Structure and electronic absorption spectra of nematogenic alkoxycinnamic acids - a comparative study based on semiempirical and DFT methods

Structure of nematogenic p-n-Alkoxy cinnamic acids (nOCAC) with various alkyl chain carbon atoms (n = 2, 4, 6, 8) has been optimized using density functional B3LYP with 6-31+G (d) basis set using crystallographic geometry as input. Using the optimized geometry, electronic structure of the molecules has been evaluated using the semiempirical methods and DFT calculations. Molecular charge distribution and phase stability of these systems have been analyzed based on Mulliken and L?wdin population analysis. The electronic absorption spectra of nOCAC molecules have been simulated by employing DFT method, semiempirical CNDO/S and INDO/S parameterizations. Two types of calculations have been performed for model systems containing single and double molecules of nOCAC. UV-Visible spectra have been calculated for all single molecules. The UV stability of the molecules has been discussed in light of the electronic transition oscillator strength (f). The dimer complexes of higher homologues (n = 6, 8) have also been reported to enable the comparison between single and double molecules.     

Electronic absorption spectroscopy and time-dependent density functional theory calculations on the nickel(II) complex of 1,4-bis(pyrrol-2-ylmethyleneamino)butane

The electronic structure of the 1,4-bis(pyrrol-2-ylmethyleneamino)butane nickel(II) complex has been studied using electronic absorption spectroscopy and density functional theory (DFT) calculations. The DFT optimised structure is in excellent agreement with the X-ray crystal structure of the complex and time-dependent DFT calculations have been used to probe the nature of the transitions observed in the electronic absorption spectrum.     

The fine structure of luminescence spectra of azurin.

The spectra of azurin absorption, fluorescence, phosphorescence and fluorescence excitation have been measured in aqueous solutions at ordinary and liquid nitrogen temperatures. The fluorescence spectra of azurin even at ordinary temperatures have a well resolved fine vibrational structure. The frequency analysis reveals practically the same wave number distances between the main structure peaks in fluorescence spectra at room and low temperatures and in phosphorescence spectra. The comparison of the protein absorption and excitation spectra shows that all the energy absorbed by tyrosine residues is transferred onto indole chromophore. These data suggest an unusual tryptophan environment in this protein, which is characterized by the absence of any hydrogen bonding or other polar interaction of tryptophan with its environment. The problem of the possibility of contributions of two electronic transitions (1La in equilibrium A and 1Lb in equilibrium A) in absorption and emission spectra of azurin tryptophan arising from their mirror symmetry is discussed.     

Hydrophobic acridine dyes for fluorescence staining of mitochondria in living cells. 1.Thermodynamic and spectroscopic properties of 10-n-alkylacridine orange chlorides

10-n-Alkyl-acridine-orange-chlorides (alkyl-AOs) are excellent dyes for fluorescence staining of mitochondria in living cells. The thermodynamic and spectroscopic properties of the series alkyl = methyl to nonyl have been investigated. The dyes form dimers in aqueous solution. The dimerisation is mainly a consequence of the hydrophobic interaction. The dissociation constant K respectively association constant K-1 of the dimers describes the hydrophobic interaction and therefore the hydrophobic properties of the dye cations. The dissociation constant K = K0 at the standard temperature T = 298 K has been determined spectroscopically in aqueous solution. It depends on the length of the alkyl residue n-CmH2m + 1 (m = 1 - 9) (Table 2). In addition the standard dissociation enthalpies (energies) delta H0 and dissociation entropies delta S0 have been determined from the temperature dependence of K (Table 2). With increasing chain length m the thermodynamic parameters K0, delta H0, delta S0 decrease. Therefore with growing m the dimers are stabilized. This stabilization is an entropic effect which is diminished by the energetic effect. The change of the thermodynamic parameters with m is in agreement with the concept of hydrophobic interaction and the stabilization of water structure in the surroundings of hydrophobic residues. As one would expect nonyl-AO is the most hydrophobic dye of the series. As an example the spectroscopic properties of nonyl-AO have been determined. We measured the absorption, luminescence and polarization spectra in rigid ethanol at 77 K. Under these conditions alkyl-AOs associate like dyes in Water at room temperature. The spectra depend on the concentration of the solution. In very dilute solution we observe mainly the spectra of the monomers M, in concentrated solution the spectra of the dimers D. The spectra of M and D are characteristically different. The monomers have one long wave length absorption M1 = 20.000 cm-1 with resonance fluorescence. In addition there is a long living phosphorescence at 16.600 cm-1. Its polarization is nearly perpendicular to the plane of the AO residue. The dimers have two long wave length absorption bands D1 = 18.700 and D2 = 21.200 cm-1 with very different intensities. D1 has very low intensity and is forbitten, D2 is allowed. D1 shows fluorescence. Phosphorescence has not been observed. D1, D2 and also M1 are polarized in the plane of the AO residue. At short wave length absorption and polarization spectra are very similar. From the spectra we constructed the energy level diagram of M and D (Fig. 9). The first excited state of M splits in D in two levels. The level splitting and the transition i     

The effect of anchoring group number on molecular structures and absorption spectra of triphenylamine sensitizers: a computational study

The molecular structures and absorption spectra of triphenylamine dyes containing different numbers of anchoring groups (S1-S3) were investigated by density functional theory (DFT) and time-dependent DFT. The calculated geometries indicate that strong conjugation is formed in the dyes. The interfacial charge transfer between the TiO₂ electrode and S1-S3 are electron injection processes from the excited dyes to the semiconductor conduction band. The simulated absorption bands are assigned to π → π* transitions according to the qualitative agreement between the experimental and calculated results. The effect of anchoring group number on the molecular structures, absorption spectra and photovoltaic performance were comparatively discussed.     

Electronic spectra and fluorescence properties of multichromophoric sulfonylureas

The multichromophoric character of two sulfonylurea herbicides, SMT and BNS, has been investigated in its manifestations in the electronic absorption spectra and in some fluorescence properties through a combined experimental and theoretical approach. After a theoretical analysis of the most stable structures of these flexible systems, the UV absorption spectra of the two multichromophoric compounds have been analysed both experimentally and theoretically, and most transitions have been assigned to individual chromophores, also by comparison with four suitable reference compounds (5-8). Finally, some experimental information concerning the fluorescence spectra and quantum yields have been analysed with reference to the contributions from single fluorophores and the role of low-lying n → π^∗ states.     

Ethanol inhibits leptin-induced STAT3 activation in Huh7 cells

The manganese (Mn) complex of photosystem II catalyzes water oxidation. For the first time, its advancement through the reaction cycle was monitored by time-resolved X-ray absorption measurements at the Mn K-edge at room temperature. The complex was stepped through its four oxidation states by nano-second-laser flashes applied to samples exposed to the X-ray beam. Time courses of the X-ray fluorescence intensity were recorded during a flash sequence. Extended X-ray absorption fine-structure spectra were recorded with the S(1), S(2), and S(3) oxidation states highly populated. The room temperature data is compatible with the formation of a third di-mu-oxo bridge between two Mn atoms upon the S(2)-->S(3) transition.     

Photophysics of pyrene-labelled compounds of biophysical interest.

The effects of the chemical constitution and structure of the substituent on the excited state dynamics of several model fluorescent pyrene-labelled molecules of biophysical interest have been examined. Nine new 1-substituted pyrenyl compounds, Py-NH-CO-C2H5, Py-NH-CO-Leu-Boc, Py-CH2-NH-CO-C2H5, Py-CH2-NH-CO-Leu-Boc, Py-CO-NH-C3H7, Py-CO-NH-Leu-OMe, Py-CH2-CO-NH-C3H7, Py-CH2-CO-NH-Leu-OMe and Py-C3H6-CO-NH-Leu-OMe, have been synthesized and their electronic spectra, fluorescence quantum yields and excited state lifetimes measured. These data have been used to calculate the radiative, kr, and non-radiative decay constants of their S1 states and the values of these constants correlated with the structures of the tethers. Non-radiative S1 decay rates (mainly intersystem crossing to T1) vary in parallel with the radiative rates so that the excited state lifetimes and radiative rate constants change considerably with the structure of the substituent whereas the quantum yields of fluorescence do not. An excellent correlation between [epsilon]max of the S1-S0 transition and either kr or the excited state lifetime is observed as long as no additional intermolecular or intramolecular excited state decay process of significant rate competes with the 'normal' radiative and non-radiative (ISC) decay processes of the pyrenyl chromophore. This correlation may have predictive value. Rates of bimolecular quenching of the S1 states of these molecules by molecular oxygen have been measured. The quenching process is diffusion-controlled with a spin statistical factor of 1, indicating that the S1-T1 electronic energy spacings of all the derivatives exceed the O2(1Deltag-3Sigmag-) electronic excitation energy of ca. 1 eV.     

Interpreting the visible absorption bands of 1,4-(dihydroxy)-9,10-anthraquinone and its metal chelates

The visible absorption spectra of 1,4-(dihydroxy)-9,10-anthraquinone and of Co(II), Ni(II), Cu(II) and Zn(II) chelates have been studied in different organic solvents. This system provides a model for the anthracycline antibiotics and their metal chelates. The band structure of the spectrum has been determined using the second and fourth derivatives of the spectrum. The visible absorption band of the parent molecule can be assigned to a single electronic state with a reduced dipole moment in the excited state; structure in this band is ascribed to two overlapping vibrational progressions. In contrast, the dianion (hydroxy protons removed) shows a single electronic state with an increased dipole moment in the excited state; structure in this band can be assigned to a single vibrational progression. All of the metal chelates show spectra which are similar in appearance to that of the dianion although the identity of the metal determines the bathochromic shift of the absorption band. Titration of 1,4-dihydroxyanthraquinone with Cu(ClO4)2.6H2O demonstrates that three chelates with metal-to-ligand ratios of 1:2, 1:1 and 2:1 can form depending on the identity of the metal, ratio of metal to ligand, and donor character of the solvent.     

Effects of solvent polarity on the absorption and fluorescence spectra of chlorogenic acid and caffeic acid compounds: determination of the dipole moments

The effects of solvent polarity on absorption and fluorescence spectra of biologically active compounds (chlorogenic acid (CGA) and caffeic acids (CA)) have been investigated. In both spectra pronounced solvatochromic effects were observed with shift of emission peaks larger than the corresponding UV‐vis electronic absorption spectra. From solvatochromic theory the ground and excited‐state dipole moments were determined experimentally and theoretically. The differences between the excited and ground state dipole moment determined by Bakhshiev, Kawski–Chamma–Viallet and Reichardt equations are quite similar. The ground and excited‐state dipole moments were determined by theoretical quantum chemical calculation using density function theory (DFT) method (Gaussian 09) and were also similar to the experimental results. The HOMO‐LUMO energy band gaps for CGA and CFA were calculated and found to be 4.1119 and 1.8732 eV respectively. The results also indicated the CGA molecule is more stable than that of CFA. It was also observed that in both compounds the excited state possesses a higher dipole moment than that of the ground state. This confirms that the excited state of the hydroxycinnamic compounds is more polarized than that of the ground state and therefore is more sensitive to the solvent. Copyright © 2015 John Wiley & Sons, Ltd.     

Systematic investigation of interactions between papain and MPA-capped CdTe quantum dots

Fluorescent quantum dots (QDs) have been widely applied in biological and biomedical areas, but relatively little is known about the interaction of QDs with some natural enzymes. Herein, the interactions between 3-mercaptopropionic acid-capped CdTe QDs (MPA-QDs) and papain were systematically investigated by UV–Vis absorption spectra, fluorescence spectra and circular dichroism (CD) spectra under the physiological conditions. The fluorescence spectra results indicated that MPA-QDs quenched the fluorescence intensity of papain. The modified Stern–Volmer quenching constant K _a at different temperatures and the corresponding thermodynamic parameters ΔH, ΔG and ΔS were also calculated. The binding of MPA-QDs and papain is a result of the formation of QDs-papain complex and the electrostatic interactions play a major role in stabilizing the complex. The CD technique was further used to analyze the conformational changes of papain induced by MPA-QDs and the results indicated that the biological activity of papain was affected by MPA-QDs dramatically.     

Mechanism of nonphotochemical quenching in green plants: energies of the lowest excited singlet states of violaxanthin and zeaxanthin

The xanthophyll cycle is an enzymatic, reversible process through which the carotenoids violaxanthin, antheraxanthin, and zeaxanthin are interconverted in response to the need to balance light absorption with the capacity to use the energy to drive the reactions of photosynthesis. The cycle is thought to be one of the main avenues for safely dissipating excitation energy absorbed by plants in excess of that needed for photosynthesis. One of the key factors needed to elucidate the molecular mechanism by which the potentially damaging excess energy is dissipated is the energy of the lowest excited singlet (S(1)) state of the xanthophyll pigments. Absorption from the ground state (S(0)) to S(1) is forbidden by symmetry, making a determination of the S(1) state energies of these molecules by absorption spectroscopy very difficult. Fluorescence spectroscopy is potentially the most direct method for obtaining the S(1) state energies. However, because of problems with sample purity, low emission quantum yields, and detection sensitivity, fluorescence spectra from these molecules, until now, have never been reported. In this work these technical obstacles have been overcome, and S(1) --> S(0) fluorescence spectra of violaxanthin and zeaxanthin are presented. The energies of the S(1) states deduced from the fluorescence spectra are 14 880 +/- 90 cm(-)(1) for violaxanthin and 14 550 +/- 90 cm(-)(1) for zeaxanthin. The results provide important insights into the mechanism of nonphotochemical dissipation of excess energy in plants.     

Characteristics of the tertiary structure of histone H1 from the calf thymus

By optical methods it has been previously shown that the globular "head" of histone H1 forms a hydrophobic cavity containing Tyr72. The latter is screened from the polar water surrounding and its intramolecular mobility is drastically hindered. As a consequence of the alteration in the micromilieu are a long wave shift (lambda max = 279,5 nm) and a more pronounced longwave absorption spectra, higher anisotropy (A = 0,11), augmented quantum yield of fluorescence (approximately 0,2) and a decrease of the Stern-Volmer constant for Hl at fluorescence quenching by acrylamide. It was found that changes in fluorescence intensity of histones are connected with alterations in the quantum yield of fluorescence at lambda exc = = 265 nm, but not at lambda exc = 280 nm. The changes in fluorescence intensity at light excitation 280 nm (F280) and 265 nm (F265) are in good accordance with shift delta E286 in differential absorption spectra. Introduction of parameter Cf = F280/F265 allows to study shifts of excitation spectra instead of shifts in absorption spectra of histones. This method has certain advantages, since it permits investigations with lower protein concentrations and in turbid solutions. The data obtained allow to draw out Tyr72 of histone Hl into a special class of fluorescent-tyrosyls, that differ in properties from those of other tryptophandevoided proteins: RNAse, insulin and core-histones H2A, H2B, H3 and H4.     

Intrinsic fluorescence, difference spectrophotometry and theoretical studies on tertiary structure of calf thymus histone H1

Tyr-72 is included in the hydrophobic cleft which is formed in the histone H1 globular head. Tyr-72 is screened against polar aqueous environment and its intramolecular mobility is sharply retarded. This microenvironment causes a red shift (lambda max = 279 nm) and a sharpening of the longer wavelength shoulder of absorption spectra, a high fluoresence anisotropy value (A = 0,11), high quantum yield of fluoresence (approximately 0.2) and a decrease of the Stern-Volmer Constant during quenching of histone H1 fluorescence by acrylamide. It has been found that the change in the intensity of histone fluorescence at lambda excit = 265 nm, but not at lambda excit = 280 nm, is due to the changes in the quantum yield of fluorescence. The increase of fluorescence intensity at lambda excit = 280 nm depends on the changes in the quantum yield and molar extinction coefficient of histone H1 tyrosyl chromophore. The change in the ratio of fluorescence intensity exited at 280 nm (F280) to the fluorescence intensity excited at 265 nm (F265) corresponds to the change of delta epsilon 286 in difference absorption spectra. The introduction of the parameter Cf = F280/F265 allows one to go over to studying excitation spectrum shifts instead of histone absorption spectrum shifts, which is much more convenient methodologically since in this case it is possible to carry out research using lower protein concentrations and turbid solutions. The results make it possible to designate Tyr-72 of histone H1 as a special class of fluorescent tyrosyls whose properties differ from those of tyrosyls of other tryptophane-free proteins: RNAase, insulin, core histones--H2A, H2B, H3, H4 and some others.     

Characterization of the myricetin-human serum albumin complex by spectroscopic and molecular modeling approaches

The interaction mechanism of flavonol myricetin (3,5,7,3',4',5'-hexahydroxyflavone) and human serum albumin (HSA) has been characterized by fluorescence, electronic absorption, and Fourier transform infrared (FT-IR) spectroscopic approaches and the molecular modeling method. The structural characteristics of myricetin and HSA were probed, and their binding affinities were determined under different pH conditions. The results showed that the binding abilities of the drug to protein decreased under lower pH conditions (pH 3.5 and 2.0) due to the alterations of the protein secondary and tertiary structures. The second derivative absorption spectra of myricetin after interacting with the protein showed that the drug existed as an anion form in the binding pocket. The fluorescence emission intensities of the normal and excited-state proton transfer (ESTP) tautomer of myricetin significantly enhanced in the presence of HSA with conspicuous shifts of the emission bands when excited with a wavelength of 370 nm, while the intensity ratios of the normal to ESTP tautomers rose rapidly with the increase of the HSA concentrations under different pH environments. This illustrated that the fluorescence emission of the normal tautomer (S1-S0, non-proton-transferred) predominated due to the interaction of drug and surrounding polar and ionic side chains of amino acid residues in the binding cavity. The similar spectroscopic properties of myricetin-HSA complex at pH 7.4 and 3.5 showed that the drug was located in subdomain IIA of the protein in the vicinity of the single Trp 214 because of the unfolding of the protein domain III in its F state. From the molecular modeling results, the drug-protein complex was stabilized by electrostatic force and hydrogen bonding with the amino acid residue in the binding pocket, which was consistent with the experimental results.     

Experimental and quantum chemical calculational studies on 2-[(4-Fluorophenylimino)methyl]-3,5-dimethoxyphenol

The Schiff base compound, 2-[(4-Fluorophenylimino)methyl]-3,5-dimethoxyphenol, has been synthesized and characterized by IR, electronic spectroscopy, and X-ray single-crystal determination. Molecular geometry from X-ray experiment of the title compound in the ground state have been compared using the Hartree-Fock (HF) and density functional method (B3LYP) with 6–31G(d) basis set. Calculated results show that density functional theory (DFT) and HF can well reproduce the structure of the title compound. The energetic behavior of the title compound in solvent media has been examined using B3LYP method with the 6–31G(d) basis set by applying the polarizable continuum model (PCM). The total energy of the title compound decrease with the increasing polarity of the solvent. By using TD-DFT and TD-HF methods, electronic absorption spectra of the title compound have been predicted and a good agreement with the TD-DFT method and the experimental ones is determined. In addition, DFT calculations of the title compound, molecular electrostatic potential (MEP), natural bond orbital (NBO), and thermodynamic properties were performed at B3LYP/6–31G(d) level of theory.     

Donor-substituted phenyl-pi-chromones: electrochemiluminescence and intriguing electronic properties.

Phenylethynylchromones bearing different donor groups at the phenyl moiety have been prepared and their photophysical and electrogenerated chemiluminescence (ECL) properties have been studied with respect to their structural features. Intriguingly, the presence and variation of donor groups do not much influence the absorption spectra, which can be compared with the spectrum of unsubstituted chromone, whereas the photoluminescence (PL) spectra show pronounced changes. Density functional theory (DFT) calculations indicate enhancement of HOMO energy levels upon increasing the donor strength. The photophysical properties have also been studied in various solvents, and the PL spectra in particular show the anticipated trend. The introduction of pi-extension imparts ECL to the new molecules and the electronic coupling between the donor and the acceptor moieties through C-C triple bond influences ECL emission maxima. Weaker donors impart excimer ECL while stronger donors impart monomeric intramolecular charge transfer (ICT) ECL.     

Photochemistry of 2-acyloxycarbazoles. A potential tool in the synthesis of carbazole alkaloids.

The photochemistry of two 2-acyloxycarbazoles, 2-acetyl- and 2-benzoyloxycarbazole, in different solvents has been studied. Irradiation of the 2-acyloxycarbazoles in organic media at 254 or 313 nm yields the [1,3]-migrated photoproducts, 1-acyl-2-hydroxycarbazole, 3-acyl-2-hydroxycarbazole and 2-hydroxycarbazole. The effects of the solvent, the atmosphere and the intensity of the light source on the photochemistry of 2-acyloxycarbazole have been studied. Laser flash photolysis as well as photosensitization experiments were performed in order to determine the photoreactive excited state. Electronic spectra (absorption, fluorescence and phosphorescence emission spectra) of the 2-acyloxycarbazoles have been recorded in homogeneous media at 298 K and in solid matrices at 77 K. The dynamic properties of the lowest singlet excited state in terms of fluorescence lifetime and fluorescence quantum yield have been measured in different organic solvents at room temperature. The photo-Fries rearrangement as a mild and clean one-pot reaction for the preparation of an advanced intermediate precursor in the total synthesis of carbazole alkaloids is described.     

Structure and dynamics of condensed DNA probed by 1,1'-(4,4,8,8-tetramethyl-4,8-diazaundecamethylene)bis[4-[[3- methylbenz-1,3-oxazol-2-yl]methylidine]-1,4-dihydroquinolinium] tetraiodide fluorescence

Information on the structure and dynamics of condensed forms of DNA is important in understanding both natural situations such as DNA packaging and artificial systems such as gene delivery complexes. We have established the fluorescence of bisintercalator 1,1'-(4,4,8,8-tetramethyl-4,8-diazaundecamethylene)bis[4-[[3-methylbenz-1,3-oxazol-2-yl]methylidine]-1,4-dihydroquinolinium] tetraiodide (YOYO-1) as a novel probe for DNA condensation. When the level of DNA-bound YOYO-1 is sufficiently large, condensation by either polyethylenimine (PEI) or the cationic detergent cetyltrimethylammonium bromide (CTAB) leads to electronic interaction among YOYO-1 molecules bound on the same DNA molecule. This interaction results in an excitonic blue shift of the absorption spectra of YOYO-1 and dramatic decrease in the fluorescence quantum yield. These observations constitute a signature of the condensation of DNA. We further examined the comparative properties of DNA condensed by PEI, CTAB, or Co(NH(3))(6)(3+) through the steady-state and dynamic fluorescence of YOYO-1. Condensation by either PEI or CTAB was associated with a blue shift in the absorption spectra of YOYO-1, although the magnitude of the shift was larger in the case of PEI when compared to that of CTAB. In contrast, condensation by Co(NH(3))(6)(3+) was not associated with a measurable shift in the absorption spectra. These results were interpreted as signifying the varying level of compactness of the DNA condensates. Quenching of fluorescence by acrylamide showed that condensation by all three agents led to an increase in the level of solvent exposure of the base pairs. Observation of the decay of fluorescence intensity and anisotropy of DNA-bound YOYO-1 showed that while condensation by either PEI or CTAB froze the segmental mobility of the helix, condensation by Co(NH(3))(6)(3+) enhanced the flexibility of DNA. The relevance of our findings to functions such as efficiency of gene delivery is discussed.