Photoreactions of aureochrome-1

Aureochrome is a recently discovered blue light photosensor that controls a light-dependent morphology change. As a photosensor, it has a unique DNA binding domain (bZIP). Although the biological functions of aureochrome have been revealed, the fundamental photochemistry of this protein has not been elucidated. The photochemical reaction dynamics of the LOV (light, oxygen, or voltage) domain of aureochrome-1 (AUREO1-LOV) and the LOV domain with the bZIP domain (AUREO1-ZL) were studied by employing the transient-grating (TG) technique, using size-exclusion chromatography to verify results. For both samples, adduct formation takes place with a time constant of 2.8 μs. Although significant diffusion changes were observed for both AUREO1-LOV and AUREO1-ZL after adduct formation, the origins of these changes were significantly different. The TG signal of AUREO1-LOV was strongly concentration-dependent. From analysis of the signal, it was concluded that AUREO1-LOV exists in equilibrium between the monomer and dimer, and dimerization of the monomer is the main reaction, i.e., irradiation with blue light enhances the strength of the interdomain interaction. On the other hand, the reaction of AUREO1-ZL is independent of concentration, suggesting that an intraprotein conformational change occurs in the bZIP domain with a time constant of 160 ms. These results revealed the different reactions and roles of the two domains; the LOV domain acts as a photosensor, leading to a subsequent conformational change in the bZIP domain, which should change its ability to bind to DNA. A model is proposed that demonstrates how aureochrome uses blue light to control its affinity for DNA.     

Role of Phe1010 in light-induced structural changes of the neo1-LOV2 domain of Adiantum

Phototropin (phot) is a blue-light sensor protein that elicits several photo responses in plants. Phototropin has two flavin mononucleotide (FMN)-binding domains, LOV1 and LOV2, in its N-terminal half. The C-terminal half is a blue-light-regulated Ser/Thr kinase. Various functional studies have reported that only LOV2 is responsible for the kinase activity, whereas the X-ray crystallographic structures of the LOV1 and LOV2 domains are almost identical. How does such a functional difference emerge? Our previous FTIR study of the LOV domains of Adiantum neochrome1 (neo1) showed that light-induced protein structural changes are small and temperature independent for neo1-LOV1, whereas the structural changes are large and highly temperature dependent for neo1-LOV2, which involve loops, alpha-helices, and beta-sheets. These observations successfully explained the different functions in terms of protein structural changes. They also suggested the presence of some crucial amino acids responsible for greater protein structural changes in the LOV2 domain. Here, we focused on phenylalanine-1010 (Phe1010) in neo1-LOV2, where FMN is sandwiched between Phe1010 and the reactive cysteine. Phenylalanine at this position is conserved for LOV2 domains, while the corresponding amino acid is leucine for LOV1 domains in almost all plant phototropins. We observed that unlike wild-type LOV2, the FTIR spectra of F1010L LOV2 exhibited no temperature dependence in the alpha-helical and beta-sheet regions and that spectral changes in amide-I of these regions were significantly reduced, which was similar to LOV1. Thus, the replacement of phenylalanine with leucine converts neo1-LOV2 into neo1-LOV1 in terms of protein structural changes that must be related to the different functions. We will discuss the roles of phenylalanine and leucine in the LOV2 and LOV1 domains, respectively.     

Photoactivation Reduces Side-Chain Dynamics of a LOV Photoreceptor

We used neutron-scattering experiments to probe the conformational dynamics of the light, oxygen, voltage (LOV) photoreceptor PpSB1-LOV from Pseudomonas putida in both the dark and light states. Global protein diffusion and internal macromolecular dynamics were measured using incoherent neutron time-of-flight and backscattering spectroscopy on the picosecond to nanosecond timescales. Global protein diffusion of PpSB1-LOV is not influenced by photoactivation. Observation-time-dependent global diffusion coefficients were found, which converge on the nanosecond timescale toward diffusion coefficients determined by dynamic light scattering. Mean-square displacements of localized internal motions and effective force constants, <k′>, describing the resilience of the proteins were determined on the respective timescales. Photoactivation significantly modifies the flexibility and the resilience of PpSB1-LOV. On the fast, picosecond timescale, small changes in the mean-square displacement and <k′> are observed, which are enhanced on the slower, nanosecond timescale. Photoactivation results in a slightly larger resilience of the photoreceptor on the fast, picosecond timescale, whereas in the nanosecond range, a significantly less resilient structure of the light-state protein is observed. For a residue-resolved interpretation of the experimental neutron-scattering data, we analyzed molecular dynamics simulations of the PpSB1-LOV X-ray structure. Based on these data, it is tempting to speculate that light-induced changes in the protein result in altered side-chain mobility mostly for residues on the protruding Jα helix and on the LOV-LOV dimer interface. Our results provide strong experimental evidence that side-chain dynamics play a crucial role in photoactivation and signaling of PpSB1-LOV via modulation of conformational entropy.     

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.     

Comparative investigation of the LOV1 and LOV2 domains in Adiantum phytochrome3

Phototropin (phot) is a blue-light photoreceptor for phototropic responses, relocation of chloroplasts, and stomata opening in plants. Phototropin has two chromophore-binding domains named LOV1 and LOV2 in its N-terminal half, each of which binds a flavin mononucleotide (FMN) noncovalently. The C-terminal half is a Ser/Thr kinase. A transgenic study of Arabidopsis suggested that only LOV2 domain is necessary for the kinase activity, whereas X-ray crystallographic structures of LOV1 and LOV2 domains are almost identical. These facts imply that the detailed structures and/or structural changes are different between LOV1 and LOV2 domains. In this study, we compared light-induced structural changes of the LOV1 and LOV2 domains of a phototropin, Adiantum phytochrome3 (phy3), by means of UV-visible and Fourier transform infrared (FTIR) spectroscopy. Photochemical properties of an adduct formation between FMN and a cysteine are essentially similar between phy3-LOV1 and phy3-LOV2. On the other hand, the S-H group of the reactive cysteine forms a hydrogen bond in phy3-LOV1, which is strengthened at low temperatures. This is possibly correlated with the fact that no adduct formation takes place for phy3-LOV1 at 77 K as revealed by the UV-visible absorption spectra. The most prominent difference was seen in the amide-I vibration that monitors the secondary structure of peptide backbone. Protein structural changes in phy3-LOV2 involve the regions of loops, alpha-helices, and beta-sheets, which differ significantly among various temperatures. Extended protein structural changes are probably correlated with the signal transduction activity of LOV2. In contrast, protein structural changes were very small in phy3-LOV1, and they were almost temperature independent. The photocycle of phy3-LOV1 takes 3.1 h, being more than 100 times longer than that of phy3-LOV2. These facts suggest that Adiantum phy3-LOV1 does not work for light sensing, being consistent with the previous transgenic study of Arabidopsis. It is likely that plants utilize a unique protein architecture (LOV domain) for different functions by regulating their protein structural changes.     

Quaternary structure of LOV-domain containing polypeptide of Arabidopsis FKF1 protein

Flavin-binding, Kelch repeat, F-box (FKF1) protein is a photoreceptor to regulate flowering of Arabidopsis. The protein has a light, oxygen and voltage (LOV)-sensing domain binding a flavin mononucleotide. The photo-activation of the domain is an indispensable step to initiate the cellular signaling for flowering. In the present study, a LOV-containing polypeptide of FKF1 was prepared by an overexpression system, and the quaternary structure of it was studied by size exclusion chromatography and small-angle X-ray scattering. The apparent molecular weight from chromatography suggested a globular trimeric or an anisotropic-shaped dimeric association of the polypeptide in solution. The scattering experiment demonstrated a dimeric association of the polypeptides with an elongated molecular shape displaying the radius of gyration of 27 A and the maximum dimension of 94 A. The molecular shape simulated from scattering profiles suggests an antiparallel association of the LOV domains in the dimer. Though the absorption spectrum of blue-light irradiated polypeptide was stable in the photoactivated state for a long period, the scattering profiles showed very small changes between the dark and light conditions. Based on the homologies in the amino-acid sequences and the scattering profiles, these results are discussed in connection with the structures and function of LOV domains of phototropin.     

Structural basis of the LOV1 dimerization of Arabidopsis phototropins 1 and 2

Phototropin (phot) is a blue-light receptor protein that triggers phototropic responses, chloroplast relocation, and stomata opening to maximize the efficiency of photosynthesis in higher plants. Phot is composed of three functional domains. The N-terminal half folds into two light-oxygen-voltage-sensing domains called LOV1 and LOV2, each binding a flavin mononucleotide to absorb blue light. The C-terminal half is a serine/threonine kinase domain that causes light-dependent autophosphorylation leading to cellular signaling cascades. LOV2 domain is primarily responsible for activation of the kinase, and LOV1 domain is thought to act as a dimerization site and to regulate sensitivity to activation by blue light. Here we show the crystal structures of LOV1 domains of Arabidopsis phot1 and phot2 in the dark at resolutions of 2.1 Å and 2.0 Å, respectively. Either LOV1 domain forms a dimer through face-to-face association of β-scaffolds in the crystallographic asymmetric unit. Three types of interactions stabilizing the dimer structures found are as follows: contacts of side chains in their β-scaffolds, hydrophobic interactions of a short helix found in the N-terminus of a subunit with the β-scaffolds of both subunits, and hydrogen bonds mediated by hydration water molecules filling the dimer interface. The critical residues for dimerization are Cys261, forming a disulfide bridge between subunits in phot1-LOV1 domain, and Thr217 and Met232 in phot2-LOV1. The topology in homodimeric associations of the LOV1 domains is discussed when referring to those of homodimers or heterodimers of light-oxygen-voltage-sensing or Per-ARNT-Sim domains. The present results also provide clues to understanding structural basis in dimeric interactions of Per-ARNT-Sim protein modules in cellular signaling.     

Structural basis for the slow dark recovery of a full-length LOV protein from Pseudomonas putida

Blue-light photoreceptors containing light–oxygen–voltage (LOV) domains regulate a myriad of different physiological responses in both eukaryotes and prokaryotes. Their light sensitivity is intricately linked to the photochemistry of the non-covalently bound flavin mononucleotide (FMN) chromophore that forms a covalent adduct with a conserved cysteine residue in the LOV domain upon illumination with blue light. All LOV domains undergo the same primary photochemistry leading to adduct formation; however, considerable variation is found in the lifetime of the adduct state that varies from seconds to several hours. The molecular mechanism underlying this variation among the structurally conserved LOV protein family is not well understood. Here, we describe the structural characterization of PpSB1-LOV, a very slow cycling full-length LOV protein from the Gram-negative bacterium Pseudomonas putida KT2440. Its crystal structure reveals a novel dimer interface that is mediated by N- and C-terminal auxiliary structural elements and a unique cluster of four arginine residues coordinating with the FMN-phosphate moiety. Site-directed mutagenesis of two arginines (R61 and R66) in PpSB1-LOV resulted in acceleration of the dark recovery reaction approximately by a factor of 280. The presented structural and biochemical data suggest a direct link between structural features and the slow dark recovery observed for PpSB1-LOV. The overall structural arrangement of PpSB1-LOV, together with a complementary phylogenetic analysis, highlights a common ancestry of bacterial LOV photoreceptors and Per-ARNT-Sim chemosensors.     

Higher plants use LOV to perceive blue light

Higher plants use several classes of blue light receptors to modulate a wide variety of physiological responses. Among them, both the phototropins and members of the Zeitlupe (ZTL) family use light oxygen voltage (LOV) photosensory domains. In Arabidopsis, these families comprise phot1, phot2 and ZTL, LOV Kelch Protein 2 (LKP2), and Flavin-binding Kelch F-box1 (FKF1). It has now been convincingly shown that blue-light-induced autophosphorylation of the phot1 kinase domain is an essential step in signal transduction. Recent experiments also shed light on the partially distinct photosensory specificities of phot1 and phot2. Phototropin signaling branches rapidly following photoreceptor activation to mediate distinct responses such as chloroplast movements or phototropism. Light activation of the LOV domain in ZTL family members modulates their capacity to interact with GIGANTEA (GI) and their ubiquitin E3 ligase activity. A complex between GI and FKF1 is required to trigger the degradation of a repressor of CO (CONSTANS) expression and thus modulates flowering time. In contrast, light-regulated complex formation between ZTL and GI appears to limit the capacity of ZTL to degrade its targets, which are part of the circadian oscillator.     

Photoreaction cycle of the light, oxygen, and voltage domain in FKF1 determined by low-temperature absorption spectroscopy

Flavin-binding Kelch repeat F-box (FKF1) protein plays important roles in the photoregulation of flowering in Arabidopsis. FKF1 has a light, oxygen, and voltage (LOV) sensing domain binding a flavin mononucleotide (FMN) as a chromophore noncovalently. Photoreaction of the FKF1-LOV polypeptide was studied by low-temperature absorption spectroscopy. Upon blue light irradiation, a ground state, D(450), is converted to S(390) known as a cysteinyl-flavin adduct intermediate in the photoreaction of phototropin. Below 150 K, bleaching of D(450) was much reduced and a new photoproduct, Z(370), appeared as well as S(390) formation. The calculated absorption spectrum for Z(370) is very similar to those of flavoproteins in an anion radical state. On the basis of the results that S(390) formation proceeds to Z(370) formation and that Z(370) formed at low temperatures reverts to D(450) upon temperature increase, Z(370) is concluded to be not an intermediate from D(450) to S(390). Z(370) is suggested to be formed from the biradical triplet-excited state after relaxing to the ground state with the FMN anion radical trapped at the low temperature, in which the SH of the cysteine is in the wrong position that is able to produce a radical pair but unable to form the cysteinyl-flavin adduct. The counter SH in the cationic radical state may revert to the ground state by extracting an electron from the unidentified amino acid residue. Interestingly, S(390) that has been thought to be irreversible to D(450) was revealed to revert to D(450) very slowly with a half-life time of 62.5 h in solution at 298 K. The photoreaction mechanism is discussed in reference to the calculated activation energy of the reaction processes.     

LOV KELCH PROTEIN2 and ZEITLUPE repress Arabidopsis photoperiodic flowering under non-inductive conditions, dependent on FLAVIN-BINDING KELCH REPEAT F-BOX1

LOV KELCH PROTEIN2 (LKP2), ZEITLUPE (ZTL)/LOV KELCH PROTEIN1 (LKP1) and FLAVIN‐BINDING KELCH REPEAT F‐BOX1 (FKF1) constitute a family of Arabidopsis F‐box proteins that regulate the circadian clock. Over‐expression of LKP2 or ZTL causes arrhythmicity of multiple clock outputs under constant light and in constant darkness. Here, we show the significance of LKP2 and ZTL in the photoperiodic control of flowering time in Arabidopsis. In plants over‐expressing LKP2, CO and FT expression was down‐regulated under long‐day conditions. LKP2 and ZTL physically interacted with FKF1, which was recruited from the nucleus into cytosolic speckles. LKP2 and ZTL inhibited the interaction of FKF1 with CYCLING DOF FACTOR 1, a ubiquitination substrate for FKF1 that is localized in the nucleus. The Kelch repeat regions of LKP2 and ZTL were sufficient for their physical interaction with FKF1 and translocation of FKF1 to the cytoplasm. Over‐expression of LKP2 Kelch repeats induced late flowering under long‐day conditions. lkp2 ztl double mutant plants flowered earlier than wild‐type plants under short‐day (non‐inductive) conditions, and both CO and FT expression levels were up‐regulated in the double mutant plants. The early flowering of lkp2 ztl was dependent on FKF1. LKP2, ZTL or both affected the accumulation of FKF1 protein during the early light period. These results indicate that an important role of LKP2 and ZTL in the photoperiodic pathway is repression of flowering under non‐inductive conditions, and this is dependent on FKF1.     

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.     

Identification of the C=O stretching vibrations of FMN and peptide backbone by 13C-labeling of the LOV2 domain of Adiantum phytochrome3

Phototropin, a blue-light photoreceptor in plants, has two FMN-binding domains named LOV1 and LOV2. We previously observed temperature-dependent FTIR spectral changes in the C=O stretching region (amide-I vibrational region of the peptide backbone) for the LOV2 domain of Adiantum phytochrome3 (phy3-LOV2), suggesting progressive structural changes in the protein moiety (Iwata, T., Nozaki, D., Tokutomi, S., Kagawa, T., Wada, M., and Kandori, H. (2003) Biochemistry 42, 8183-8191). Because FMN also possesses two C=O groups, in this article, we aimed at assigning C=O stretching vibrations of the FMN and protein by using 13C-labeling. We assigned the C(4)=O and C(2)=O stretching vibrations of FMN by using [4,10a-13C2] and [2-13C] FMNs, respectively, whereas C=O stretching vibrations of amide-I were assigned by using 13C-labeling of protein. We found that both C(4)=O and C(2)=O stretching vibrations shift to higher frequencies upon the formation of S390 at 77-295 K, suggesting that the hydrogen bonds of the C=O groups are weakened by adduct formation. Adduct formation presumably relocates the FMN chromophore apart from its hydrogen-bonding donors. Temperature-dependent amide-I bands are unequivocally assigned by separating the chromophore bands. The hydrogen bond of the peptide backbone in the loop region is weakened upon S390 formation at low temperatures, while being strengthened at room temperature. The hydrogen bond of the peptide backbone in the alpha-helix is weakened regardless of temperature. On the other hand, structural perturbation of the beta-sheet is observed only at room temperature, where the hydrogen bond is strengthened. Light-signal transduction by phy3-LOV2 must be achieved by the progressive protein structural changes initiated by the adduct formation of the FMN.     

Hydration and temperature similarly affect light-induced protein structural changes in the chromophoric domain of phototropin

Phototropin is a blue-light sensor protein in plants, and LOV domain binds a flavin mononucleotide (FMN) as a chromophore. A photointermediate state, S390, is formed by light-induced adduct formation between FMN and an S-H group of nearby cysteine, which triggers protein structural changes for kinase activation in phototropin. We previously studied the low-temperature Fourier transform infrared (FTIR) spectra between the S390 and unphotolyzed states for a LOV2 domain of a phototropin from Adiantum (neo1-LOV2), and found that the protein structures of the S390 intermediate are highly temperature dependent (Iwata, T., Nozaki, D., Tokutomi, S., Kagawa, T., Wada, M., and Kandori, H. (2003) Biochemistry 42, 8183-8191). At physiological temperature, amide-I vibration at 1640-1620 cm-1 is significantly changed, implying structural alteration of beta-sheet region. Such changes are largely suppressed at low temperatures, though S390 is formed. This observation suggested the presence of progressive protein structural changes in the unique active state (S390). Here we report that the hydration dependence of the amide-I vibrational bands in neo1-LOV2 is similar to the temperature dependence. As hydration of the sample is lowered, amide-I vibration at 1640-1620 cm-1 is significantly reduced. Instead, amide-I vibration at 1694 cm-1 newly emerged at low hydration as well as at low temperature, which shows a weakened hydrogen bond in the loop region. Spectral coincidence between low hydrations and temperatures strongly suggested that protein structural changes are similarly restricted under such conditions. It is likely that protein fluctuations are prerequisite for formation of the active state of neo1-LOV2.     

Oligomeric structure of LOV domains in Arabidopsis phototropin

Oligomeric structures of the four LOV domains in Arabidopsis phototropin1 (phot1) and 2 (phot2) were studied using crosslinking. Both LOV1 domains of phot1 and phot2 form a dimer independently on the light conditions, suggesting that the LOV1 domain can be a stable dimerization site of phot in vivo. In contrast, phot1-LOV2 is in a monomer-dimer equilibrium and phot2-LOV2 exists as a monomer in the dark. Blue light-induced a slight increase in the monomer population in phot1-LOV2, suggesting a possible blue light-inducible dissociation of dimers. Furthermore, blue light caused a band shift of the phot2-LOV2 monomer. CD spectra revealed the unfolding of helices and the formation of strand structures. Both light-induced changes were reversible in the dark.

Structured summary

MINT-6823377, MINT-6823391:PHOT1 (uniprotkb:O48963) and PHOT1 (uniprotkb: O48963) bind (MI:0407) by cross-linking studies (MI:0030)MINT-6823495, MINT-6823508:PHOT2 (uniprotkb:P93025) and PHOT2 (uniprotkb:P93025) bind (MI:0407) by cross-linking studies (MI:0030)     

LOV domain-containing F-box proteins: light-dependent protein degradation modules in Arabidopsis

Plants constantly survey the surrounding environment using several sets of photoreceptors. They can sense changes in the quantity (=intensity) and quality (=wavelength) of light and use this information to adjust their physiological responses, growth, and developmental patterns. In addition to the classical photoreceptors, such as phytochromes, cryptochromes, and phototropins, ZEITLUPE (ZTL), FLAVIN-BINDING, KELCH REPEAT, F-BOX 1 (FKF1), and LOV KELCH PROTEIN 2 (LKP2) proteins have been recently identified as blue-light photoreceptors that are important for regulation of the circadian clock and photoperiodic flowering. The ZTL/FKF1/LKP2 protein family possesses a unique combination of domains: a blue-light-absorbing LOV (Light, Oxygen, or Voltage) domain along with domains involved in protein degradation. Here, we summarize recent advances in our understanding of the function of the Arabidopsis ZTL/FKF1/LKP2 proteins. We summarize the distinct photochemical properties of their LOV domains and discuss the molecular mechanisms by which the ZTL/FKF1/LKP2 proteins regulate the circadian clock and photoperiodic flowering by controlling blue-light-dependent protein degradation.     

Kinetic measurement of transient dimerization and dissociation reactions of Arabidopsis phototropin 1 LOV2 domain

Photochemical reaction of a plant blue-light photoreceptor, Arabidopsis phototropin 1-LOV (light-oxygen-voltage sensing) domain 2, was studied with a view to the diffusion coefficients (D) using the pulsed-laser-induced transient grating method. Although the reaction dynamics completes at a rate of several microseconds as long as it is monitored by the absorption change, the diffusion coefficient was found to be time-dependent in a time range of submilliseconds to seconds. The observed signal can be analyzed by the two-state model, which includes the D-value decrease from D of the reactant (9.8 +/- 0.4) x 10(-11) m2/s to D of the product (8.0 +/- 0.4) x 10(-11) m2/s. The D-value of the reactant implies that the dominant form in the ground state of phototropin 1 LOV2 is the monomeric form in a concentration range of 50-200 microM. According to the Stokes-Einstein relationship, the D-change can be explained by a volume increase of 1.8 times. Furthermore, the rate of the D-change was roughly proportional to the concentration of the sample. These two observations indicate that the LOV2 domain transiently forms a dimer upon photoexcitation. When the sample concentration is increased (>180 microM), a new signal component appears within a few milliseconds. This signal represents a D increase from 8.0 x 10(-11) m2/s to 9.8 x 10(-11) m2/s with a time constant of 300 micros. The completely opposite D-change from that observed in a lower concentration, as well as the concentration dependence, implies that a dimer is formed in the ground state in a higher concentration range, even though the fraction of the dimer is still minor in this range. This dimer is photodissociated, with a time constant of 300 micros. This research clearly shows that the time-resolved diffusion measurement is a very powerful tool for detecting spectrally silent association/dissociation processes during chemical reactions. The photoreaction of the LOV2 domain is discussed.     

FMN Binding and Photochemical Properties of Plant Putative Photoreceptors Containing Two LOV Domains,LOV/LOV Proteins

LOV domains function as blue light-sensing modules in various photoreceptors in plants, fungi, algae, and bacteria. A LOV/LOV protein (LLP) has been found from Arabidopsis thaliana (AtLLP) as a two LOV domain-containing protein. However, its function remains unknown. We isolated cDNA clones coding for an LLP homolog from tomato (Solanum lycopersicum) and two homologs from the moss Physcomitrella patens. The tomato LLP (SlLLP) contains two LOV domains (LOV1 and LOV2 domains), as in AtLLP. Most of the amino acids required for association with chromophore are conserved in both LOV domains, except that the amino acid at the position equivalent to the cysteine essential for cysteinyl adduct formation is glycine in the LOV1 domain as in AtLLP. When expressed in Escherichia coli, SlLLP binds FMN and undergoes a self-contained photocycle upon irradiation of blue light. Analyses using mutant SlLLPs revealed that SlLLP binds FMN in both LOV domains, although the LOV1 domain does not show spectral changes on irradiation. However, when Gly⁶⁶ in the LOV1 domain, which is located at the position equivalent to the essential cysteine of LOV domains, is replaced by cysteine, the mutated LOV1 domain shows light-induced spectral changes. In addition, all four LOV domains of P. patens LLPs (PpLLP1 and PpLLP2) show the typical features of LOV domains, including the reactive cysteine in each. This study shows that plants have a new LOV domain-containing protein family with the typical biochemical and photochemical properties of other LOV domain-containing proteins such as the phototropins.     

Time-Resolved Fourier Transform Infrared Study on Photoadduct Formation and Secondary Structural Changes within the Phototropin LOV Domain

Phototropins are plant blue-light photoreceptors containing two light-, oxygen-, or voltage-sensitive (LOV) domains and a C-terminal kinase domain. The two LOV domains bind noncovalently flavin mononucleotide as a chromophore. We investigated the photocycle of fast-recovery mutant LOV2-I403V from Arabidopsis phototropin 2 by step-scan Fourier transform infrared spectroscopy. The reaction of the triplet excited state of flavin with cysteine takes place with a time constant of 3 μs to yield the covalent adduct. Our data provide evidence that the flavin is unprotonated in the productive triplet state, disfavoring an ionic mechanism of bond formation. An intermediate adduct species was evident that displayed changes in secondary structure in the helix or loop region, and relaxed with a time constant of 120 μs. In milliseconds, the final adduct state is formed by further alterations of secondary structure, including β-sheets. A comparison with wild-type adduct spectra shows that the mutation does not interfere with the functionality of the domain. All signals originate from within the LOV domain, because the construct does not comprise the adjacent Jα helix required for signal transduction. The contribution of early and late adduct intermediates to signal transfer to the Jα helix outside of the domain is discussed.     

Ordering of C-terminal loop and glutaminase domains of glucosamine-6-phosphate synthase promotes sugar ring opening and formation of the ammonia channel

Glucosamine-6-phosphate synthase (GlmS) channels ammonia from glutamine at the glutaminase site to fructose 6-phosphate (Fru6P) at the synthase site. Escherichia coli GlmS is composed of two C-terminal synthase domains that form the dimer interface and two N-terminal glutaminase domains at its periphery. We report the crystal structures of GlmS alone and in complex with the glucosamine-6-phosphate product at 2.95 Å and 2.9 Å resolution, respectively. Surprisingly, although the whole protein is present in this crystal form, no electron density for the glutaminase domain was observed, indicating its mobility. Comparison of the two structures with that of the previously reported GlmS-Fru6P complex shows that, upon sugar binding, the C-terminal loop, which forms the major part of the channel walls, becomes ordered and covers the synthase site. The ordering of the glutaminase domains likely follows Fru6P binding by the anchoring of Trp74, which acts as the gate of the channel, on the closed C-terminal loop. This is accompanied by a major conformational change of the side chain of Lys503^# of the neighboring synthase domain that strengthens the interactions of the synthase domain with the C-terminal loop and completely shields the synthase site. The concomitant conformational change of the Lys503^#-Gly505^# tripeptide places catalytic His504^# in the proper position to open the sugar and buries the linear sugar, which is now in the vicinity of the catalytic groups involved in the sugar isomerization reaction. Together with the previously reported structures of GlmS in complex with Fru6P or glucose 6-phosphate and a glutamine analogue, the new structures reveal the structural changes occurring during the whole catalytic cycle.