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.     

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.     

Light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 studied by low-temperature FTIR and UV-visible spectroscopy

Phototropin (Phot) is a blue-light receptor in plants. The molecule has two FMN (flavin mononucleotide) binding domains named LOV (light-, oxygen-, and voltage-sensing), which is a subset of the PAS (Per-Arnt-Sim) superfamily. Illumination of the phot-LOV domains in the dark state (D447) produces a covalent C(4a) flavin-cysteinyl adduct (S390) via a triplet excited state (L660), which reverts to D447 in the dark. In this work, we studied the light-induced structural changes in the LOV2 domain of Adiantum phytochrome3 (phy3), which is a fusion protein of phot containing the phytochrome chromophoric domain, by low-temperature UV-visible and FTIR spectroscopy. UV-visible spectroscopy detected only one intermediate state, S390, in the temperature range from 77 to 295 K, indicating that the adduct is produced even at temperatures as low as 77 K, although a portion of D447 cannot be converted to S390 at low temperatures possibly because of motional freezing. In the whole temperature range, FTIR spectra in the S-H stretching frequency region showed that Cys966 of phy3-LOV2 is protonated in D447 and unprotonated on illumination, supporting adduct formation. The pK(a) of the S-H group in D447 is estimated to be >10. FTIR spectra also showed the light-induced appearance of a positive peak around 3621 cm(-1) in the whole temperature range, indicating that adduct formation accompanies rearrangement of a hydrogen bond of a water molecule(s), which can be either water25, water45, or both, near the chromophore. In contrast to the weak temperature dependence of the spectral changes in the UV-visible absorption and the FTIR of both S-H and O-H stretching bands, light-induced changes in the amide I vibration that probes protein backbone structure vary significantly with the increase in temperature. The spectral changes suggest that light excitation of FMN loosens the local structure around it, particularly in turns, in the early stages and that another change subsequently takes place to tighten it, mainly in beta-structure, but some occur in the alpha-helical structure of the protein moiety as well. Interestingly, these changes proceed without altering the shape of UV-visible spectra, suggesting the presence of multiple conformation states in S390.     

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.     

Vibrational spectroscopy of an algal Phot-LOV1 domain probes the molecular changes associated with blue-light reception

The LOV1 domain of the blue light Phot1-receptor (phototropin homolog) from Chlamydomonas reinhardtii has been studied by vibrational spectroscopy. The FMN modes of the dark state of LOV1 were identified by preresonance Raman spectroscopy and assigned to molecular vibrations. By comparing the blue-light-induced FTIR difference spectrum with the preresonance Raman spectrum, most of the differences are due to FMN modes. Thus, we exclude large backbone changes of the protein that might occur during the phototransformation of the dark state LOV1-447 into the putative signaling state LOV1-390. Still, the presence of smaller amide difference bands cannot be excluded but may be masked by overlapping FMN modes. The band at 2567 cm(-1) is assigned to the S-H stretching vibration of C57, the residue that forms the transient thio-adduct with the chromophore FMN. The occurrence of this band is evidence that C57 is protonated in the dark state of LOV1. This result challenges conclusions from the homologous LOV2 domain from oat that the thiolate of the corresponding cysteine is the reactive species.     

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.     

Primary reactions of the LOV2 domain of phototropin,a plant blue-light photoreceptor

The phototropins constitute an important class of plant photoreceptor kinases that control a range of physiological responses, including phototropism, light-directed chloroplast movement, and light-induced stomatal opening. The LOV2 domain of phototropin binds a molecule of flavin mononucleotide (FMN) and undergoes a photocycle involving light-driven covalent adduct formation between a conserved cysteine residue and the C(4a) atom of FMN. This product state promotes C-terminal kinase activation and downstream signal transduction. Here, we report the primary photophysics and photochemistry of LOV2 domains of phototropin 1 of Avena sativa (oat) and of the phy3 photoreceptor of Adiantum capillus-veneris (maidenhair fern). In agreement with earlier reports [Swartz, T. E., et al. (2001) J. Biol. Chem. 276, 36493-36500], we find that the FMN triplet state is the reactive species from which the photoreaction occurs. We demonstrate that the triplet state is the primary photoproduct in the LOV2 photocycle, generated at 60% efficiency. No spectroscopically distinguishable intermediates precede the FMN triplet on the femtosecond to nanosecond time scale, indicating that it is formed directly via intersystem crossing (ISC) from the singlet state. Our results indicate that the majority of the FMN triplets in the LOV2 domain exist in the protonated form. We propose a reaction mechanism that involves excited-state proton transfer, on the nanosecond time scale or faster, from the sulfhydryl group of the conserved cysteine to the N5 atom of FMN. This event promotes adduct formation by increasing the electrophilicity of C(4a) and subsequent nucleophilic attack by the cysteine's thiolate anion. Comparison to free FMN in solution shows that the protein environment of LOV2 increases the ISC rate of FMN by a factor of 2.4, thus improving the yield of the cysteinyl-flavin adduct and the efficiency of phototropin-mediated signaling processes.     

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.     

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.     

A LOV story: the signaling state of the phot1 LOV2 photocycle involves chromophore-triggered protein structure relaxation, as probed by far-UV time-resolved optical rotatory dispersion spectroscopy

Light-, oxygen-, or voltage-regulated (LOV1 and LOV2) domains bind flavin mononucleotide (FMN) and activate the phototropism photoreceptors phototropin 1 (phot1) and phototropin 2 (phot2) by using energy from absorbed blue light. Upon absorption of blue light, chromophore and protein conformational changes trigger the kinase domain for subsequent autophosphorylation and presumed downstream signal transduction. To date, the light-induced photocycle of the phot1 LOV2 protein is known to involve formation of a triplet flavin mononucleotide (FMN) chromophore followed by the appearance of a FMN adduct within 4 micros [Swartz, T. E., Corchnoy, S. B., Christie, J. M., Lewis, J. W., Szundi, I., Briggs, W. R., and Bogomolni, R. A. (2001) J. Biol. Chem. 276, 36493-36500] before thermal decay back to the dark state. To probe the mechanism by which the blue light information is relayed from the chromophore to the protein, nanosecond time-resolved optical rotatory dispersion (TRORD) spectroscopy, which is a direct probe of global secondary structure, was used to study the phot1 LOV2 protein in the far-UV region. These TRORD experiments reveal a previously unobserved intermediate species (tau approximately 90 micros) that is characterized by a FMN adduct chromophore and partially unfolded secondary structure (LOV390(S2)). This intermediate appears shortly after the formation of the FMN adduct. For LOV2, formation of a long-lived species that is ready to interact with a receptor domain for downstream signaling is much faster by comparison with formation of a similar species in other light-sensing proteins.     

A base-catalyzed mechanism for dark state recovery in the Avena sativa phototropin-1 LOV2 domain

Phototropins are autophosphorylating serine/threonine kinases responsible for blue-light perception in plants; their action gives rise to phototropism, chloroplast relocation, and opening of stomatal guard cells. The kinase domain constitutes the C-terminal part of Avena sativa phototropin 1. The N-terminal part contains two light, oxygen, or voltage (LOV) sensing domains, LOV1 and LOV2; each binds a flavin mononucleotide (FMN) chromophore (lambdamax = 447 nm, termed D447) and forms the light-sensitive domains, of which LOV2 is the principal component. Blue-light absorption produces a covalent adduct between a very conserved nearby cysteine residue and the C(4a) atom of the FMN moiety via the triplet state of the flavin. The covalent adduct thermally decays to regenerate the D447 dark state, with a rate that may vary by several orders of magnitude between different species. We report that the imidazole base can act as a very efficient enhancer of the dark recovery of A. sativa phot1 LOV2 (AsLOV2) and some other well-characterized LOV domains. Imidazole accelerates the thermal decay of AsLOV2 by 3 orders of magnitude in the submolar concentration range, via a base-catalyzed mechanism involving base abstraction of the FMN N(5)-H adduct state and subsequent reprotonation of the reactive cysteine. The LOV2 crystal structure suggests that the imidazole molecules may act from a cavity located in the vicinity of the FMN, explaining its high efficiency, populated through a channel connecting the cavity to the protein surface. Use of pH titration and chemical inactivation by diethyl pyrocarbonate (DEPC) suggests that histidines located at the surface of the LOV domain act as base catalysts via an as yet unidentified H-bond network, operating at a rate of (55 s)-1 at pH 8. In addition, molecular processes other than histidine-mediated base catalysis contibute significantly to the total thermal decay rate of the adduct and operate at a rate constant of (65 s)-1, leading to a net adduct decay time constant of 30 s at pH 8.     

Photochemical and mutational analysis of the FMN-binding domains of the plant blue light receptor, phototropin

The plant photoreceptor phototropin is an autophosphorylating serine-threonine protein kinase activated by UV-A/blue light. Two domains, LOV1 and LOV2, members of the PAS domain superfamily, mediate light sensing by phototropin. Heterologous expression studies have shown that both domains function as FMN-binding sites. Although three plant blue light photoreceptors, cry1, cry2, and phototropin, have been identified to date, the photochemical reactions underlying photoactivation of these light sensors have not been described so far. Herein, we demonstrate that the LOV domains of Avena sativa phototropin undergo a self-contained photocycle characterized by a loss of blue light absorbance in response to light and a spontaneous recovery of the blue light-absorbing form in the dark. Rate constants and quantum efficiencies for the photoreactions indicate that LOV1 exhibits a lower photosensitivity than LOV2. The spectral properties of the photoproduct produced for both LOV domains are unrelated to those found for photoreduced flavins and flavoproteins, but are consistent with those of a flavin-cysteinyl adduct. Flavin-thiol adducts are generally short-lifetime reaction intermediates formed during the flavoprotein-catalyzed reduction of protein disulfides. By site-directed mutagenesis, we have identified several amino acid residues within the putative chromophore binding site of LOV1 and LOV2 that appear to be important for FMN binding and/or the photochemical reactivity. Among those is Cys39, which plays an important role in the photochemical reaction of the LOV domains. Replacement of Cys39 with Ala abolished the photochemical reactions of both LOV domains. We therefore propose that light sensing by the phototropin LOV domains occurs via the formation of a stable adduct between the FMN chromophore and Cys39.     

Phototropin LOV domains exhibit distinct roles in regulating photoreceptor function

Phototropins (phot1 and phot2) are autophosphorylating serine/threonine kinases that function as photoreceptors for phototropism, light-induced chloroplast movement, and stomatal opening in Arabidopsis. The N-terminal region of phot1 and phot2 contains two specialized PAS domains, designated LOV1 and LOV2, which function as binding sites for the chromophore flavin mononucleotide (FMN). Both LOV1 and LOV2 undergo a self-contained photocycle, which involves the formation of a covalent adduct between the FMN chromophore and a conserved active-site cysteine residue (Cys39). Replacement of Cys39 with alanine abolishes the light-induced photochemical reaction of LOV1 and LOV2. Here we have used the Cys39Ala mutation to investigate the role of LOV1 and LOV2 in regulating phototropin function. Photochemical analysis of a bacterially expressed LOV1 + LOV2 fusion protein indicates that LOV2 functions as the predominant light-sensing domain for phot1. LOV2 also plays a major role in mediating light-dependent autophosphorylation of full-length phot1 expressed in insect cells and transgenic Arabidopsis. Moreover, photochemically active LOV2 alone in full-length phot1 is sufficient to elicit hypocotyl phototropism in transgenic Arabidopsis, whereas photochemically active LOV1 alone is not. Further photochemical and biochemical analyses also indicate that the LOV1 and LOV2 domains of phot2 exhibit distinct roles. The significance for the different roles of the phototropin LOV domains is discussed.     

Distinct cysteine sulfhydryl environments detected by analysis of Raman S-hh markers of Cys-->Ser mutant proteins

Very little is known about the character or functional relevance of hydrogen-bonded cysteine sulfhydryl (S-H) groups in proteins. The Raman S-H band is a unique and sensitive probe of the local S-H environment. Here, we report the use of Raman spectroscopy combined with site-specific mutagenesis to document the existence of five distinguishable hydrogen-bonded states of buried cysteine sulfhydryl groups in a native protein. The 666 residue subunit of the Salmonella typhimurium bacteriophage P22 tailspike contains eight cysteine residues distributed through the elongated structure. The tailspike cysteine residues display an unusual Raman S-H band complex (2500-2600 cm(-1) interval) indicative of diverse S-H hydrogen-bonding interactions in the native trimeric structure. To resolve specific Cys contributions to the complex Raman band we characterized a set of tailspike proteins with each cysteine replaced by a serine. The mutant proteins, once folded, were structurally and functionally indistinguishable from wild-type tailspikes, except for their Raman S-H signatures. Comparison of the Raman spectra of the mutant and wild-type proteins reveals the following hydrogen-bond classes for cysteine sulfhydryl groups. (i) Cys613 forms the strongest S-H...X bond of the tailspike, stronger than any heretofore observed for a protein. (ii) Cys267, Cys287 and Cys458 form robust S-H...X bonds. (iii) Moderate S-H...X bonding occurs for Cys169 and Cys635. (iv) Cys290 and Cys496 form weak hydrogen bonds. (v) It is remarkable that Cys287 contributes two Raman S-H markers, indicating the population of two distinct hydrogen-bonding states. The sum of the S-H Raman signatures of all eight mutants accurately reproduces the composite Raman band of the wild-type tailspike. The diverse cysteine states may be an outcome of the folding and assembly pathway of the tailspike, which though lacking disulfide bonds in the native state, utilizes transient disulfide bonds in the maturation pathway. This Raman study represents the first detailed assessment of local S-H hydrogen bonding in a native protein and provides information not obtainable directly by other structural probes. The method employed here should be applicable to a wide range of cysteine-containing proteins.     

Role of Gln1029 in the photoactivation processes of the LOV2 domain in adiantum phytochrome3

Phototropin (phot) is a blue-light receptor in plants. The molecule has two FMN (flavin mononucleotide)-binding domains named the LOV (light-oxygen-voltage) domain, that is a subset of a PAS (per-arnt-sim) superfamily. Illumination of phot-LOV domains produces a covalent C(4a) flavin-cysteinyl adduct, which is called the S390 intermediate state. According to the crystal structures of the LOV2 domain of Adiantum phytochrome3 (phy3), a fusion protein of phot containing the phytochrome chromophoric domain, in the unphotolyzed and S390 states, and the side chain of Gln1029 switches hydrogen bonds with the FMN chromophore. Gln1029 is the hydrogen-bonding donor of the C(4)=O group of FMN in the unphotolyzed state, whereas Gln1029 is the hydrogen-bonding acceptor of the N(5)-H group of FMN in S390. In this paper, we measured the light-induced structural changes in the Q1029L mutant protein of phy3-LOV2 by means of low-temperature FTIR spectroscopy, and the obtained spectra are compared with those of the wild type. Low-temperature UV-visible spectroscopy of Q1029L detected only one intermediate state, S390, at 77-295 K, as well as the wild type. The C(4)=O stretch of FMN at 1710 cm(-1) is shifted to 1723 cm(-1) in Q1029L, presumably because of the lack of hydrogen bonds between Gln1029 and FMN. Upon formation of S390, the C(4)=O group hydrogen bond is weakened in both wild type and Q1029L. These observations are fully consistent with the X-ray crystal structures of the unphotolyzed and S390 states. On the other hand, the C(4)=O stretch of FMN and amide-I vibrations are temperature-independent in Q1029L, in contrast to wild type, in which highly temperature-dependent FTIR spectra are detected. Amide-I vibrations of Q1029L at room temperature are similar to those of the wild type at 77-150 K but not at room temperature. These facts imply that the Q1029L mutant protein lacks progressive protein structural changes following flavin-cysteinyl adduct formation in the wild type, which eventually alter structures of beta sheet and alpha helix in the protein moiety. Hydrogen-bonding interaction of Gln1029 with the FMN chromophore likely plays an important role in the protein structural changes of phy3-LOV2.     

Blue light perception in plants. Detection and characterization of a light-induced neutral flavin radical in a C450A mutant of phototropin

The LOV2 domain of Avena sativa phototropin and its C450A mutant were expressed as recombinant fusion proteins and were examined by optical spectroscopy, electron paramagnetic resonance, and electron-nuclear double resonance. Upon irradiation (420-480 nm), the LOV2 C450A mutant protein gave an optical absorption spectrum characteristic of a flavin radical even in the absence of exogenous electron donors, thus demonstrating that the flavin mononucleotide (FMN) cofactor in its photogenerated triplet state is a potent oxidant for redox-active amino acid residues within the LOV2 domain. The FMN radical in the LOV2 C450A mutant is N(5)-protonated, suggesting that the local pH close to the FMN is acidic enough so that the cysteine residue in the wild-type protein is likely to be also protonated. An electron paramagnetic resonance analysis of the photogenerated FMN radical gave information on the geometrical and electronic structure and the environment of the FMN cofactor. The experimentally determined hyperfine couplings of the FMN radical point to a highly restricted delocalization of the unpaired electron spin in the isoalloxazine moiety. In the light of these results a possible radical-pair mechanism for the formation of the FMN-C(4a)-cysteinyl adduct in LOV domains is discussed.     

Mechanism of the SDS-resistant synaptotagmin clustering mediated by the cysteine cluster at the interface between the transmembrane and spacer domains

Synaptotagmin I (Syt I), a proposed major Ca(2+) sensor in the central nervous system, has been hypothesized as functioning in an oligomerized state during neurotransmitter release. We previously showed that Syts I, II, VII, and VIII form a stable SDS-resistant, beta-mercaptoethanol-insensitive, and Ca(2+)-independent oligomer surrounding the transmembrane domain (Fukuda, M., and Mikoshiba, K. (2000) J. Biol. Chem. 275, 28180-28185), but little is known about the molecular mechanism of the Ca(2+)-independent oligomerization by the synaptotagmin family. In this study, we analyzed the Ca(2+)-independent oligomerization properties of Syt I and found that it shows two distinct forms of self-oligomerization activity: stable SDS-resistant self-oligomerization activity and relatively unstable SDS-sensitive self-oligomerization activity. The former was found to be mediated by a post-translationally modified (i.e. fatty-acylated) cysteine (Cys) cluster (Cys-74, Cys-75, Cys-77, Cys-79, and Cys-82) at the interface between the transmembrane and spacer domains of Syt I. We also show that the number of Cys residues at the interface between the transmembrane and spacer domains determines the SDS- resistant oligomerizing capacity of each synaptotagmin isoform: Syt II, which contains seven Cys residues, showed the strongest SDS-resistant oligomerizing activity in the synaptotagmin family, whereas Syt XII, which has no Cys residues, did not form any SDS-resistant oligomers. The latter SDS-sensitive self-oligomerization of Syt I is mediated by the spacer domain, because deletion of the whole spacer domain, including the Cys cluster, abolished it, whereas a Syt I(CA) mutant carrying Cys to Ala substitutions still exhibited self-oligomerization. Based on these results, we propose that the oligomerization of the synaptotagmin family is regulated by two distinct mechanisms: the stable SDS-resistant oligomerization is mediated by the modified Cys cluster, whereas the relatively unstable (SDS-sensitive) oligomerization is mediated by the environment of the spacer domain.     

Structural roles of subunit cysteines in the folding and assembly of the DNA packaging machine (portal) of bacteriophage P22

The DNA packaging machine (portal assembly) of bacteriophage P22 is constructed from 12 copies of a multidomain 725-residue subunit comprising a complex alpha/beta fold. The portal subunit contains four cysteines (Cys 153, Cys 173, Cys 283, and Cys 516), which produce distinctive Raman markers in the spectral interval 2500-2600 cm(-1) originating from S-H bond-stretching vibrations diagnostic of S-H...X hydrogen-bonding interactions. The Raman spectrum is unique in the capability to characterize cysteine sulfhydryl interactions in proteins and shows that portal cysteine environments are significantly altered by assembly (Rodriguez-Casado et al. (2001) Biochemistry 40, 13583-13591). We have employed site-directed mutagenesis, size-exclusion chromatography, and Raman difference spectroscopy to characterize the roles of portal cysteines in subunit folding and dodecamer assembly. The stability of the portal monomer is severely reduced by a Cys --> Ser point mutation introduced at either residue 173 or 516. In the case of C516S, the destabilized monomer still forms portal rings, as visualized by negative-stain electron microscopy, whereas portal ring formation cannot be detected for C173S, which forms aberrant aggregates. The C283S mutant is a hyperstable monomer that is defective in portal ring formation. Interestingly, Cys 283 is suggested by secondary structure homology with the phi29 portal to be within a domain involved in DNA translocation. Conversely, the phenotype of the C153S mutant is close to that of the wild-type protein, implying that the sulfhydryl moiety of Cys 153 is not essential to formation of the native subunit fold and productive assembly dynamics. The present results demonstrate that cysteines of the P22 portal protein span a wide range of sulfhydryl hydrogen-bonding strengths in the wild-type assembly, that three of the four sulfhydryls play key roles in portal protein stability and assembly kinetics, and that substitution of a mutant seryl interaction (O-H...X) for a wild-type cysteinyl interaction (S-H...X) can either stabilize or destabilize the native fold depending upon sequence context.     

Primary Reactions of the LOV2 Domain of Phototropin Studied with Ultrafast Mid-Infrared Spectroscopy and Quantum Chemistry

Phototropins, major blue-light receptors in plants, are sensitive to blue light through a pair of flavin mononucleotide (FMN)-binding light oxygen and voltage (LOV) domains, LOV1 and LOV2. LOV2 undergoes a photocycle involving light-driven covalent adduct formation between a conserved cysteine and the FMN C(4a) atom. Here, the primary reactions of Avena sativa phototropin 1 LOV2 (AsLOV2) were studied using ultrafast mid-infrared spectroscopy and quantum chemistry. The singlet excited state (S1) evolves into the triplet state (T1) with a lifetime of 1.5 ns at a yield of ∼50%. The infrared signature of S1 is characterized by absorption bands at 1657 cm⁻¹, 1495-1415 cm⁻¹, and 1375 cm⁻¹. The T1 state shows infrared bands at 1657 cm⁻¹, 1645 cm⁻¹, 1491-1438 cm⁻¹, and 1390 cm⁻¹. For both electronic states, these bands are assigned principally to C=O, C=N, C-C, and C-N stretch modes. The overall downshifting of C=O and C=N bond stretch modes is consistent with an overall bond-order decrease of the conjugated isoalloxazine system upon a π-π^∗ transition. The configuration interaction singles (CIS) method was used to calculate the vibrational spectra of the S1 and T1 excited ππ^∗ states, as well as respective electronic energies, structural parameters, electronic dipole moments, and intrinsic force constants. The harmonic frequencies of S1 and T1, as calculated by the CIS method, are in satisfactory agreement with the evident band positions and intensities. On the other hand, CIS calculations of a T1 cation that was protonated at the N(5) site did not reproduce the experimental FMN T1 spectrum. We conclude that the FMN T1 state remains nonprotonated on a nanosecond timescale, which rules out an ionic mechanism for covalent adduct formation involving cysteine-N(5) proton transfer on this timescale. Finally, we observed a heterogeneous population of singly and doubly H-bonded FMN C(4)=O conformers in the dark state, with stretch frequencies at 1714 cm⁻¹ and 1694 cm⁻¹, respectively.     

The FMN to heme electron transfer in cytochrome P450BM-3. Effect of chemical modification of cysteines engineered at the FMN-heme domain interaction site

The crystal structure of the complex between the heme and FMN-containing domains of Bacillus megaterium cytochrome P450BM-3 (Sevrioukova, I. F., Li, H., Zhang, H., Peterson, J. A., and Poulos, T. L. (1999) Proc. Natl. Acad. Sci. U. S. A. 96, 1863-1868) indicates that the proximal side of the heme domain molecule is the docking site for the FMN domain and that the Pro(382)-Gln(387) peptide may provide an electron transfer (ET) path from the FMN to the heme iron. In order to evaluate whether ET complexes formed in solution by the heme and FMN domains are structurally relevant to that seen in the crystal structure, we utilized site-directed mutagenesis to introduce Cys residues at positions 104 and 387, which are sites of close contact between the domains in the crystal structure and at position 372 as a control. Cys residues were modified with a bulky sulfhydryl reagent, 1-dimethylaminonaphthalene-5-sulfonate-L-cystine (dansylcystine (DC)), to prevent the FMN domain from binding at the site seen in the crystal structure. The DC modification of Cys(372) and Cys(387) resulted in a 2-fold decrease in the rates of interdomain ET in the reconstituted system consisting of the separate heme and FMN domains and had no effect on heme reduction in the intact heme/FMN-binding fragment of P450BM-3. DC modification of Cys(104) caused a 10-20-fold decrease in the interdomain ET reaction rate in both the reconstituted system and the intact heme/FMN domain. This indicates that the proximal side of the heme domain molecule represents the FMN domain binding site in both the crystallized and solution complexes, with the area around residue 104 being the most critical for the redox partner docking.