Aggregation of chlorophylls in monolayers. V. The effect of water on chlorophyll a and chlorophyll b in mono and multilayer arrays

The nature of the interactions between water molecules and monolayers and multilayers of chlorophyll a (Chl a), and monolayers and multilayers of Chl b. obtained by the Langmuir-Blodgett technique, is examined by infrared spectroscopy. Following deposition of the monolayer or multilayer of Chl a or Chl b onto a plate, repetitive scans showed some modifications in the infrared spectra which are interpreted as a reorganization of the molecules as some water molecules leave the array. Drying the sample further modifies the spectra, which indicates the departure of more tenacious water molecules. Putting the sample in a moist atmosphere does not restore the original spectrum. This is an indication of a nonreversibie reorganization in the chlorophyll array. The spectra of the monolayer of chlorophyll are much more complicated than those of the multilayer, owing to the nonintegrating effect of the monolayer, which reveals the perturbing effect of the different dielectric milieux on each functional group. On the basis of the analysis of the spectra and the information gathered from the surface pressure isotherms, a model is proposed for the monolayer arrangement at the air/water interface which implies two set of dimers of water per molecule of chlorophyll. One pair of dimers constitutes the water of the first kind and is composed of vapor-like dimers. This kind of water is situated between the porphyrin planes of chlorophyll molecules and is easily removed from the monolayer. The second pair of dimers is composed of water of the second and third kinds situated between the Mg atom of the chlorophyll molecules and the water of the subphase. The second kind of water is closest to the Mg atom and is the most difficult one to remove. The third kind of water is closest to the surface and its mobility is intermediate between that of water of the first kind and that of water of the second kind. Comparing the infrared spectra of a freshly prepared monolayers of Chl a with the resonance Raman spectra of intact chloroplasts (M. Lutz, Biochim. Biophys. Acta 460 (1977) 408), we notice great similarities. This is an indication that the model we propose for the monolayer of Chl a could play an important role in the chloroplast.     

Aggregation of chlorophylls in monolayers. VI. Infrared study of the CH stretching bands of chlorophyll a and of chlorophyll b in monolayers

The CH vibrational stretch bands of chlorophyll (Chl) in monolayers, obtained by the Langmuir-Blodgett technique have been studied by infrared spectroscopy. Compared to a solution or to a multilayer which shows three to four bands, the spectra of Chl a or Chl b molecules in monolayers have revealed more than seven bands, which are assigned to the various CH groups in the molecule. In contrast to solutions or to multilayer samples which give featureless bands, each band of the monolayers is composed of many components which are modified when the system is perturbed either by drying or by hydration techniques. The separation between the components of the CH aliphatic bands is typical of crystalline field splitting and the modification of the intensities of these components is associated with the movement of the phytyl chain of the chlorophyll molecules. The CH aromatic stretch bands have been observed; the displacement and variation of the intensities of these bands are associated with deformation of the porphyrin ring. The CH band of the formyl group on Chl b has also been observed. The displacement and variation of the intensity of this band are related to the association that this group makes with the surrounding molecules and with the displacement of the porphyrin ring.     

Determination of anesthetic molecule environments by infrared spectroscopy. II. Multiple sites for nitrous oxide in proteins, lipids, and brain tissue

The presence of molecules of the general anesthetic nitrous oxide (N2O) in oils, esters, proteins, red cells, cream, lipid vesicles, and brain tissue upon exposure to the gas was observed by infrared spectroscopy. Analysis of the N-N-O antisymmetric stretch band reveals a distribution of N2O molecules among several sites of differing polarity in these solutions and tissues. The sensitivity of the band intensity and frequency to the number and strength of the dipoles in the solvating molecules is demonstrated by the resolution of N2O-ester and N2O-alkane interactions in acetic acid ethyl ester and oleic acid methyl ester. In all aqueous solutions and in all tissues a population of N2O molecules in water is observed. At least two sites of N2O-protein interaction are observed in purified hemoglobin A and packed red cells; multiple N2O sites may also be present in bovine serum albumin. Two sites of N2O-lipid interaction are observed in whipping cream and in an aqueous suspension of phosphatidylcholine vesicles. The sites providing the least polar immediate environment to N2O in hemoglobin, cream, and vesicles give similar band frequencies to those found in pure alkane solvents. Infrared spectra of bovine brain tissue, upon exposure to N2O, show N2O molecules present in water and in two less-polar environments. Analysis of spectra of N2O in cerebellum tissue removed from a dog under halothane-N2O anesthesia reveals, in addition to N2O in water, a single population of N2O molecules in an alkane-like environment. Infrared spectroscopy provides a unique means of probing the structure of the environment of N2O and should prove useful in correlating anesthetic potency with anesthetic environment under physiological conditions.     

Aggregation of chlorophylls in monolayers.

The interaction of dioxane vapor with monolayer and multilayers of chlorophyll has been studied using electronic and infarared spectroscopies. Our results indicate the formation of a complex implying the oxygene of the dioxanc molecules with the magnesiums of adjacent chlorophyll molecules. These results are consistent with the molecular orbital calculations, using the "free electron network" method done by Le Brech, Leblanc and Antippa [Chem. Phys. Letters 26(1974) 37-44].     

Water structural changes in the bacteriorhodopsin photocycle: analysis by Fourier transform infrared spectroscopy.

The Fourier transform infrared difference spectra between light-adapted bacteriorhodopsin (BR) and its photointermediates, L and M, were analyzed for the 3750-3450-cm-1 region. The O-H stretching vibrational bands were identified from spectra upon substitution with 2H2O. Among them, the 3642-cm-1 band of BR was assigned to water by substitution with H2(18)O. By a comparison with the published infrared spectra of the water in model systems [Mohr, S.C., Wilk, W.D., & Barrow, G.M. (1965) J. Am. Chem. Soc. 87, 3048-3052], it is shown that the O-H bonds of the water in BR interact very weakly. Upon formation of L, the interaction becomes stronger. The O-H bonds of the protein side chain undergo similar changes. On the other hand, M formation further weakens the interaction of the same water molecules in BR. The appearance of a sharp band at 3486 cm-1, which was assigned tentatively to the N-H stretching vibration of the peptide bond, is unique to L. The results suggest that the water molecules are involved in the perturbation of Asp-96 in the L intermediate and that they are exerted from the protonated Schiff base which changes position upon the light-induced reaction.     

Crystallization of water in multilamellar vesicles

The two-step crystallization of water in multilamellar vesicles (MLVs) of phosphatidylcholines has been investigated. The main crystallization occurs near -15 degrees C and involves bulk water. Contrary to unilamellar vesicles, a sub-zero phase transition is observed for MLVs at -40 degrees C that corresponds to the crystallization of interstitial water, as proved by Fourier transform infrared absorption and differential scanning calorimetry (DSC) experiments. Furthermore, by means of the DSC method and, more specifically, using the enthalpy change values Delta H(sub) at the sub-zero transition, the number of water molecules per 1,2-dipalmitoylphosphatidylcholine (DPPC) molecule giving rise to this transition has been estimated for different H(2)O/DPPC molar ratios. The curve of the molecular fraction of water molecules involved in the sub-zero transition versus the H(2)O/DPPC molar ratio exhibits a maximum for H(2)O/DPPC equal to 27 (40% in mass of water) and tends towards zero for H(2)O/DPPC ratio values approaching that of the swelling limit of the membrane. A smaller enthalpy value of the sub-zero transition is found for 1-oleoyl-2-palmitoyl-3-phosphatidylcholine (OPPC) than for DPPC. This may be explained by the decrease of interstitial water's quantity when the lipid contains an unsaturated chain. When troxerutin, a hydrophilic drug, is added to the DPPC multilayers, the decrease of Delta H(sub) and melting enthalpy of bulk water is attributed to a decrease of the entropy of the liquid phase owing to the network of water molecules surrounding troxerutin molecules. In all cases, the experiments revealed that the sub-zero transition occurs only in the presence of excess water with respect to the swelling limit of membranes. This evidence could be, at least qualitatively, related to an increase of membrane pressure on interstitial water subsequent to bulk water crystallization.     

Alcohols dehydrate lipid membranes: an infrared study on hydrogen bonding.

The effects of alcohols (methanol, ethanol, and n-butanol) on the hydrogen bonding of dipalmitoylphosphatidylcholine (DPPC) were studied by Fourier-transform infrared spectroscopy (FTIR) in water-in-oil (carbon tetrachloride) reversed micelles. The bound O-H stretching mode of water, bonded to DPPC, appeared as a broad band at around 3400 cm-1. The O-H bending mode of this complex appeared as a weak broad band at 1644 cm-1. No free O-H signal was observed. When alcohols were added, a part of DPPC-bound water was replaced by the alcohols. The released 'free' water appeared at 3680 cm-1. This free O-H stretching band represents water-alcohol complex. A new broad band of O-H stretching appeared at 3235 cm-1, which represents the alcohol molecules bound to the phosphate moiety of DPPC. When the alcohol concentration was increased, the intensities of the free O-H stretching and bending bands increased. The P = O- antisymmetric stretching band at 1238 cm-1 became broader and shifted to lower frequencies. This means that alcohols interacted with the phosphate moiety and replaced the bound water. In the deconvoluted spectra of the C = O stretching mode, the ratio between the free sn-2 and the hydrogen-bonded sn-2 bands increased; a part of the bound water at the sn-2 carbon in the glycerol skeleton is also released and the free sn-2 signal increased. From the change in the intensity of the P = O- stretching band, the partition coefficients of alcohols between the phosphate region of DPPC and water were estimated: methanol 7.8, ethanol 16.7 at 22.0 degrees C in mole fraction bases. In molality, these values translates into methanol 0.21 and ethanol 0.45. These results indicate that short-chain alcohols interact with lipid membranes at the phosphate moiety at the hydrophilic head, weaken the membrane-water interaction, and destabilize membranes.     

In vitro preparation and characterization of a 700 nm absorbing chlorophyll-water adduct according to the proposed primary molecular unit in photosynthesis.

1. This study characterized chlorophyll a-H2O adducts in vitro in order to establish their generic relationship to the recently proposed [15, 18-20, 31] primary molecular adduct in photosynthesis. The effects of water titration and temperature on the absorption, fluorescence, excitation, and redox properties of the various in vitro chlorophyll a aggregate species are investigated. 2. From fluorescence measurements, we conclude that the driest chlorophyll a sample contains an equimolar amount of water. This conclusion is consistent with earlier experimental work [2, 3, 14, 17, 31], and clarifies the origin of the controversial [15] Katz model [14] of chlorophyll a-H2O interactions. 3. With increasing water concentration or as the temperature is lowered below room temperature, the A-663 monohydrate chlorophyll a-H2O (species absorbing at 663 nm) is favored at the expense of the A-678 anhydrous aggregate according to the equilibrium 2H2O+chlorophyll a2in equilibrium2 chlorophyll a-H2O. Under excess water conditions, A-663 is converted to A-743 (chlorophyll a-2H2O)n. 4. On slow sample cooling to T less than or approximately 200 degrees K, we observe the growth of A-700 at the expense of A-663. There is a direct correspondence between the increasing (decreasing) absorption by A-700 (A-633) and increasing (decreasing) fluorescence at 720 nm (664 nm). 5. It is concluded that A-700 is most probably the dimer participating in the equilibrium 2 chlorophyll a-H2O in equilibrium (chlorophyll a-H2O)2. The A-700 band consists of two exciton components (separated by approximately 280 cm1) that are interpretable in terms of the dimeric origin of A-700. 6. The deconvoluted A-700 absorption spectrum and the excitation spectrum of the 720 nm fluorescence are compared with the light-minus-dark spectra of P-700. 7. It is found that A-700 is reversibly bleached by I2 (E0 equals 0.54 V). The significance of this observation is discussed in terms of the redox properties of monomeric chlorophyll a and P-700.     

Protein and chlorophyll in photosystem II probed by infrared spectroscopy

The infrared spectra of photosystem II (PS II) enriched submembrane fractions isolated from spinach are obtained in water and in heavy water suspension Other spectra are obtained after a photooxidation reaction was performed on PS II to bleach the pigments. The water bands are removed by computer subtraction and the amide bands (A, B, I, II, and III) of the protein are identified. Computer enhancement techniques are used to narrow the bandwidth of the bands that the weak chlorophyll bands, buried in the much stronger protein bands, can be observed. Comparing the spectra of native and photooxidized PS II pr in water and in heavy water, we determine that three polypeptide domains are present in the native material. The first domain, which contains 22% of th is situated in the peripheral region of the PS II system. The polypeptides in this region are unfolded and devoid of chlorophyll. The second domain con of the polypeptides, is more organized, and contains the chlorophylls. The third domain has an alpha-helix configuration, does not contain chlorophyll, a affected by the photooxidation reaction or by the proton/deuteron exchange. Three different types of chlorophyll organisation are identified: two have carbonyl groups non-bonded, differing from one another only in their hydrophobic milieux; the third is weakly bonded to another unidentified group. Other forms of chlorophyll organisation are present but could not be observed because their absorption is buried in the protein amide I band.     

Energy transfer by chlorophyll beta in detergent micelles.

The concentration-dependent depolarization, concentration-dependent quenching, absorption and fluorescence spectra in solutions of chlorophyll beta-containing detergent micelles with Triton X-100 were studied in a concentration range of c equal to 0.4 muM-0.6mM chlorophyll beta and cd equal to 0.4-7.0 mM Triton X-100. The concentration-dependent depolarization obeys F?rster's theory of depolarization of fluorescence with a transfer distance parameter R0 equal to 43 plus or minus 2 A. The concentration-dependent quenching is described by an empirical formula for the relative fluorescence yield n/n0 equal to 1/[1+(c/c1/2)-2] given by Kelly and Porter (Kelly A. R. and Porter, G. (1970) Proc. R. Soc. Lond. Ser. A. 315, 149-161). With increasing chlorophyll beta concentration the red absorption band at 650 nm is shifted toward a longer wavelength and its width increases by 10nm, the intensity of the long wave fluorescence band increases about 720 nm. The results analysed in terms of these findings lead to the conclusions that chlorophyll beta molecules are (a) locally concentrated in the micelles up to the concentration range of in vivo conditions, (b) partly in an aggregated state capable for fluorescence, (c) the chlorophyll beta yields chlorophyll beta homotransfer may be about 3-26% of the homotransfer chlorophyll alpha yields chlorophyll-alpha depending on the ratio of their concentrations.     

ATR-FTIR study of the structure and orientation of transmembrane domains of the Saccharomyces cerevisiae alpha-mating factor receptor in phospholipids

The structures of seven synthetic transmembrane domains (TMDs) of the alpha-factor receptor (Ste2p) from Saccharomyces cerevisiae were studied in phospholipid multilayers by transmission Fourier transform infrared (FTIR) and attenuated total reflection Fourier transform infrared (ATR-FTIR) spectroscopies. Peptide conformation assumed in multilayers depended on the method of sample preparation. Amide proton H/D exchange experiments showed that 60-80% of the NH bonds in these TMDs did not exchange with bulk water in 1,2-dimyristoyl-sn-glycero-3-phosphocholine (DMPC) multilayers. FTIR results showed that peptides corresponding to TMDs one, two, and seven were mostly alpha-helical in DMPC multilayers. Peptides corresponding to TMDs three and six assumed predominantly beta-sheet structures, whereas those corresponding to TMDs four and five were a mixture of alpha-helices and beta-sheets. ATR-FTIR showed that in DMPC the alpha-helices of TMDs two and five oriented with tilt angles of 34 degrees and 32 degrees, respectively, with respect to the multilayer normal. Similar results were obtained for six of the transmembrane domains in DMPC/DMPG (4:1) multilayers. In a mixture [POPC/POPE/POPS/PI/ergosterol (30:20:5:20:25)] which mimicked the lipid composition of the S. cerevisiae cell membrane, the percentage of alpha-helical structures found for TMDs one and five increased compared to those in DMPC and DMPC/DMPG (4:1) multilayers, and TMD six exhibited a mixture of beta-sheet ( approximately 60%) and alpha-helical ( approximately 40%) structure. These experiments provide biophysical evidence that peptides representing the seven transmembrane domains in Ste2p assume different structures and tilt angles within a membrane multilayer.     

Incorporation of acylated antibody into planar lipid multilayers: characterization and cell binding

Multiple (up to 14) layers of lipid were deposited onto an alkylated glass surface by dialysis of egg phosphatidylcholine (PC) and deoxycholate mixed micelles in the presence of alkylated glass coverslips. The amount of lipid associated with the coverslips was measured by using radioactive PC. It was found that the number of PC molecules in the multilayer increased with increasing initial lipid concentration in the dialysis mixture. Inclusion of cholesterol resulted in a significant increase in the amount of total lipid deposited in the multilayer. However, the PC/cholesterol ratio was up to 2-fold higher in the multilayers than in the liposomes present in the same dialysis bag. In addition, mouse monoclonal anti-H2Kk antibody which had previously been derivatized with palmitic acid could be readily incorporated into the lipid multilayer during dialysis. Measurements of lateral mobility with the fluorescence recovery after photobleaching technique on fluorescently labeled lipid or antibody in the multilayer showed that the lipid molecules diffused rapidly while the antibodies were essentially immobile. Lymphoma cells such as RDM4 cells expressing surface H2Kk glycoproteins could rapidly bind to the antibody-containing multilayers. The binding was blocked by free antibody or by goat anti-mouse immunoglobulin G, indicating the immunospecificity of the binding. Cell binding to the multilayer also exhibited a threshold dependence on the antibody density of the multilayer. A lower threshold was found for cells expressing a higher surface density of H2Kk. This system may be useful for model studies of cellular recognition.     

Time-resolved x-ray diffraction studies of the sarcoplasmic reticulum membrane during active transport.

X-ray and neutron diffraction studies of oriented multilayers of a highly purified fraction of isolated sarcoplasmic reticulum (SR) have previously provided the separate profile structures of the lipid bilayer and the Ca2+-ATPase molecule within the membrane profile to approximately 10-A resolution. These studies used biosynthetically deuterated SR phospholipids incorporated isomorphously into the isolated SR membranes via phospholipid transfer proteins. Time-resolved x-ray diffraction studies of these oriented SR membrane multilayers have detected significant changes in the membrane profile structure associated with phosphorylation of the Ca2+-ATPase within a single turnover of the Ca2+-transport cycle. These studies used the flash photolysis of caged ATP to effectively synchronize the ensemble of Ca2+-ATPase molecules in the multilayer, synchrotron x-radiation to provide 100-500-ms data collection times, and double-beam spectrophotometry to monitor the Ca2+-transport process directly in the oriented SR membrane multilayer.     

Fourier transform infrared spectroscopy of 13C = O-labeled phospholipids hydrogen bonding to carbonyl groups

Fourier transform infrared spectroscopy has been used to characterize the carbonyl stretching vibration of DMPC, DMPE, DMPG, and DMPA, all labeled with 13C at the carbonyl group of the sn-2 chain. Due to the vibrational isotope effect, the 13C = O and the 12C = O vibrational bands are separated by ca. 40-43 cm-1. This frequency difference does not change when the labeling is reversed with the 13C = O group at the sn-1 chain. For lipids in organic solvents possible conformational differences between the sn-1 and sn-2 ester groups have no effect on the vibrational frequency of the C = O groups. In aqueous dispersion unlabeled phospholipids always show a superposition of two bands for the C = O vibration located at ca. 1740 and 1727 cm-1. These two bands have previously been assigned to the sn-1 and sn-2 C = O groups. FT-IR spectra of 13C-labeled phospholipids show that the vibrational bands of both, the sn-1 as well as the sn-2 C = O group, are clearly superpositions of at least two underlying components of different frequency and intensity. Band frequencies were determined by Fourier self-deconvolution and second-derivative spectroscopy. The difference between the component bands is ca. 11-17 cm-1. Again, the conformational effect as shown by reversed labeling is negligible with only 1-2 cm-1. The splitting of the C = O vibrational bands in H2O and D2O is caused by hydrogen bonding of water molecules to both C = O groups as shown by a comparison with spectra of model ester compounds in different solvents. To extract quantitative information about changes in hydration, band profiles were stimulated with Gaussian-Lorentzian functions. The chemical nature of the head group and its electronic charge have distinctive effects on the extent of hydration of the carbonyl groups. In the gel and liquid-crystalline phase of DMPC the sn-2 C = O group is more hydrated than the sn-1 C = O. This is accord with the conformation determined by X-ray analysis. In DMPG the sn-1 C = O group seems to be more accessible to water, indicating a different conformation of the glycerol backbone.     

Synthesis, characterization, cytotoxicity and DNA binding studies of diamminediethyldithiocarbamato-platinum(II) nitrate.

A new complex [Pt(NH3)2(ddtc)]NO3.2H2O as a 1:1 electrolyte has been prepared. This was characterized by spectroscopic methods. The electronic absorption spectrum of this complex in water suggests that it has a square planar geometry. The infrared, 1H NMR and x-ray photoelectron spectroscopic studies suggest the bonding of ammonia molecules and diethyldithiocarbamate as bidentate ligand to platinum(II) in this complex. The 50% inhibition value of this complex against P388 lymphocytic leukemia cells is comparable with cisplatin. This complex interacts with calf thymus DNA by coordinate covalent bond.     

The stratum corneum lipid thermotropic phase behavior.

The stratum corneum, the outermost layer of mammalian skin, is considered the least permeable skin layer to the diffusion of water and other solutes. It is generally accepted that the intercellular lipid multilayer domain is the diffusional pathway for most lipophilic solutes. Fluidization of the lipid multilayers is believed to result in the loss of barrier properties of the stratum corneum. Current investigations address the lipid thermotropic phase behavior in terms of lipid alkyl chain packing, mobility and conformational order as measured by Fourier transform infrared (FTIR) spectroscopy. A solid-solid phase transition is observed with increased alkyl chain mobility followed by a gel to liquid-crystalline phase transition near 65 degrees C. These results further elucidate the role of lipid fluidity that may contribute to the transport properties of the stratum corneum.     

Active internal waters in the bacteriorhodopsin photocycle. A comparative study of the L and M intermediates at room and cryogenic temperatures by infrared spectroscopy

We present time-resolved room-temperature infrared difference spectra for the bacteriorhodopsin (bR) photocycle at 8 cm (-1) spectral and 5 micros temporal resolution, from 4000 to 800 cm (-1). An in situ hydration method allowed for a controlled and stable sample hydration (92% relative humidity), largely improving the quality of the data without affecting the functionality of bR. Experiments in both H 2 (16)O and H 2 (18)O were conducted to assign bands to internal water molecules. Room-temperature difference spectra of the L and M intermediates minus the bR ground state (L-BR and M-BR, respectively) were comprehensively compared with their low-temperature counterparts. The room-temperature M-BR spectrum was almost identical to that obtained at 230 K, except for a continuum band. The continuum band contains water vibrations from this spectral comparison between H 2 (16)O and H 2 (18)O, and no continuum band at 230 K suggests that the protein/solvent dynamics are insufficient for deprotonation of the water cluster. On the other hand, an intense positive broadband in the low-temperature L-BR spectrum (170 K) assigned to the formation of a water cavity in the cytoplasmic domain is absent at room temperature. This water cavity, proposed to be an essential feature for the formation of L, seems now to be a low-temperature artifact caused by restricted protein dynamics at 170 K. The observed differences between low- and room-temperature FTIR spectra are further discussed in light of previously reported dynamic transitions in bR. Finally, we show that the kinetics of the transient heat relaxation of bR after photoexcitation proceeds as a thermal diffusion process, uncorrelated with the photocycle itself.     

Inhibition of nuclease activity in Bacillus subtilis following infection with bacteriophage SP82G.

The Raman Spectra of Blodgett-Langmuir multilayer assemblies made from behenic acid, barium behenate and barium cis-13 erucate are reported. In particular, the peak height intensity ratio of the hydrocarbon chain methylene CH stretch Raman bands, $\text{I}{}_{2890}\text{I}{}_{2850}$, for each multilayer assembly is compared to that of phosphatidylcholine in powders and water dispersions as well as to samples of crystalline hydrocarbon chains. It is found that the fatty acid multilayers are more ordered than the phospholipid samples but less ordered than the crystalline samples. It is suggested that Blodgett-Langmuir multilayer assemblies of lipid might be a useful reference in quantitative studies of packing order in lipid phases.     

Layer-by-layer assembly of multilayer films composed of avidin and biotin-labeled antibody for immunosensing

Protein multilayers composed of avidin and biotin-labeled antibody (bio-Ab) were prepared on gold surface by layer-by-layer assembly technology using the high specific binding constant (K(a): approximately 10(15) M(-1)) between avidin and biotin. The assembly process of the multilayer films was monitored by using real-time BIA technique based on surface plasmon resonance (SPR). The multilayer films were also characterized by electrochemical impedance spectroscopy (EIS) and reflection absorption Fourier transform infrared spectroscopy (FTIR). The results indicate that the growth of the multilayer is uniform. From response of SPR for each layer, the stoichiometry S for the interaction between avidin and bio-Ab is calculated to be 0.37 in the multilayer whereas 0.82 in the first layer. The protein mass concentration for each layer was also obtained. The schematic figure for the multilayer assembly was proposed according to the layer mass concentration and S value. The utility of the mutilayer films for immunosensing has been investigated via their subsequent interaction with hIgG. The binding ability of the multilayer increased for one to three layers of antibody, and then reach saturation after the fourth layer. These layer-by-layer constructed antibody multilayers enhance the binding ability than covalently immobilized monolayer antibody. This technology can be also used for construction of other thin films for immunosensing and biosensor.     

Interaction of metal ions with humic-like models. Part VII. Mn(II), Co(II), Ni(II), Cu(II), Zn(II) and Cd(II) complexes of 2,5-dihydroxybenzoic acid

Complexes of formula M(2,5-DHB)₂4H₂O (M = Mn, Co, Ni, Zn, Cu and Cd; 2,5-DHB = 2,5-dihydroxybenzoate) were prepared and characterized by means of infrared and electronic spectroscopy, and by electron spin resonance. For the Zn complex the crystal and molecular structure was also determined by single-crystal X-ray diffraction analysis. The crystal is orthorhombic, space group Pbca (No. 61), with a = 18.503(4), b = 13.536(3), c = 6.900(2) Å, and Z = 4. The final refinement used 877 reflections and gave a residual R value of 0.041. The complex has slightly compressed octahedral coordination, with the zinc atom bound to two monodentate carboxylate groups lying in trans positions and four water molecules. X-ray data and infrared spectra show the Mn, Co, Ni, Zn and Cd complexes to be isostructural with the Zn compound. The electronic, infrared and ESR spectra of the copper(II) complex are consistent with a CuO_4? based chromophore involving two water molecules and two monodentate carboxylate groups in the metal plane, and long axial contacts.