Different level of fluorescence in Raman spectra of montmorillonites

The paper presents the study of selected montmorillonite standards by Raman spectroscopy and microscopy supported by elemental analysis, X-ray powder diffraction analysis and thermal analysis. Dispersive Raman spectroscopy with excitation lasers of 532 nm and 780 nm, dispersive Raman microscopy with excitation laser of 532 nm and 100× magnifying lens, and Fourier Transform-Raman spectroscopy with excitation laser of 1064 nm were used for the analysis of four montmorillonites (Kunipia-F, SWy-2, STx-1b and SAz-2). These mineral standards differed mainly in the type of interlayer cation and substitution of octahedral aluminium by magnesium or iron. A comparison of measured Raman spectra of montmorillonite with regard to their level of fluorescence and the presence of characteristic spectral bands was carried out. Almost all measured spectra of montmorillonites were significantly affected by fluorescence and only one sample was influenced by fluorescence slightly or not at all. In the spectra of tested montmorillonites, several characteristic Raman bands were found. The most intensive band at 96 cm⁻¹ belongs to deformation vibrations of interlayer cations. The band at 200 cm⁻¹ corresponds to deformation vibrations of the AlO₆ octahedron and at 710 cm⁻¹ can be assigned to deformation vibrations of the SiO₄ tetrahedron. The band at 3620 cm⁻¹ corresponds to the stretching vibration of structural OH groups in montmorillonites.     

Theoretical considerations of the electronic spectra of methyl flavins

Methyl groups in flavins are best treated by the group-orbital approximation. The pseudo-heteroatom approximation overestimates methyl hyperconjugation with the Pariser–Parr–Pople SCF –MO method. Singlet π → π* transition energies are calculated by various MO methods with differing degrees of sophistication, and the results from the P ? P ? P method agree reasonably with the experimental values. 2- and 4-thioflavin analogs are also treated satisfactorily. The effects of position and number of the methyl groups on the spectra of flavins are described in detail. Rough estimates of the n → π* energies of flavins suggest that the lowest singlet excited state is (π, π*), consistent with the fluorescence and phosphorescence polarization data.     

Matching fluorescence spectra of oil spills with spectra from suspect sources

Fluorescence spectroscopy is ideally suited to the analysis of oil spills as it allows chemical information of polycyclic aromatic hydrocarbons to be acquired quickly, sensitively and selectively. Unlike infrared spectra which have detailed peak information, many fluorescence spectra have only a few broad peaks. Nine different samples of crude and diesel oils were used for testing point-to-point matching across the spectral range. Five of them were discriminated by point-to-point matching algorithms and the other four very similar samples were not. Principal components analysis (PCA) did successfully discriminate among all similar samples. PCA could also distinguish the extent of weathering of different samples, an important factor in matching environmental spills.     

Raman spectra phthalocyanines

Raman spectra of amorphous phthalocyanine thin films have been studied. Theoretical and experimental correlations in polarization ratios are applied to vibrational assignments of symmetry species and to the problem of molecular orientation in thin solid films.     

Absorption,fluorescence and resonance Raman spectra of adriamycin and its complex with DNA

Absorption, fluorescence and resonance Raman spectra of adriamycin and of its complex with DNA have been measured. These results together with the analysis of the excitation profiles of the solid drug were used to interpret the complex pattern of the absorption spectra as due to the vibronic structure of a single electronic state. In addition a surplus band, depending on the concentration, was attributed to self-association.Further support was given for the intercalation nature of the drug-DNA complex. In particular it was found that the monomer form of adriamycin interacts with the nucleic acid and that interaction involves the whole chromophore framework.     

Resonance Raman spectra of n-methylthioacetamide

Rigorous resonance, as well as preresonance Raman spectra of N-methylthioacetamide and its N-deuterated compound are reported. The observed selectivity in the resonance intensity enhancement is discussed in relation to the potential energy distributions obtained by normal coordinate treatment. The structural change concerning the CN and CS bond lengths is suggested to accompany the π^* ← π electronic excitation.     

Raman spectra of gases: XIV. Hexachlorodisiloxane

The Raman spectra (50–1200 cm^?1) of gaseous, liquid, and solid (Cl₃Si)₂O have been recorded. The infrared spectra of the gas and solid have been recorded from 55–2000 cm^?1 . The spectra of the gas have been interpreted in detail on the basis of C_2v symmetry with the A₁ skeletal Si-O-Si bend assigned at 63 cm^?1. The spectra gave evidence that there are structural changes upon condensation of the gas and the Si-O-Si angle approaches linearity in the solid state. The opening of this angle is probably due to crystal packing factors.     

Raman spectra of inorganic ions

This paper contains the Raman spectra of 79 inorganic salts and sulphur which may be used as an aid in qualitative inorganic analyses. These were obtained some years ago by conventional Raman spectroscopy. No such collection exists and the order of the reference spectra is identical to those in a collection of IR spectra. A table of characteristic frequencies for 17 polyatomic ions is given. These data have increased relevance following the emergence of FT-Raman as a rapid and efficient modern technique.     

The Raman spectra of bromoform

In this work the Raman spectrum of bromoform is recorded at various temperatures in the pure compound and in solution in carbon tetrachloride and the features shown by some of the bands are considered in the light of previous spectroscopic data interpretations. In particular, the concentration dependent effects exhibited by the ν₅(e) vibrational mode suggest, by comparison with similar effects previously observed in chloroform and trichloromethyl fluoride, the existence, in the pure liquid at room temperature, of important intermolecular interactions.     

Raman spectra of some terpenes

Summary Investigation of Raman spectra indicates increase in the interaction between the double bonds as we pass from sylvestrene and isosylvestrene to sylveterpinolene and indicates that the character of the interaction in the last compound is more complex than in 1,3-butadiene and other similar conjugated systems.     

Raman spectra of titanium dioxide

First-order Raman spectra have been recorded at room temperature for the anatase and rutile phases of polycrystalline titanium dioxide using an argon ion laser as exciter. The high-temperature rutile phase was found to be stabilized at temperatures below 450°C. Anatase transforms to rutile phase at ～750°C. All the Raman active fundamentals predicted by group theory are observed.     

Raman spectra of chlorophyll forms

The Raman spectra of chlorophyll a (Chl) forms in aqueous poly(vinyl alcohol) (PVA) and in dimethyl sulfoxide (DMSO)—water mixtures were recorded at 457.9 nm excitation and their structures were characterized by comparison with the spectra of the following well-known chlorophyll forms: (1) monomers (Chl)₁ in the polar solvents of group (A), i.e., diethyl ether, tetrahydrofuran, acetone, N,N-dimethylformamide and DMSO, of which the oxygen atom is expected to coordinate to the central magnesium atom; (2) monomers (Chl)₁ in the polar solvents of group (B), i.e., methanol, ethanol, 1-propanol, 2-propanol and 1-butanol, which are supposed to form a hydrogen-bond to the C₉=O group in addition to the coordination-bond to the Mg atom; (3) dehydrated aggregates (Chl)_n in dry non-polar solvents, i.e., carbon tetrachloride, n-hexane and n-octane; and (4) hydrated aggregates (Chl·2H₂O)_n in wet non-polar solvents, i.e., n-hexane and n-octane. The frequency of the C₉ = O stretching Raman line of each of the above chlorophyll forms was: (1) 1702—1680 cm⁻¹; (2) 1673—1668 cm⁻¹; (3) around 1655 cm⁻¹; (4) around 1645 cm⁻¹. The frequency proved to be a marker of intermolecular interaction of the Chl molecules. The spectral patterns in the 1650—700 cm⁻¹ region of (1), (2) and (3) were similar. However, the relative intensities of Raman lines of (4), which was ascribed to a one-dimensional, regular stacking of the Chl macrocycles, were quite different from those of (1)—(3).The chlorophyll form in PVA aqueous solution was identified as (Chl·2H₂O)_n by spectral comparison. The chlorophyll forms present in the DMSO—water mixtures were highly dependent on the DMSO content. It is suggested that (Chl)₁ having hydrogen-bonded H₂O should be present in 10% DMSO solution, and that a new chlorophyll form (Chl·DMSO)_n having (a) a stoichiometric intermolecular interaction with DMSO and (b) a regular stacking of the chlorophyll macrocycles, should be predominant in 50% DMSO aqueous solution.     

Evidence from action and fluorescence spectra that UV-induced violet-blue-green fluorescence enhances leaf photosynthesis

We assessed the contribution of UV-induced violet-blue-green leaf fluorescence to photosynthesis in Poa annua, Sorghum halepense and Nerium oleander by measuring UV-induced fluorescence spectra (280-380 nm excitation, 400-550 nm emission) from leaf surfaces and determining the monochromatic UV action spectra for leaf photosynthetic O2-evolution. Peak fluorescence emission wavelengths from leaf surfaces ranged from violet (408 nm) to blue (448 nm), while excitation peaks for these maxima ranged from 333 to 344 nm. Action spectra were developed by supplementing monochromatic radiation from 280 to 440 nm, in 20 nm increments, to a visible nonsaturating background of 500 mumol m-2 s-1 photosynthetically active radiation and measuring photosynthetic O2-evolution rates. Photosynthetic rates tended to be higher with the 340 nm supplement than with higher or lower wavelength UV supplements. Comparing photosynthetic rates with the 340 nm supplement to those with the 400 nm supplement, the percentage enhancement in photosynthetic rates at 340 nm ranged from 7.8 to 9.8%. We suspect that 340 nm UV improves photosynthetic rates via fluorescence that provides violet-blue-green photons for photosynthetic energy conversion because (1) the peak excitation wavelength (340 nm) for violet-blue-green fluorescence from leaves was also the most effective UV wavelength at enhancing photosynthetic rates, and (2) the magnitude of photosynthetic enhancements attributable to supplemental 340 nm UV was well correlated (R2 = 0.90) with the apparent intensity of 340 nm UV-induced violet-blue-green fluorescence emission from leaves.     

Photophysics on surfaces: determination of absolute fluorescence quantum yields from reflectance spectra

A method for the calculation of absolute fluorescence quantum yields for dyes attached to solid particles based on reflectance measurements is reported. The same procedure allows calculation of true reflectance spectra (free of fluorescence) for highly fluorescent materials as well. Samples ofcresyl violet were immobilized by adsorption on microgranular cellulose in the concentration range 4.5 x 10(-9) to 3.8 x 10(-6) mol g(-1). Diffuse and total reflectance spectra were recorded with and without insertion of an optical absorption filter between the output of the integrating sphere of a reflectance spectrometer and the photodetector in order to block fluorescence partially. From these data, the relative emission spectrum of the dye, the filter transmission spectrum, and the detector sensitivity, true reflectances and absolute fluorescence quantum yields were recovered. Observed fluorescence quantum yields, affected by dye aggregation and inner filter effects, were concentration and wavelength dependent, ranging approximately between 0.1 and 0.6. The analysis of remission function spectra showed that dye aggregation is negligible up to a concentration of 1.41 x 10(-7) mol g(-1). Fluorescence data were corrected for reemission and reabsorption using a suitable model [Lagorio, M. G.; Dicelio, L. E.; Litter, M. I.; San Roman, E. J. Chem. Soc., Faraday Trans. 1998, 94, 419]. Application of this model to samples showing no aggregation yielded a wavelength-independent true fluorescence quantum yield of 0.60 +/- 0.05, similar to values found in solution. The usage of cresyl violet as a reference for the evaluation of fluorescence quantum yields for weakly fluorescing samples in the solid phase is discussed.     

Effect of gold nanoparticles on an aerosil surface on the fluorescence and Raman spectra of adsorbed tryptophan

We discuss the fluorescence and Raman spectra of the amino acid tryptophan (Trp) in the presence of gold nanoparticles in solution and on the surface of highly dispersed silica (aerosil) containing gold nanoparticles (Au-SiO₂). The fluorescence of Trp is efficiently quenched in the presence of gold nanoparticles both in solution and on the SiO₂ surface. The fluorescence and excitation spectra contain bands for molecular Trp and a charge transfer complex between Trp and the nanoparticles. In the Raman spectra of Trp with gold nanoparticles, considerably enhanced intense vibrations appear for the carboxyl and amino groups and also for the benzene and pyrrole rings. The effect of gold nanoparticles on the Raman spectra of Trp in a heterogeneous system is considerably weakened due to strong light scattering by the dispersed silica.