Photochemical intermediates of Arabidopsis phototropin 2 LOV domains associated with conformational changes

The photochemical reactions of Arabidopsis phototropin 2 light- oxygen-voltage domain 2 (LOV2) with the linker region (LOV2-linker), without the linker (LOV2), and LOV1 were studied using the time-resolved transient grating (TG) and transient lens (TrL) methods. Although the absorption spectra did not change after the formation of the adduct species, a small volume expansion process with a time constant of 9 ms was observed for LOV2. For the LOV2-linker, at 293 K, a volume contraction process with a time constant of 140 mus was observed in addition to a volume expansion process with 9 ms and the diffusion coefficient change with 2 ms. The reaction intermediate species were characterized on the basis of their thermodynamic properties, such as changes in enthalpy, thermal expansion, and heat capacity. For the first intermediate (S(390)), the values of these properties were similar to those of the ground state for both LOV2 and LOV2-linker. A relatively large thermal expansion volume (0.09 cm(3)mol(-1)K(-1)) and a positive heat capacity change (4.7 kJ mol(-1)K(-1)) were detected for the intermediates of LOV2-linker. These characteristic features were interpreted in terms of structural fluctuation and exposure of hydrophobic residues in the linker domain, respectively. The enthalpy change of S(390) of the LOV1 domain was significantly greater than changes for the LOV2 or LOV2-linker samples. Data from this study support a major conformational change of the linker region in the photochemical reaction of phototropin.     

Laser-induced transient grating analysis of dynamics of interaction between sensory rhodopsin II D75N and the HtrII transducer

The interaction between sensory rhodopsin II (SRII) and its transducer HtrII was studied by the time-resolved laser-induced transient grating method using the D75N mutant of SRII, which exhibits minimal visible light absorption changes during its photocycle, but mediates normal phototaxis responses. Flash-induced transient absorption spectra of transducer-free D75N and D75N joined to 120 amino-acid residues of the N-terminal part of the SRII transducer protein HtrII (DeltaHtrII) showed only one spectrally distinct K-like intermediate in their photocycles, but the transient grating method resolved four intermediates (K(1)-K(4)) distinct in their volumes. D75N bound to HtrII exhibited one additional slower kinetic species, which persists after complete recovery of the initial state as assessed by absorption changes in the UV-visible region. The kinetics indicate a conformationally changed form of the transducer portion (designated Tr*), which persists after the photoreceptor returns to the unphotolyzed state. The largest conformational change in the DeltaHtrII portion was found to cause a DeltaHtrII-dependent increase in volume rising in 8 micros in the K(4) state and a drastic decrease in the diffusion coefficient (D) of K(4) relatively to those of the unphotolyzed state and Tr*. The magnitude of the decrease in D indicates a large structural change, presumably in the solvent-exposed HAMP domain of DeltaHtrII, where rearrangement of interacting molecules in the solvent would substantially change friction between the protein and the solvent.     

Transducer binding establishes localized interactions to tune sensory rhodopsin II

In haloarchaea, sensory rhodopsin II (SRII) mediates a photophobic response to avoid photo-oxidative damage in bright light. Upon light activation the receptor undergoes a conformational change that activates a tightly bound transducer molecule (HtrII), which in turn by a chain of homologous reactions transmits the signal to the chemotactic eubacterial two-component system. Here, using single-molecule force spectroscopy, we localize and quantify changes to the intramolecular interactions within SRII of Natronomonas pharaonis (NpSRII) upon NpHtrII binding. Transducer binding affected the interactions at transmembrane alpha helices F and G of NpSRII to which the transducer was in contact. Remarkably, the interactions were distributed asymmetrically and significantly stabilized alpha helix G entirely but alpha helix F only at its extracellular tip. These findings provide unique insights into molecular mechanisms that "prime" the complex for signaling, and guide the receptor toward transmitting light-activated structural changes to its cognate transducer.     

Structural insights into the early steps of receptor-transducer signal transfer in archaeal phototaxis

Electron paramagnetic resonance-based inter-residue distance measurements between site-directed spin-labelled sites of sensory rhodopsin II (NpSRII) and its transducer NpHtrII from Natronobacterium pharaonis revealed a 2:2 complex with 2-fold symmetry. The core of the complex is formed by the four transmembrane helices of a transducer dimer. Upon light excitation, the previously reported flap-like movement of helix F of NpSRII induces a conformational change in the transmembrane domain of the transducer. The inter-residue distance changes determined provide strong evidence for a rotary motion of the second transmembrane helix of the transducer. This helix rotation becomes uncoupled from changes in the receptor during the last step of the photocycle.     

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein

Themodynamic and transport properties of intermediate states of the photocyclic reaction of photoactive yellow protein (PYP) were studied by a combination of the pulsed laser-induced transient grating (TG), transient lens (TrL), and photoacoustic (PA) spectroscopies from tens of nanoseconds to hundreds of milliseconds. The diffusion coefficients (D) of PYP in the ground state (pG) and of the second intermediate state (pB) were determined by the TG analysis, and it was found that D of pG is about 1.2 times larger than D of pB. At the same time, D at various denatured conditions were measured using guanidine hydrochloride as the denaturant. D of completely unfolded protein is about 0.4 times that of the native form. The enthalpy of pB is estimated to be 60 kJ/mol by the TrL method with an assumption that the volume change of pB is not sensitive to the temperature. Since the enthalpy of the first intermediate state (pR) is as high as 160 kJ/mol, it implies that most of the photon energy is stored as the strain of the protein in pR, and this may be the driving force for the successive reaction to pB. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients between pG and pR was calculated. All of the characteristic features of PYP, the negative volume change, the larger thermal expansion coefficient, and the slower diffusion process, indicate that the intermediate pR and pB are reasonably interpreted in terms of the unfolded (loosened) protein structure.     

Structural change of site-directed mutants of PYP: new dynamics during pR state

The energetics, protein dynamics, and diffusion coefficients of three mutants of photoactive yellow protein, R52Q, P68A, and W119G, were studied by the transient grating and pulsed laser-induced photoacoustic method. We observed a new dynamics with a lifetime of approximately 1 micro s in the transient grating signal, which is silent by the light absorption technique. This fact indicates that, after the structure change around the chromophore is completed (pR(1)), the protein part located far from the chromophore is still moving to finally create another pR (pR(2)) species, which can transform to the next intermediate, pB. Although the kinetics of pR(2)-->pB-->pG are very different depending on the mutants, the enthalpies of the first long-lived (in micro seconds, 100-micro s range) intermediate species (pR(2)) are similar and very high for all mutants. The diffusion coefficients of the parent (pG) and pB species of the mutants are also similar to that of the wild-type photoactive yellow protein. From the temperature dependence of the volume change, the difference in the thermal expansion coefficients taken as indicator of the flexibility of the structure between pG and pR(2) is measured. They are also similar to that of the wild-type photoactive yellow protein. These results suggest that the protein structures of pR(2) and pB in these mutants are globally different from that of pG, and this structural change is not altered so much by the single amino acid residue mutation. This is consistent with the partially unfolded nature of these intermediate species. On the other hand, the volume changes during pR(1)-->pR(2) are sensitive to the mutations, which may suggest that the volume change reflects a rather local character of the structure, such as the chromophore-protein interaction.     

Oligomeric-State-Dependent Conformational Change of the BLUF Protein TePixD (Tll0078)

The photochemical reaction dynamics of a BLUF (sensors of blue light using FAD) protein, PixD, from a thermophilic cyanobacterium Thermosynechococcus elongatus BP-1 (TePixD, Tll0078) were studied by pulsed laser-induced transient grating method. After the formation of an intermediate species with a red-shifted absorption spectrum, two new reaction phases reflecting protein conformational changes were discovered; one reaction phase manifested itself as expansion of partial molar volume with a time constant of 40 μs, whereas the other reaction phase represented a change in the diffusion coefficient D [i.e., the diffusion-sensitive conformational change (DSCC)]. D decreased from 4.9 × 10^− 11 to 4.4 × 10^− 11 m² s^− 1 upon the formation of the first intermediate, and subsequently showed a more pronounced decrease to 3.2 × 10^− 11 m² s^− 1 upon formation of the second intermediate. From a global analysis of signals at various grating wavenumbers, the time constant of D-change was determined to be 4 ms. Although the magnitude and rate constant of the faster volume change were independent of protein concentration, the amplitude of the signal that reflects the later DSCC significantly decreased as the protein concentration decreased. This concentration dependence suggests that two species exist in solution: a reactive species exhibiting the DSCC, and a second species that is nonreactive. The fraction of these species was found to be dependent on the concentration. The difference in reactivity was attributed to the different oligomeric states of TePixD (i.e., pentamer and decamer). The equilibrium of these states in the dark was confirmed by size-exclusion chromatography at various concentrations. These results demonstrated that only the decamer state is responsible for the conformational change. The results may suggest that the oligomeric state is functionally important in the signal transduction of this photosensory protein.     

Salt-driven equilibrium between two conformations in the HAMP domain from Natronomonas pharaonis: the language of signal transfer?

HAMP domains (conserved in histidine kinases, adenylyl cyclases, methyl-accepting chemotaxis proteins, and phosphatases) perform their putative function as signal transducing units in diversified environments in a variety of protein families. Here the conformational changes induced by environmental agents, namely salt and temperature, on the structure and function of a HAMP domain of the phototransducer from Natronomonas pharaonis (NpHtrII) in complex with sensory rhodopsin II (NpSRII) were investigated by site-directed spin labeling electron paramagnetic resonance. A series of spin labeled mutants were engineered in NpHtrII157, a truncated analog containing only the first HAMP domain following the transmembrane helix 2. This truncated transducer is shown to be a valid model system for a signal transduction domain anchored to the transmembrane light sensor NpSRII. The HAMP domain is found to be engaged in a "two-state" equilibrium between a highly dynamic (dHAMP) and a more compact (cHAMP) conformation. The structural properties of the cHAMP as proven by mobility, accessibility, and intra-transducer-dimer distance data are in agreement with the four helical bundle NMR model of the HAMP domain from Archaeoglobus fulgidus.     

Photoreverse reaction dynamics of octopus rhodopsin

Photoreverse reactions of octopus rhodopsin (Rh) from acid-metarhodopsin (Acid-Meta), which is the final product of the photoreaction of Rh, to Rh were studied by the time-resolved transient absorption and transient grating methods. The time course of the absorption signal showed a rapid change within 500 ns followed by one phase with a time constant of approximately 470 micros, whereas the transient grating signal indicates three phases with time constants of <500 ns, approximately 490 micros, and 2.6 ms. The faster two phases indicate the conformational change in the vicinity of the chromophore, and the slowest one represents conformational change far from the chromophore. The absorption spectrum of the first intermediate created just after the laser excitation (<500 ns) is already very similar to the final product, Rh. This behavior is quite different from that of the forward reaction from Rh to Acid-Meta, in which several intermediates with different absorption spectra are involved within 50 ns-500 micros. This result indicates that the conformation around the chromophore is easily adjusted from all-trans to 11-cis forms compared with that from 11-cis to all-trans forms. Furthermore, it was found that the protein energy is quickly relaxed after the excitation. One of the significantly different properties between Rh and Acid-Meta is the diffusion coefficient (D). D is reduced by about half the transformation from Rh to Acid-Meta. This large reduction was interpreted in terms of the helix opening of the Rh structure.     

Structural analysis of a HAMP domain: the linker region of the phototransducer in complex with sensory rhodopsin II

Sensory rhodopsin II, the photophobic receptor from Natronomonas pharaonis (NpSRII)5, forms a 2:2 complex with its cognate transducer (N. pharaonis halobacterial transducer of rhodopsins II (NpHtrII)) in lipid membranes. Light activation of NpSRII leads to a displacement of helix F, which in turn triggers a rotation/screw-like motion of TM2 in NpHtrII. This conformational change is thought to be transmitted through the membrane adjacent conserved signal transduction domain in histidine kinases, adenylyl cyclases, methyl-accepting chemotaxis proteins, and phosphatases (HAMP domain) to the cytoplasmic signaling domain of the transducer. The architecture and function of the HAMP domain are still unknown. In order to obtain information on the structure and dynamics of this region, EPR experiments on a truncated transducer (NpHtrII(157)) and NpSRII, site-directed spin-labeled and reconstituted into purple membrane lipids, have been carried out. A nitroxide scanning involving residues in the transducer helix TM2, in the predicted AS-1 region, and at selected positions in the following connector and AS-2 regions of the HAMP domain has been performed. Accessibility and dynamics data allowed us to identify a helical region up to residue Ala(94) in the AS-1 amphipathic sequence, followed by a highly dynamic domain protruding into the water phase. Additionally, transducer-transducer and transducer-receptor proximity relations revealed the overall architecture of the AS-1 sequences in the 2:2 complex, which are suggested to form a molten globular type of a coiled-coil bundle.     

Active state of sensory rhodopsin II: structural determinants for signal transfer and proton pumping

The molecular mechanism of transmembrane signal transduction is still a pertinent question in cellular biology. Generally, a receptor can transfer an external signal via its cytoplasmic surface, as found for G-protein-coupled receptors such as rhodopsin, or via the membrane domain, such as that in sensory rhodopsin II (SRII) in complex with its transducer, HtrII. In the absence of HtrII, SRII functions as a proton pump. Here, we report on the crystal structure of the active state of uncomplexed SRII from Natronomonas pharaonis, NpSRII. The problem with a dramatic loss of diffraction quality upon loading of the active state was overcome by growing better crystals and by reducing the occupancy of the state. The conformational changes in the region comprising helices F and G are similar to those observed for the NpSRII-transducer complex but are much more pronounced. The meaning of these differences for the understanding of proton pumping and signal transduction by NpSRII is discussed.     

Light-induced conformational changes in full-length Arabidopsis thaliana cryptochrome

Cryptochromes (CRYs) are widespread flavoproteins with homology to photolyases (PHRs), a class of blue-light-activated DNA repair enzymes. Unlike PHRs, both plant and animal CRYs have a C-terminal domain. This cryptochrome C-terminal (CCT) domain mediates interactions with other proteins, while the PHR-like domain converts light energy into a signal via reduction and radical formation of the flavin adenine dinucleotide cofactor. However, the mechanism by which the PHR-like domain regulates the CCT domain is not known. Here, we applied the pulsed-laser-induced transient grating method to detect conformational changes induced by blue-light excitation of full-length Arabidopsis thaliana cryptochrome 1 (AtCRY1). A significant reduction in the diffusion coefficient of AtCRY1 was observed upon photoexcitation, indicating that a large conformational change occurs in this monomeric protein. AtCRY1 containing a single mutation (W324F) that abolishes an intra-protein electron transfer cascade did not exhibit this conformational change. Moreover, the conformational change was much reduced in protein lacking the CCT domain. Thus, we conclude that the observed large conformational changes triggered by light excitation of the PHR-like domain result from C-terminal domain rearrangement. This inter-domain modulation would be critical for CRYs' ability to transduce a blue-light signal into altered protein-protein interactions for biological activity. Lastly, we demonstrate that the transient grating technique provides a powerful method for the direct observation and understanding of photoreceptor dynamics.     

Spectroscopic evidence for the formation of an N intermediate during the photocycle of sensory rhodopsin II (phoborhodopsin) from Natronobacterium pharaonis

Sensory rhodopsin II is a seven transmembrane helical retinal protein and functions as a photoreceptor protein in negative phototaxis of halophilic archaea. Sensory rhodopsin II from Natronomonas pharaonis (NpSRII) is stable under various conditions and can be expressed functionally in Escherichia coli cell membranes. Rhodopsins from microorganisms, known as microbial rhodopsins, exhibit a photocycle, and light irradiation of these molecules leads to a high-energy intermediate, which relaxes thermally to the original pigment after passing through several intermediates. For bacteriorhodopsin (BR), a light-driven proton pump, the photocycle is established as BR → K → L → M → N → O → BR. The photocycle of NpSRII is similar to that of BR except for N, i.e., M thermally decays into the O, and N has not been well characterized in the photocycle. Thus we here examined the second half of the photocycle in NpSRII, and in the present transient absorption study we found the formation of a new photointermediate whose absorption maximum is ～500 nm. This intermediate becomes pronounced in the presence of azide, which accelerates the decay of M. Transient resonance Raman spectroscopy was further applied to demonstrate that this intermediate contains a 13-cis retinal protonated Schiff base. However, detailed analysis of the transient absorption data indicated that M-decay does not directly produce N but rather produces O that is in equilibrium with N. These observations allowed us to propose a structural model for a photocycle that involves N.     

Light-induced conformational change and transient dissociation reaction of the BLUF photoreceptor Synechocystis PixD (Slr1694)

The light-induced reaction of the BLUF (blue light photoreceptor using flavin adenine dinucleotide) photoreceptor PixD from Synechocystis sp. PCC6803 (Slr1694) was investigated using the time-resolved transient grating method. A conformational change coupled with a volume contraction of 13 mL mol^− 1 was observed with a time constant of 45 ms following photoexcitation. At a weak excitation light intensity, there were no further changes in volume and diffusion coefficient (D). The determined D-value (3.7 × 10^− 11 m² s^− 1) suggests that PixD exists as a decamer in solution, and this oligomeric state was confirmed by size-exclusion chromatography and blue native polyacrylamide gel electrophoresis. Surprisingly, by increasing the excitation laser power, we observed a large increase in D with a time constant of 350 ms following the volume contraction reaction. The D-value of this photoproduct species (7.5 × 10^− 11 m² s^− 1) is close to that of the PixD dimer. Combined with transient grating and size-exclusion chromatography measurements under light-illuminated conditions, the light-induced increase in D was attributed to a transient dissociation reaction of the PixD decamer to a dimer. For the M93A-mutated PixD, no volume or D-change was observed. Furthermore, we showed that the M93A mutant did not form the decamer but only the dimer in the dark state. These results indicate that the formation of the decamer and the conformational change around the Met residue are important factors that control the regulation of the downstream signal transduction by the PixD photoreceptor.     

Structural analysis of the phototactic transducer protein HtrII linker region from Natronomonas pharaonis

Halobacterial pharaonis phoborhodopsin [ppR, also called Natronomonas pharaonis sensory rhodopsin II (NpSRII)] is a phototaxis protein which transmits a light signal to the cytoplasm through its transducer protein (pHtrII). pHtrII, a two-transmembrane protein that interacts with ppR, belongs to the group of methyl-accepting chemotaxis proteins (MCPs). Several mutation studies have indicated that the linker region connecting the transmembrane and methylation regions is necessary for signal transduction. However, the three-dimensional (3D) structure of an MCP linker region has yet to be reported, and hence, details concerning the signal transduction mechanism remain unknown. Here the structure of the pHtrII linker region was investigated biochemically and biophysically. Following limited proteolysis, only one trypsin resistant fragment in the pHtrII linker region was identified. This fragment forms a homodimer with a Kd value of 115 microM. The 3D structure of this fragment was determined by solution NMR, and only one alpha-helix was found between two HAMP domains of the linker region. This alpha-helix was significantly stabilized within transmembrane protein pHtrII as revealed by CW-EPR. The presence of Af1503 HAMP domain-like structures in the linker region was supported by CD, NMR, and ELDOR data. The alpha-helix determined here presumably works as a mechanical joint between two HAMP domains in the linker region to transfer the photoactivated conformational change downstream.     

A fluorescence stopped-flow study on troponin labeled with N-ethyl maleimide and N-(p-(2-benzimidazolyl)phenyl) maleimide

The kinetics of the conformational change of the troponin-C (TN-C) subunit in N-(p-(2-benzimidazolyl)phenyl) maleimide (BIPM)-N-ethyl maleimide (NEM)-labeled troponin induced by calcium binding or removal were studied with the fluorescence stopped-flow method. The kinetic process of the conformational change was biphasic, the rate constants of the two phases were determined as a function of the free calcium ion concentration of the protein solution. The kinetic behaviour of the conformational change of TN-C in BIPM-NEM-labeled troponin was explained by a simple molecular kinetic mechanism: (Formula: see text) This molecular kinetic mechanism is different from that of the isolated TN-C which we found in the previous work (1). That is, formation of a complex of TN-C with troponin-I (TN-I) and troponin-T (TN-T) modifies the molecular kinetic mechanism of the conformational change of TN-C.     

Dynamics of conformational changes of Arabidopsis phototropin 1 LOV2 with the linker domain

Conformational changes of Arabidopsis phot1-LOV2 with the linker (phot1-LOV2-linker) were investigated from the viewpoint of the changes in molecular volume and molecular diffusion coefficient (D) by time-resolved transient grating (TG) and transient lens (TrL) methods. Although the absorption spectrum change completes within a few microseconds, the D-value detected by the TG method decreased drastically with a time constant of 1.0 ms from 9.2(+/-0.4)x10(-11) m(2)/s to 5.0(+/-0.3)x10(-11) m(2)/s. This time-dependent D was interpreted in terms of the unfolding of alpha-helices in the linker region. The change of the alpha-helices was confirmed by observing the recovery of the circular dichroism intensity. The TrL signal showed that the molecular volume decreases with two time constants; 300 micros and 1.0 ms. The former time constant is close to the previously observed photo-dissociation reaction rate of the phot1-LOV2 (without the linker) dimer, and the latter one agrees well with the rate of the D-change. Considering a similar time constant of the dissociation reaction of the LOV2 dimer, we interpreted these kinetics in terms of the dissociation step of the linker region from the LOV2 domain (T(390)(pre) state). After this step, the protein volume and D are decreased significantly with the lifetime of 1.0 ms. The D decrease indicates the increase of the intermolecular interaction between the protein and water molecules. On the basis of these observations, a two-step mechanism of the linker unfolding is proposed.     

A spectrally silent transformation in the photolysis of octopus rhodopsin: a protein conformational change without any accompanying change of the chromophore's absorption

A spectrally silent transformation in the photolysis of octopus rhodopsin was detected by the time-resolved transient grating method. Our results showed that at least two photointermediates, which share the same chromophore absorption spectrum, exist after the final absorption changes. Previously, mesorhodopsin was thought to decay to the final photoproduct, acid metarhodopsin with a lifetime of 38 micros at 15 degrees C, but the present results show that there is at least one intermediate species (called transient acid metarhodopsin) with a lifetime of 180 micros at 15 degrees C, before forming acid metarhodopsin. This indicates that the parts of the protein distant from the chromophore are still changing even after the changes in microenvironment around the chromophore are over. From the signal intensity detected by the transient grating method, the volume change of the spectrally silent transformation was found to be DeltaV = 13 ml/mol. The activation energy of the spectrally silent transformation is much lower than those of other transformations of octopus rhodopsin. Since stable acid metarhodopsin has not been shown to activate the G protein, this transient acid metarhodopsin may be responsible for G protein activation.     

Structural dynamics of distal histidine replaced mutants of myoglobin accompanied with the photodissociation reaction of the ligand

Protein dynamics observed by the transient grating (TG) method are studied for some site-directed mutants at the distal histidine of myoglobin (H64L, H64Q, H64V). The time profiles of the TG signals are very sensitive to the amino acid residue of the 64 position. It was found that the sensitivity is mostly caused by the different rates of the ligand escape from the protein to solvent and the magnitude of the molecular volume change. Several molecular origins of the volume difference between MbCO and Mb, such as the electrostatic interaction in the distal pocket, movement of helices, and distal water, are proposed. Interestingly, the volume difference between the CO-trapped Mb inside the protein interior and Mb is similar to that of the partial molar volume of CO in organic solvent. The effect of mutation on the nature of the CO trapped site is discussed.     

The detection of human beta 2-microglobulin by grating coupler immunosensor with three dimensional antibody networks.

Immunosensors for the detection of human beta 2-microglobulin (B2M) were prepared by immobilisation of covalently crosslinked assemblies containing various numbers of molecular layers of monoclonal antibody against B2M (anti-B2M) on the surface of a Ta2O5 grating coupler sensor. The immobilisation procedure consisted of repeated successive adsorption of anti-B2M and dextran sulfate (DS) followed by glutaraldehyde (GA) crosslinking of anti-B2M and washing out DS. The flexibility of the resulting anti-B2M networks was evaluated from the sensor response to the reversible expansion and contraction of the networks induced by changing pH of the ambient solution. A decreased GA concentration and the use of a higher-molecular-mass DS increased the network flexibility. The sensor sensitivity to B2M increased with increasing flexibility of the antibody networks and with increasing number of anti-B2M molecular layers, indicating that B2M can penetrate inside the antibody network.