore protonation as monitored by the rise and decay of the blue-shifted state I(2) (lambda(max) = 355 nm). For wild type the proton uptake kinetics is synchronized with the fast phase of I(2) formation (tau = 500 micros at pH 6.2). The transient absorption signal from the dye also contains a slower component which is not due to dye deprotonation but is caused by dye binding to a hydrophobic patch that is transiently exposed in the structurally changed and partially unfolded I(2) intermediate. This conclusion is based on the wavelength, pH, and concentration dependence of the dye signal and on dye measurements in the presence of buffer. SVD analysis, moreover, indicates the presence of two components in the dye signal: protonation and dye binding. The dye binding has a rise time of about 4 ms and is coupled kinetically with a transition between two I(2) intermediates. In the mutant E46Q, which lacks the putative internal proton donor E46, the formation of I(2) is accelerated, but the proton uptake kinetics remains kinetically coupled to the fast phase of I(2) formation (tau = 100 micros at pH 6.3). For this mutant the protein conformational change, as monitored by the dye binding, occurs with about the same time constant as in wild type but with reduced amplitude. In the alkaline form of the mutant E46A the formation of the I(2)-like intermediate is even faster as is the proton uptake (tau = 20 micros at pH 8.3). No dye binding occurred in E46A, suggesting the absence of a conformational change. In all of the systems proton release is synchronized with the decay of I(2). Our results support mechanisms in which the chromophore of PYP is protonated directly from the external medium rather than by the internal donor E46.

The P(r) to P(fr) transition of recombinant Synechocystis PCC 6803 phytochrome Cph1 and its N-terminal sensor domain Cph1Delta2 is accompanied by net acidification in unbuffered solution. The extent of this net photoreversible proton release was measured with a conventional pH electrode and increased from less than 0.1 proton released per P(fr) formed at pH 9 to between 0.6 (Cph1) and 1.1 (Cph1Delta2) H(+)/P(fr) at pH 6. The kinetics of the proton release were monitored at pH 7 and pH 8 using flash-induced transient absorption measurements with the pH indicator dye fluorescein. Proton release occurs with time constants of approximately 4 and approximately 20 ms that were also observed in parallel measurements of the photocycle (tau(3) and tau(4)). The number of transiently released protons per P(fr) formed is about one. This H(+) release phase is followed by a proton uptake phase of a smaller amplitude that has a time constant of approximately 270 ms (tau(5)) and is synchronous with the formation of P(fr). The acidification observed in the P(r) to P(fr) transition with pH electrodes is the net effect of these two sequential protonation changes. Flash-induced transient absorption measurements were carried out with Cph1 and Cph1Delta2 at pH 7 and pH 8. Global analysis indicated the presence of five kinetic components (tau(1)-tau(5): 5 and 300 micros and 3, 30, and 300 ms). Whereas the time constants were approximately pH independent, the corresponding amplitude spectra (B(1), B(3), and B(5)) showed significant pH dependence. Measurements of the P(r)/P(fr) photoequilibrium indicated that it is pH independent in the range of 6.5-9.0. Analysis of the pH dependence of the absorption spectra from 6.5 to 9.0 suggested that the phycocyanobilin chromophore deprotonates at alkaline pH in both P(r) and P(fr) with an approximate pK(a) of 9.5. The protonation state of the chromophore at neutral pH is therefore the same in both P(r) and P(fr). The light-induced deprotonation and reprotonation of Cph1 at neutral pH are thus due to pK(a) changes in the protein moiety, which are linked to conformational transitions occurring around 4 and 270 ms after photoexcitation. These transient structural changes may be relevant for signal transduction by this cyanobacterial phytochrome.

Light-induced isomerization leads to orientational changes of the retinylidene chromophore of bacteriorhodopsin in its binding pocket. The chromophore reorientation has been characterized by the following methods: polarized absorption spectroscopy in the visible, UV and IR; polarized resonance Raman scattering; solid-state deuterium nuclear magnetic resonance; neutron and X-ray diffraction. Most of these experiments were performed at low temperatures with bacteriorhodopsin trapped in one or a mixture of intermediates. Time-resolved measurements at room temperature with bacteriorhodopsin in aqueous suspension can currently only be carried out with transient polarized absorption spectroscopy in the visible. The results obtained to date for the initial state and the K, L and M intermediates are presented and discussed. The most extensive data are available for the M intermediate, which plays an essential role in the function of bacteriorhodopsin. For this intermediate the various methods lead to a consistent picture: the curved all-trans polyene chain in the initial state straightens out in the M intermediate (13-cis) and the chain segment between C(5) and C(13) tilts upwards in the direction of the cytoplasmic surface. The kink at C(13) allows the positions of beta-ionone ring and Schiff base nitrogen to remain approximately fixed.

The authors report a case of postradiotherapy cervical myelopathy after treatment of laryngeal cancer. The patient aged 61 was referred to a neurological hospital department with suspected metastasis of laryngeal cancer to the spine with symptoms indicating cervical cord lesion. During observation and after imaging examinations of the cervical spine cancer recurrence was excluded. History data and imaging methods served a basis for the diagnosis of postradiation myelopathy. The authors warn against too ready diagnosis of cancer in such cases and a repetition of radiotherapy.