Wavelength dependent cis-trans isomerization in vision.

The primary event in vision is the light-driven cis-trans isomerization of the 11-cis-retinal chromophore in the G-protein coupled receptor rhodopsin. Early measurements showed that this photoisomerization has a reaction quantum yield phi of approximately 0.67 [Dartnall (1936) Proc. R. Soc. A 156, 158-170; Dartnall (1968) Vision Res. 8, 339-358] and suggested that the quantum yield was wavelength independent [Schneider (1939) Proc. Natl. Acad. Sci. U.S.A. 170, 102-112]. Here we more accurately determine phi(500) = 0.65 +/- 0.01 and reveal that phi surprisingly depends on the wavelength of the incident light. Although there is no difference in the quantum yield between 450 and 480 nm, the quantum yield falls significantly as the photon energy is reduced below 20 000 cm(-1) (500 nm). At the reddest wavelength measured (570 nm), the quantum yield is reduced by 5 +/- 1% relative to the 500 nm value. These experiments correct the long-held presumption that the quantum yield in vision is wavelength independent, and support the hypothesis that the 200 fs photoisomerization reaction that initiates vision is dictated by nonstationary excited-state vibrational wave packet dynamics.     

The primary event in vision investigated by time-resolved fluorescence spectroscopy.

The picosecond fluorescence kinetics and quantum yield from bovine rhodopsin were measured in the 5-40 degrees K range. The fluorescence rise and decay times are faster than our resolution of 15 ps (full width at half maximum) over this entire temperature range. The size of the observed emission was also temperature independent, and we find that the upper limit of rhodopsin's fluorescence quantum yield to be phi f approximately equal to 10(-5). Replacing all of rhodopsin's exchangeable protons with deuterons by suspending rhodopsin in D2O had no effect on either the kinetics of the emission or the value of the quantum yield. Our data provide strong confirmation of the idea that the first step in the visual process is an excited-state cis-to-trans isomerization about the C11-C12 double bond of retinal.     

Analysis of the mode-specific excited-state energy distribution and wavelength-dependent photoreaction quantum yield in rhodopsin

The photoreaction quantum yield of rhodopsin is wavelength dependent: phi(lambda) is reduced by up to 5% at wavelengths to the red of 500 nm but is invariant (phi = 0.65 +/- 0.01) between 450 and 500 nm (Kim et al., 2001). To understand this nonstatistical internal conversion process, these results are compared with predictions of a Landau-Zener model for dynamic curve crossing. The initial distribution of excess photon energy in the 28 Franck-Condon active vibrational modes of rhodopsin is defined by a fully thermalized sum-over-states vibronic calculation. This calculation reveals that absorption by high-frequency unreactive modes (e.g., C[double bond]C stretches) increases as the excitation wavelength is shifted from 570 to 450 nm whereas relatively less energy is deposited into reactive low-frequency modes. This result qualitatively explains the experimentally observed wavelength dependence of phi(lambda) for rhodopsin and reveals the importance of delocalized, torsional modes in the reactive pathway.     

Quantum efficiencies of bacteriorhodopsin photochemical reactions.

Determination of quantum efficiencies of bacteriorhodopsin (bR) photoreactions is an essential step toward a full understanding of its light-driven proton-pumping mechanism. The bR molecules can be photoconverted into and from a K state, which is stable at 110 K. I measured the absorption spectra of pure bR, and the photoequilibrium states of bR and K generated with 420, 460, 500, 510, 520, 540, 560, 570, 580, 590, and 600 nm illumination at 110 K. The fraction of the K population in the photoequilibrium state, fk, is determined by AbR and AK the absorbances of the bR and K states at the excitation wavelengths, and also by phi 1 and phi 2, the quantum efficiencies for the bR to K and K to bR photoconversion: fK = phi 1 AbR/(phi 1AbR + phi 2Ak). By assuming that the ratio phi 1/phi 2 is the same at two different but close wavelengths, for example 570 and 580 nm, the value of phi 1/phi 2 at 570 and 580 nm was determined to be 0.55 +/- 0.02, and the spectrum of the K state was obtained with the peak absorbance at 607 nm. The values of phi 1/phi 2 at the other excitation wavelengths were then evaluated using the known K spectrum, and show almost no dependence on the excitation wavelength within the main band. The result phi 1/phi 2 = 0.55 +/- 0.02 disagrees with those of many other groups. The advantages of this method over others are its minimal assumptions and its straightforward procedure.     

Raman microscope and quantum yield studies on the primary photochemistry of A2-visual pigments.

The 77-K resonance Raman vibrational spectrum of intact goldfish rod photoreceptors containing 3,4-dehydro (A2) retinal is dominated by scattering from the 9-cis component of the steady state at all excitation wavelengths. Intact goldfish photoreceptors were regenerated with an A1-retinal chromophore to determine whether this behavior is caused by the protein or the chromophore. The resulting Raman spectrum was typical of an A1-pigment exhibiting significant scattering from all three components of the steady state: rhodopsin, bathorhodopsin, and isorhodopsin. Furthermore, regeneration of bovine opsin with A2-retinal produces a characteristic "A2-Raman spectrum" that is dominated by scattering from the 9-cis pigment. We conclude that the differences between the Raman spectra of the A1-and A2-pigments are caused by some intrinsic difference in the photochemical properties of the retinal chromophores. To quantitate these observations, the 77-K adsorption spectra and the photochemical quantum yields (phi) of the native A2-goldfish and the regenerated A2-bovine pigments were measured. In the goldfish A2-pigment, the value of phi 4 (9-cis----trans) is 0.05; phi 3 (trans----9-cis) is 0.10; and phi 2 (trans----11-cis) is 0.35. By contrast, in the bovine A1-pigment, these quantum yields are 0.10, 0.053, and 0.50, respectively. The reduced value of phi 4 and the increased value of phi 3 in the goldfish pigment confirms that the 9-cis isomer is photochemically more stable in A2-pigments.     

Kinetics and mechanism of protection of adenine from sulphate radical anion by caffeic acid under anoxic conditions

The rates of photo-oxidation of adenine in the presence of peroxydisulphate (PDS) have been determined by measuring the absorbance of adenine at 260.5 nm spectrophotometrically. The rates and the quantum yields (phi) of oxidation of adenine by sulphate radical anion (SO4(-)) have been determined in the presence of different concentrations of caffeic acid. Increase in the concentration of caffeic acid is found to decrease the rate of oxidation of adenine suggesting that caffeic acid acts as an efficient scavenger of SO4(-) and protects adenine from it; SO4(-) competes for adenine as well as for caffeic acid. From competition kinetics, the rate constant of SO4(-) with caffeic acid has been calculated to be 1.24 +/- 0.2 x 10(10) mol(-1)dm(3)s(-1). The quantum yields of photo-oxidation of adenine have been calculated from the rates of oxidation of adenine and the light intensity absorbed by PDS at 254 nm, the wavelength at which PDS is activated to SO4' -. The results of experimentally determined quantum yields (phi exptl) and the quantum yields calculated (phi cl) by assuming that caffeic acid acts only as a scavenger of SO4(-) radicals show that phi exptl values are lower than phi cl values. The phi prime values, which are experimentally found quantum yield values at each caffeic acid concentration and corrected for SO4(-) scavenging by caffeic acid, are also found to be greater than phi exptI values. These observations suggest that the adenine radicals are repaired by caffeic acid, in addition to scavenging of sulphate radical anions.     

Photopigment and receptor properties in Drosophila compound eye and ocellar receptors

A review of the spectral sensitivity and the rhodopsin and metarhodopsin characteristics in three compound eye receptor types (R1-6, R7, and R8) and ocellar receptors is presented (Fig. 1). Photopigment properties were determined from measures of conversion efficiency. The photopigments of R1-6 were studied using in vivo microspectrophotometry in the deep pseudopupil of white-eyed flies. These studies yielded a refined estimate of the R1-6 metarhodopsin spectrum (Fig. 2). The quantum efficiency relative to the spectral sensitivity estimate of the rhodopsin spectrum was factored out. The quantum efficiency of rhodopsin is about 1.75 times that of metarhodopsin. The peak absorbance of metarhodopsin was estimated to be about 2.6 times that of rhodopsin. The mechanism of the two-peaked R1-6 spectral sensitivity and metarhodopsin spectrum is discussed in terms of evidence that there is only one rhodopsin in R1-6 and that vitamin A deprivation preferentially lowers ultraviolet sensitivity. The prolonged depolarizing afterpotential is reviewed from the standpoint of the internal transmitter hypothesis of visual excitation. A careful comparison of the intensity-responsivity for photopigment conversion and its adaptional consequences is made (Fig. 3).     

The molar extinction of rhodopsin

The molar extinction of rhodopsin is 40,600 cm.² per mole equivalent of retinene; i.e., this is the extinction of a solution of rhodopsin which is produced by, or yields on bleaching, a molar solution of retinene. The molar extinctions of all-trans retinene and all-trans retinene oxime have also been determined in ethyl alcohol and aqueous digitonin solutions. On the assumption that each chromophoric group of rhodopsin is made from a single molecule of retinene, it is concluded that the primary photochemical conversion of rhodopsin to lumi-rhodopsin has a quantum efficiency of 1; though the over-all bleaching of rhodopsin in solution to retinene and opsin may have a quantum efficiency as low as one-half. On bleaching cattle rhodopsin, about two sulfhydryl groups appear for each molecule of retinene liberated. In frog rhodopsin the —SH:retinene ratio appears to be higher, 5:2 or perhaps even 3:1. Some of this sulfhydryl appears to have been engaged in binding retinene to opsin; some may have been exposed as the result of changes in opsin which accompany bleaching, comparable with protein denaturation.     

Temperature Dependence of the Linkage of Quantum Yield of Photosystem II to CO2 Fixation in C4 and C3 Plants

The temperature dependence of quantum yields of electron transport from photosystem II (PSII) ([phi]II, determined from chlorophyll a fluorescence) and CO2 assimilation ([phi]CO2, apparent quantum yield for CO2 assimilation) were determined simultaneously in vivo. With C4 species representing NADP-malic enzyme, NAD-malic enzyme, and phosphoenolpyruvate carboxykinase subgroups, the ratio of [phi]II/[phi]CO2 was constant over the temperature range from 15 to 40[deg]C at high light intensity (1100 [mu]mol quanta m-2 s-1). A similar response was obtained at low light intensity (300 [mu]mol quanta m-2 s-1), except the ratio of [phi]II/[phi]CO2 increased at high temperature. When the true quantum yield for CO2 fixation ([phi]CO2*) was calculated by correcting for respiration in the light (estimated from temperature dependence of dark respiration), the ratio of [phi]II/[phi]C02* remained constant with varying temperature and under both light intensities in all C4 species examined. Because the [phi]II/[phi]CO2* ratio was the same in C4 monocots representing the three subgroups, the ratio was not affected by differences in the bio-chemical mechanism of concentrating CO2 in the bundle sheath cells. The results suggest that PSII activity is closely linked to the true rate of CO2 fixation in C4 plants. The close relationship between [phi]II and [phi]CO2* in C4 species under varying temperature and light intensity conditions is apparently due to a common low level of photorespiration and a primary requirement for reductive power in the C3 pathway. In contrast, in a C3 plant the [phi] II/[phi]CO2* ratio is higher under normal atmospheric conditions than under nonphotorespiratory conditions and it increases with rising temperature. This decrease in efficiency in utilizing energy derived from PSII for CO2 fixation is due to an increase in photorespiration. In both the C3 and C4 species, photochemistry is limited under low temperature, and thus excess energy must be dissipated by nonphotochemical means.     

Energy storage in the primary step of the photocycle of bacteriorhodopsin.

A pulsed-dye laser low temperature photocalorimeter is used to study the enthalpy differences between light-adapted bacteriorhodopsin (bR568) and its primary photoproduct (K) at 77 K. A key feature of our experimental method is the use of the laser-induced photostationary state as an internal reference. Analyses of the forward (bR leads to K), reverse (K leads to bR), and mixed (bR in equilibrium K) photoreactions were carried out to measure delta H12 = EK - EbR. All three experiments yielded identical values of delta H12 within experimental error (delta Have12 = 15.8 +/- 2.5 kcal mol-1). Accordingly, the primary event in the photocycle of light-adapted bacteriorhodopsin stores approximately 30% of the absorbed photon energy at the 568-nm absorption maximum. We observe that the quantum yields phi f1(bR leads to K) and phi r2(K leads to bR) add up to unity within experimental error: phi f1 + phi r2 = 1.02 +/- 0.19 for phi f1 in the range 0.28-0.33. A theoretical analysis of energy storage in K suggests that at least one-half of the enthalpy difference between K and bR is associated with charge separation accompanying chromophore isomerization.     

The nature of the primary photochemical events in rhodopsin and isorhodopsin.

The nature of the primary photochemical events in rhodopsin and isorhodopsin is studied by using low temperature actinometry, low temperature absorption spectroscopy, and intermediate neglect of differential overlap including partial single and double configuration interaction (INDO-PSDCI) molecular orbital theory. The principal goal is a better understanding of how the protein binding site influences the energetic, photochemical, and spectroscopic properties of the bound chromophore. Absolute quantum yields for the isorhodopsin (I) to bathorhodopsin (B) phototransformation are assigned at 77 K by using the rhodopsin (R) to bathorhodopsin phototransformation as an internal standard (phi R----B = 0.67). In contrast to rhodopsin photochemistry, isorhodopsin displays a wavelength dependent quantum yield for photochemical generation of bathorhodopsin at 77 K. Measurements at seven wavelengths yielded values ranging from a low of 0.089 +/- 0.021 at 565 nm to a high of 0.168 +/- 0.012 at 440 nm. An analysis of these data based on a variety of kinetic models suggests that the I----B phototransformation encounters a small activation barrier (approximately 0.2 kcal mol-1) associated with the 9-cis----9-trans excited-state torsional-potential surface. The 9-cis retinal chromophore in solution (EPA, 77 K) has the smallest oscillator strength relative to the other isomers: 1.17 (all-trans), 0.98 (9-cis), 1.04 (11-cis), and 1.06 (13-cis). The effect of conformation is quite different for the opsin-bound chromophores. The oscillator strength of the lambda max absorption band of I is observed to be anomalously large (1.11) relative to the lambda max absorption bands of R (0.98) and B (1.07). The wavelength-dependent photoisomerization quantum yields and the anomalous oscillator strength associated with isorhodopsin provide important information on the nature of the opsin binding site. Various models of the binding site were tested by using INDO-PSDCI molecular orbital theory to predict the oscillator strengths of R, B, and I and to calculate the barriers and energy storage associated with the photochemistry of R and I for each model. Our experimental and theoretical investigation leads to the following conclusions: (a) The counterion (abbreviated as CTN) is not intimately associated with the imine proton in R, B, or I. The counterion lies underneath the plane of the chromophore in R and I, and the primary chromophore-counterion electrostatic interactions involve C15-CTN and C13-CTN. These interactions are responsible for the anomalous oscillator strength of I relative to R and B.(ABSTRACT TRUNCATED AT 400 WORDS)     

On the primary quantum yields in the bacteriorhodopsin photocycle.

Pulsed Nd laser experiments in suspensions of the purple membrane of Halobacterium halobium are carried out at room temperature. At sufficiently high laser intensities, a photostationary mixture of bacteriorhodopsin (BR) and its red-shifted (batho) photoproduct (K) is obtained. The spectra of the first three intermediates in the photocycle are reported. The data yield a value of phi1/phi2=0.40 +/- 0.05 for the ratio of the quantum yields of the forward (phi1) and reverse (phi2) processes, setting an upper limit of approximately 0.4 for the quantum efficiency of the cycle at room temperature. This method is generally available for the determination of phi2 in the case of a photoequilibrium: A in equilibrium B, where B is a short-lived transient and phi1 is known from low intensity measurements. Its potential application is of importance for the study of the photophysics of visual pigments at physiological temperatures.     

Regulation of immune responses by T cell subsets. Role of helper and suppressor T cells in the development and expression of MHC-restricted antibody responses to L-glutamic acid60-L-alanine30-L-tyrosine10 (GAT) by (responder X responder)F1 spleen cells

The roles of helper and suppressor T cells in the development and expression of antibody responses to GAT were studied in (responder X responder)F1 mice immunized with parental GAT-M phi. Spleen cells from (B10 X B10.D2)F1 mice primed in vivo with B10 or B10.D2 GAT-M phi developed secondary in vitro plaque-forming cell (PFC) responses only when stimulated by GAT-M phi syngeneic with the GAT-M phi used for in vivo priming. By contrast, virgin F1 spleen cells developed comparable primary PFC responses to both parental GAT-M phi Co-culture of T cells from (B10 X B10.D2)F1 mice primed in vivo by B10 GAT-M phi with virgin (B10 X B10.D2)F1 spleen cells demonstrated the presence of suppressor cells that inhibited the primary response of virgin spleen cells stimulated by B10.D2 GAT-M phi. Spleen cells from (B10 X B10.D2)F1 mice primed in vivo with B10.D2 GAT-M phi had suppressor T cells that suppressed primary responses stimulated by B10 GAT-M phi. The suppressor T cell mechanism was composed of at least two regulatory T cell subsets. Suppressor-inducer T cells were Lyt-2-, I-J+ and must be derived from immune spleen cells. Suppressor-effector T cells can be derived from virgin or immune spleens and were Lyt-2+ cells. When the suppressor mechanism was disabled by treatment with 1000 rad gamma irradiation or removal of Lyt-2+ cells, Lyt-2-helper T cells from (B10 X B10.D2)F1 mice primed with B10 GAT-M phi provided radioresistant help to virgin F1 B cells stimulated by B10 but not B10.D2 GAT-M phi. Suppressor inducer Lyt-2-,I-J+ cells from B10 GAT-M phi-primed (B10 X B10.D2)F1 mice were separated from the primed Lyt-2-,I-J-helper T cells. In the presence of Lyt-2+ suppressor effector cells, the Lyt-2-,I-J+ suppressor-inducer suppressed the primary response of virgin spleen or virgin T plus B cells stimulated by both B10 and B10.D2 GAT-M phi. Therefore, suppressor T cells were able to suppress primary but not secondary GAT-specific PFC responses stimulated by either parental GAT-M phi. These results showed that immunization of (responder X responder)F1 mice with parental GAT-M phi results in the development of antigen-specific helper and suppressor T cells. The primed helper T cells were radioresistant and were genetically restricted to interact with GAT in association with the major histocompatibility complex antigens of the M phi used for in vivo priming.(ABSTRACT TRUNCATED AT 400 WORDS)     

Absolute action spectrum of E-FADH2 and E-FADH2-MTHF forms of Escherichia coli DNA photolyase

Escherichia coli DNA photolyase mediates photorepair of pyrimidine dimers occurring in UV-damaged DNA. The enzyme contains two chromophores, 1,5-dihydroflavin adenine dinucleotide (FADH2) and 5,10-methenyltetrahydrofolylpolyglutamate (MTHF). To define the roles of the two chromophores in the photochemical reaction(s) resulting in DNA repair and the effect of DNA structure on the photocatalytic step, we determined the absolute action spectra of the enzyme containing only FADH2 (E-FADH2) or both chromophores (E-FADH2-MTHF), with double- and single-stranded substrates and with substrates of different sequences in the immediate vicinity of the thymine dimer. We found that the shape of the action spectrum of E-FADH2 matches that of the absorption spectrum with a quantum yield phi (FADH2) = 0.69. The action spectrum of E-FADH2-MTHF is also in a fairly good agreement with the absorption spectrum with phi (FADH2-MTHF) = 0.59. From these values and from the previously established properties of the two chromophores, we propose that MTHF transfers energy to FADH2 with a quantum yield of phi epsilon T = 0.8 and that 1FADH2 singlet transfers an electron to or from the dimer with a quantum yield phi ET = 0.69. The chemical nature of the chromophores did not change after several catalytic cycles. The enzyme repaired a thymine dimer in five different sequence contexts with the same efficiency. Similarly, single- and double-stranded DNAs were repaired with the same overall quantum yield.     

Photopigment and receptor properties in Drosophila compound eye and ocellar receptors

A review of the spectral sensitivity and the rhodopsin and metarhodopsin characteristics in three compound eye receptor types (R1–6, R7, and R8) and ocellar receptors is presented (Fig. 1). Photopigment properties were determined from measures of conversion efficiency. The photopigments of R1–6 were studied using in vivo microspectrophotometry in the deep pseudopupil of white-eyed flies. These studies yielded a refined estimate of the R1–6 metarhodopsin spectrum (Fig. 2). The quantum efficiency relative to the spectral sensitivity estimate of the rhodopsin spectrum was factored out. The quantum efficiency of rhodopsin is about 1.75 times that of metarhodopsin. The peak absorbance of metarhodopsin was estimated to be about 2.6 times that of rhodopsin. The mechanism of the two-peaked R1–6 spectral sensitivity and metarhodopsin spectrum is discussed in terms of evidence that there is only one rhodopsin in R1–6 and that vitamin A deprivation preferentially lowers ultraviolet sensitivity. The prolonged depolarizing afterpotential is reviewed from the standpoint of the internal transmitter hypothesis of visual excitation. A careful comparison of the intensity-responsivity for photopigment conversion and its adaptional consequences is made (Fig. 3).     

Action mechanism of Escherichia coli DNA photolyase. III. Photolysis of the enzyme-substrate complex and the absolute action spectrum

The absolute action spectrum of Escherichia coli DNA photolyase was determined in vitro. In vivo the photoreactivation cross-section (epsilon phi) is 2.4 X 10(4) M-1 cm-1 suggesting that the quantum yield (phi) is about 1.0 if one assumes that the enzyme has the same spectral properties (e.g. epsilon 384 = 1.8 X 10(4) M-1 cm-1) in vivo as those of the enzyme purified to homogeneity. The relative action spectrum of the pure enzyme (blue enzyme that contains FAD neutral semiquinone radical) agrees with the relative action spectrum for photoreactivation of E. coli, having lambda max = 384 nm. However, the absolute action spectrum of the blue enzyme yields a photoreactivation cross-section (epsilon phi = 1.2 X 10(3) at 384 nm) that is 20-fold lower than the in vivo values indicative of an apparent lower quantum yield (phi approximately equal to 0.07) in vitro. Reducing the enzyme with dithionite results in reduction of the flavin semiquinone and a concomitant 12-15-fold increase in the quantum yield. These results suggest that the flavin cofactor of the enzyme is fully reduced in vivo and that, upon absorption of a single photon in the 300-500 nm range, the photolyase chromophore (which consists of reduced FAD plus the second chromophore) donates an electron to the pyrimidine dimer causing its reversal to two pyrimidines. The reduced chromophore is regenerated at the end of the photochemical step thus enabling the enzyme to act catalytically.+     

Quantum efficiency of the photochemical cycle of bacteriorhodopsin

Values in the literature for the quantum efficiency of the photochemical cycle of bacteriorhodopsin (bR) range from 0.25 to 0.79 and the sum of the quantum yields of the forward and back photoreactions [Formula: see text] has been proposed to be 1. In the present work, low intensity laser flashes (532 nm) and kinetic spectroscopy were used to determine the quantum efficiency of bR photoconversion, [UNK]_bR, by measuring transient bleaching of bR at 610 nm in the millisecond time scale. Bovine rhodopsin (R) in 2% ammonyx LO was used as a photon counter. We find that the ratio of the quantum yields of bacteriorhodopsin photoconversion and bleaching of rhodopsin, [UNK]_bR/[UNK]_R, is 0.96 ± 0.04. Based on the quantum yield of the photobleaching of rhodopsin, 0.67, the quantum efficiency of bR photoconversion was determined to be 0.64 ± 0.04. The quantum yield of M formation was found to be 0.65 ± 0.06. From the transient bleaching of bR at 610 nm with a saturating laser flash (28 mJ/cm²) the maximum amount of bR cycling was estimated to be 47 ± 3%. From this value and the spectrum of K published in the literature, the ratio of the efficiencies of the forward and back light reactions, [UNK]₁/[UNK]₂, was estimated to be 0.67 ± 0.06 and so [UNK]₂ ≈ 1 (0.94 ± 0.06). The sum of [UNK]₁ + [UNK]₂ ≈ 1.6. It was found that repeated high-intensity laser flashes (>20 mJ/cm²) irreversibly transformed bR into two stable photoproducts. One has its absorption maximum at 605 nm and the other has a well-resolved vibronic spectrum with maxima at 342, 359 (main peak), and 379 nm. The quantum yield of the formation of the photoproducts is ≈ 10^-4.     

QM/MM study of energy storage and molecular rearrangements due to the primary event in vision

The energy storage and the molecular rearrangements due to the primary photochemical event in rhodopsin are investigated by using quantum mechanics/molecular mechanics hybrid methods in conjunction with high-resolution structural data of bovine visual rhodopsin. The analysis of the reactant and product molecular structures reveals the energy storage mechanism as determined by the detailed molecular rearrangements of the retinyl chromophore, including rotation of the (C11-C12) dihedral angle from -11 degrees in the 11-cis isomer to -161 degrees in the all-trans product, where the preferential sense of rotation is determined by the steric interactions between Ala-117 and the polyene chain at the C13 position, torsion of the polyene chain due to steric constraints in the binding pocket, and stretching of the salt bridge between the protonated Schiff base and the Glu-113 counterion by reorientation of the polarized bonds that localize the net positive charge at the Schiff-base linkage. The energy storage, computed at the ONIOM electronic-embedding approach (B3LYP/6-31G*:AMBER) level of theory and the S0-->S1 electronic-excitation energies for the dark and product states, obtained at the ONIOM electronic-embedding approach (TD-B3LYP/6-31G*//B3LYP/6-31G*:AMBER) level of theory, are in very good agreement with experimental data. These results are particularly relevant to the development of a first-principles understanding of the structure-function relations in prototypical G-protein-coupled receptors.     

Bacteriophage-associated glycan hydrolases specific for Escherichia coli capsular serotype K12

Four bacteriophages were identified, which carry glycan hydrolases specific for the Escherichia coli K12 capsular polysaccharide. All these glycanases catalyze the hydrolysis of the alpha-L-rhamnosyl-1,5-beta-3-deoxy-D-manno-2-octulosonic acid linkage as demonstrated with a special thiobarbituric acid assay procedure, which discriminates between the C5 substituted and unsubstituted 3-deoxy-D-manno-2-octulosonic acid (dOclA). This assay, together with gel filtration, 1H-NMR and 13C-NMR spectroscopy showed that depolymerization led to the dimer of the K12 repeating unit, (,5-beta-dOcl1Ap-2,3-alpha-LRhap-1,2-alpha LRhap-1,)2, as the primary degradation product. The phages (phi 12-W, phi 12-S, phi 82-W1, phi 82-W2) were tested for their ability to infect Escherichia coli strains Su65-42 (O4:K12:H-) and CDC63-57 [O139:K82(12):H1]. phi 12-W and phi 12-S, respectively, infected strain Su65-42 only, phi 82-W2 CDC63-57 only, and phi 82-W1 both bacterial strains. These distinct host specificities cannot be explained by differences in the action of the glycanases, which depolymerize the capsules of both strains.