989 resultados para REFLECTANCE DIFFERENCE SPECTROSCOPY


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Fully quantitative analyses of DRIFTS data are required when the surface concentrations and the specific rate constants of reaction (or desorption) of adsorbates are needed to validate microkinetic models. The relationship between the surface coverage of adsorbates and various functions derived from the signal collected by DRIFTS is discussed here. The Kubelka-Munk and pseudoabsorbance (noted here as absorbance, for the sake of brevity) transformations were considered, since those are the most commonly used functions when data collected by DRIFTS are reported. Theoretical calculations and experimental evidence based on the study of CO adsorption on Pt/SiO2 and formate species adsorbed on Pt/CeO2 showed that the absorbance (i.e., ) log 1/R������¢, with R������¢ ) relative reflectance) is the most appropriate, yet imperfect, function to give a linear representation of the adsorbate surface concentration in the examples treated here, for which the relative reflectance R������¢ is typically > 60%. When the adsorbates lead to a strong signal absorption (e.g., R������¢ < 60%), the Kubelka-Munk function is actually more appropriate. The absorbance allows a simple correction of baseline drifts, which often occur during time-resolved data collection over catalytic materials. Baseline corrections are markedly more complex in the case of the other mathematical transforms, including the function proposed by Matyshak and Krylov (Catal. Today 1995, 25, 1-87), which has been proposed as an appropriate representation of surface concentrations in DRIFTS spectroscopy.

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Singles only: DNA sequences can be induced to spontaneously adsorb to the surfaces of Ag colloids through their nucleotide side chains (see picture). The SERS spectra of these nonspecifically bound strands are sufficiently reproducible that they can be used to identify single-base mismatches in short (25-mer and 23-mer) strands. Subtracting the spectra of different DNA sequences results in difference spectra that contain features corresponding to the exchanged nucleotides.

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A study was undertaken to examine a range of sample preparation and near infrared reflectance spectroscopy (NIPS) methodologies, using undried samples, for predicting organic matter digestibility (OMD g kg(-1)) and ad libitum intake (g kg(-1) W-0.75) of grass silages. A total of eight sample preparation/NIRS scanning methods were examined involving three extents of silage comminution, two liquid extracts and scanning via either external probe (1100-2200 nm) or internal cell (1100-2500 nm). The spectral data (log 1/R) for each of the eight methods were examined by three regression techniques each with a range of data transformations. The 136 silages used in the study were obtained from farms across Northern Ireland, over a two year period, and had in vivo OMD (sheep) and ad libitum intake (cattle) determined under uniform conditions. In the comparisons of the eight sample preparation/scanning methods, and the differing mathematical treatments of the spectral data, the sample population was divided into calibration (n = 91) and validation (n = 45) sets. The standard error of performance (SEP) on the validation set was used in comparisons of prediction accuracy. Across all 8 sample preparation/scanning methods, the modified partial least squares (MPLS) technique, generally minimized SEP's for both OMD and intake. The accuracy of prediction also increased with degree of comminution of the forage and with scanning by internal cell rather than external probe. The system providing the lowest SEP used the MPLS regression technique on spectra from the finely milled material scanned through the internal cell. This resulted in SEP and R-2 (variance accounted for in validation set) values of 24 (g/kg OM) and 0.88 (OMD) and 5.37 (g/kg W-0.75) and 0.77 (intake) respectively. These data indicate that with appropriate techniques NIRS scanning of undried samples of grass silage can produce predictions of intake and digestibility with accuracies similar to those achieved previously using NIRS with dried samples. (C) 1998 Elsevier Science B.V.

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TlCu2-xFexSe2 is a p-type metal for x < 0.5 which crystallizes in a body-centred tetragonal structure. The metal atoms are situated in ab-planes, similar to 7 angstrom apart, while the metal - metal distance within the plane is similar to 2.75 angstrom. Due to the large difference in cation distances, the solid solutions show magnetic properties of mainly two-dimensional character. The SQUID measurements performed for x = 0.27 give the c-axis as the easy axis of magnetization, but also show clear hysteresis effects at 10 K, indicating a partly ferromagnetic coupling. The magnetic ordering temperature T-c is 55( 5) K as found from both SQUID and Mossbauer spectra. At T << Tc the magnetic hyperfine fields are distributed with a maximum at about 30 T, which are compared to the measured magnetic moment per iron atom, which is 0.97 mu(B)/Fe as found from SQUID measurements. The experimental results are compared to results using other methods on isostructural Tl selenides.

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An approach is developed for probing the thermodynamics and kinetics of irreversible electrochemical reactions on solid surfaces based on local frequency-voltage spectroscopy. For a model Li-ion conductor surface, two regimes for bias-controlled behavior are demonstrated and ascribed to the difference in the critical nucleus size. The electrostatic and electrochemical phenomena at the tip-surface junction are analyzed. These studies suggest an experimental pathway for exploring local electrochemical activity in solids.

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The dielectric properties of BaTiO3 thin films and multilayers are different from bulk materials because of nanoscale dimensions, interfaces, and stress-strain conditions. In this study, BaTiO3/SrTiO3 multilayers deposited on SrTiO3 substrates by pulsed laser deposition have been investigated by high-energy-resolution electron energy-loss spectroscopy. The fine structures in the spectra are discussed in terms of crystal-field splitting and the internal strain. The crystal-field splitting of the BaTiO3 thin layer is found to be a little larger than that of bulk BaTiO3, which has been interpreted by the presence of the internal strain induced by the misfit at the interface. This finding is consistent with the lattice parameters of the BaTiO3 thin layer determined by the selected area diffraction pattern. The near-edge structure of the oxygen K edge in BaTiO3 thin layers and in bulk BaTiO3 are simulated by first-principle self-consistent full multiple-scattering calculations. The results of the simulations are in a good agreement with the experimental results. Moreover, the aggregation of oxygen vacancies at the rough BaTiO3/SrTiO3 interface is indicated by the increased [Ti]/[O] element ratio, which dominates the difference of dielectric properties between BaTiO3 layer and bulk materials.

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O presente trabalho teve como principal objectivo estudar a modificação química heterogénea controlada de fibras de celulose com diferentes reagentes de modo a alterar as suas propriedades de superfície, em especial em termos da criação de um carácter hidrofóbico e lipofóbico, preservando, sempre que possível, as suas propriedades mecânicas e, consequentemente, abrindo novas perspectivas de aplicação. O desenvolvimento do trabalho envolveu três abordagens principais, envolvendo, em cada caso, o estudo de diferentes condições reaccionais. Na primeira abordagem foram utilizados como reagentes de modificação compostos perfluorados, nomeadamente o anidrido trifluoroacético (TFAA), o cloreto de 2,3,4,5,6-pentafluorobenzoílo (PFBz) e o cloreto de 3,3,3- trifluoropropanoílo (TFP), para promover a acilação heterogénea da superfície das fibras. A segunda estratégia usada consistiu na preparação de híbridos de celulose do tipo orgânico-inorgânico classe-II, através da modificação das fibras de celulose com o (3-isocianatopropil)trietoxissilano (ICPTEOS), um reagente organossilano bifuncional. A ligação às fibras de celulose foi efectuada através das funções isocianato e, posteriormente, os grupos etoxissilano foram sujeitos a tratamentos de hidrólise ácida, como tal ou na presença de outros siloxanos, nomeadamente o tetraetoxissilano (TEOS) e o 1H,1H,2H,2Hperfluorodeciltrietoxissilano (PFDTEOS). Finalmente, a última abordagem foi baseada na modificação das fibras com triclorometilssilano (TCMS), através de uma reacção gás-sólido, que dispensou assim o uso de solventes orgânicos. A ocorrência de modificação química foi em cada caso confirmada por Espectroscopia de Infravermelho com Transformada de Fourier e Reflectância Total Atenuada (FTIR-ATR), Análise Elementar (EA) e determinação de ângulos de contacto. Adicionalmente, e dependendo de cada caso específico, diversas outras técnicas foram empregues na caracterização aprofundada dos materiais preparados, nomeadamente Ressonância Magnética Nuclear CPMAS no Estado Sólido (RMN), Espectroscopia de Difracção de Raios-X (XRD), Análise Termogravimétrica (TGA), Espectrometria de Massa de Iões Secundários com Análise de Tempo de Vôo (ToF-SIMS), Espectroscopia Fotoelectrónica de Raios-X (XPS) e Microscopia Electrónica de Varrimento (SEM). Relativamente à acilação das fibras de celulose com reagentes perfluorados, o sucesso da reacção foi comprovado por FTIR-ATR, EA, XPS e ToF-SIMS. Neste contexto, obtiveram-se fibras modificadas possuindo graus de substituição (DS) compreendidos entre 0.006 e 0.39. Verificou-se por XRD que, em geral, mesmo para os valores de DS mais elevados, a cristalinidade das fibras não foi afectada, indicando que a modificação foi limitada às camadas mais superficiais das mesmas ou a regiões amorfas das suas camadas mais internas. Adicionalmente, observou-se por ToF-SIMS que a distribuição dos grupos perfluorados à superfície das fibras foi, de facto, bastante heterogénea. Todos os derivados de celulose perfluorados apresentaram elevada hidrofobicidade e lipofobicidade, tendo-se atingido ângulos de contacto com água e diiodometano de 126º e 104º, respectivamente. Um aspecto interessante relativo a estes materiais é que a elevada omnifobicidade foi observada mesmo para valores de DS muito reduzidos, não se mostrando significativamente afectada pelo aumento dos mesmos. Em consonância, verificou-se por XPS que a cobertura da superfície das fibras de celulose com grupos perfluorados aumentou apenas ligeiramente com o aumento do DS, apontando para a esterificação de camadas mais internas das fibras, associada, neste caso, predominantemente aos seus domínios amorfos. No que diz respeito à estabilidade hidrolítica destes derivados, obtiveram-se dois tipos distintos de comportamento. Por um lado, as fibras de celulose trifluoroacetiladas são facilmente hidrolisáveis em meio neutro, e, por outro, as fibras pentafluorobenzoiladas e trifluoropropanoiladas mostram-se bastante resistentes face a condições de hidrólise em meio neutro e ácido (pH 4), podendo, contudo, ser facilmente hidrolisadas em meio alcalino (pH 9 e 12, para derivados do PFBz e do TFP, respectivamente). Na segunda abordagem verificou-se a ocorrência de reacção por FTIR-ATR e EA. Em geral, a modificação química com ICPTEOS ocorre predominantemente nas zonas mais superficiais das fibras de celulose ou em regiões amorfas. Contudo, em condições reaccionais mais severas (maior quantidade de reagente e tempo de reacção), esta atingiu também regiões cristalinas, afectando, consequentemente, a estrutura cristalina das fibras, como verificado por XRD. Por RMN de 29Si observou-se que após reacção com o ICPTEOS já existiam indícios de alguma hidrólise dos grupos etoxissilano, e que a sua subsequente condensação parcial tinha levado à formação de uma película inorgânica em redor das fibras (verificado por SEM), constituída maioritariamente por estruturas lineares, com uma contribuição mais modesta de estruturas “diméricas” e outras mais ramificadas. Consequentemente, este revestimento inorgânico transformou as fibras de celulose em materiais híbridos com elevada hidrofobicidade (ângulos de contacto com água entre 103-129º). A hidrólise ácida dos restantes grupos etoxissilano, como tal ou na presença de TEOS, originou híbridos de celulose com elevada hidrofilicidade, sendo impossível medirem-se os ângulos de contacto com água dos produtos finais, devido à presença maioritária de grupos silanol (Si-OH) e ligações Si-O-Si à superfície, os quais contribuíram para o consequente aumento de energia de superfície. No entanto, quando a hidrólise foi realizada na presença de PFDTEOS, obtiveram-se materiais híbridos com elevada hidrofobicidade e lipofobicidade (ângulos de contacto com água e diiodometano de 140º e 134º, respectivamente), devido à combinação da presença de grupos perfluorados e micro- e nano-rugosidades na superfície das fibras de celulose, conforme confirmado por SEM. Finalmente, a última abordagem permitiu preparar materiais derivados de celulose altamente hidrofóbicos e lipofóbicos (ângulos de contacto com água e diiodometano de 136º e 109º, respectivamente) por um processo simples, envolvendo tempos de tratamento tão curtos como 0.5 min. Este comportamento omnifóbico foi gerado pelo efeito sinergético entre a diminuição de energia de superfície das fibras, devido à presença de grupos metilo dos resíduos de TCMS ligados a estas, e a condensação dos resíduos de TCMS na forma de micro- e nano-partículas inorgânicas, que levou à criação de um revestimento rugoso à superfície das fibras, conforme observado por RMN de 29Si e SEM, respectivamente. A pré-humidificação das fibras de celulose demonstrou desempenhar um importante papel de “acelerador” dos processos de hidrólise e condensação das moléculas de TCMS. Nestas condições, o tempo de tratamento foi um dos parâmetros mais relevantes, pois para tempos de tratamento muito curtos (0.5 min) os materiais resultantes não apresentaram quaisquer diferenças a nível de propriedades físico-químicas em relação ao substrato de partida (a humidade em excesso consumiu todo o TCMS antes que este conseguisse reagir com os grupos hidroxilo das fibras de celulose), possuindo, por exemplo, valores de ângulos de contacto com água idênticos. Para tempos de tratamento mais longos, como 30 min, os materiais finais apresentaram a maior quantidade de componentes inorgânicos, tal como verificado por EA e TGA. Assim, o controlo da humidade das fibras é imperativo para se poder moldar as propriedades finais dos produtos. Esta última abordagem é particularmente promissora uma vez que tem como base um sistema simples e “verde” que pode ser facilmente implementado. Em conclusão, este trabalho permitiu demonstrar que a modificação química heterogénea controlada das fibras de celulose representa uma iniciativa promissora para a preparação de novos materiais obtidos a partir de recursos renováveis, com propriedades interessantes e passíveis de ser potencialmente aplicados em diferentes áreas. Para além do mais, as estratégias de modificação estudadas podem também ser precursoras de novos estudos que possam vir a ser desenvolvidos dentro do mesmo âmbito.

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Polarized reflectance measurements of the quasi I-D charge-transfer salt (TMTSFh CI04 were carried out using a Martin-Puplett-type polarizing interferometer and a 3He refrigerator cryostat, at several temperatures between 0.45 K and 26 K, in the far infrared, in the 10 to 70 cm- 1 frequency range. Bis-tetramethyl-tetraselena-fulvalene perchlorate crystals, grown electrochemically and supplied by K. Behnia, of dimensions 2 to 4 by 0.4 by 0.2 mm, were assembled on a flat surface to form a mosaic of 1.5 by 3 mm. The needle shaped crystals were positioned parallel to each other along their long axis, which is the stacking direction of the planar TMTSF cations, exposing the ab plane face (parallel to which the sheets of CI04 anions are positioned). Reflectance measurements were performed with radiation polarized along the stacking direction in the sample. Measurements were carried out following either a fast (15-20 K per minute) or slow (0.1 K per minute) cooling of the sample. Slow cooling permits the anions to order near 24 K, and the sample is expected to be superconducting below 1.2 K, while fast cooling yields an insulating state at low temperatures. Upon the slow cooling the reflectance shows dependence with temperature and exhibits the 28 cm- 1 feature reported previously [1]. Thermoreflectance for both the 'slow' and 'fast' cooling of the sample calculated relative to the 26 K reflectance data indicates that the reflectance is temperature dependent, for the slow cooling case only. A low frequency edge in the absolute reflectance is assigned an electronic origin given its strong temperature dependence in the relaxed state. We attribute the peak in the absolute reflectance near 30 cm-1 to a phonon coupled to the electronic background. Both the low frequency edge and the 30 cm-1 feature are noted te shift towards higher frequcncy, upon cntering the superconducting state, by an amount of the order of the expected superconducting energy gap. Kramers-Kronig analysis was carried out to determine the optical conductivity for the slowly cooled sample from the measured reflectance. In order to do so the low frequency data was extrapolated to zero frequency using a Hagen-Ru bens behaviour, and the high frequency data was extended with the data of Cao et al. [2], and Kikuchi et al. [3]. The real part of the optical conductivity exhibits an asymmetric peak at 35 cm-1, and its background at lower frequencies seems to be losing spectral weight with lowering of the temperature, leading us to presume that a narrow peak is forming at even lower frequencies.

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The reflectance of thin films of magnesium doped SrRu03(Mg-SR0) produced by pulsed laser deposition on SrTiOa (100) substrates has been measured at room temperature between 100 and 7500 cm~^. The films were chosen to have wide range of thickness, stoichiometry and electrical properties. As the films were very thin (less than 300 nm), and some were insulating the reflectance data shows structures due to both the film and the substrate. Hence, the data was analyzed using Kramers-Kronig constrained variational fitting (VDF) method to extract the real optical conductivity of the Mg-SRO films. Although the VDF technique is flexible enough to fit all features of the reflectance spectra, it seems that VDF could not eliminate the substrate's contribution from fllm conductivity results. Also the comparison of the two different programs implementing VDF fltting shows that this technique has a uniqueness problem. The optical properties are discussed in light of the measured structural and transport properties of the fllms which vary with preparation conditions and can be correlated with differences in stoichiometry. This investigation was aimed at checking the VDF technique and also getting answer to the question whether Mg^"*" substitutes in to Ru or Sr site. Analysis of our data suggests that Mg^+ goes to Ru site.

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The optical response to far infrared radiation has been measured on a mosaic of heavy fermion CeColnssingle crystals. The superconducting transition temperature of the crystals has been determined by van der Pauw resistivity and ac-susceptibility measurements as Tc = 2.3 K. The optical measurements were taken above and below the transition temperature using a 3He cryostat and step and integrate Martin-Puplett type polarizing interferometer. The absolute reflectance of the heavy fermion CeColns in the superconducting state in range (0, 100)cm-1 was calculated from the measured thermal reflectance, using the normal state data of Singley et al and a low frequency extrapolation for a metallic material in the Hagen-Rubens regime. By means of Kramers-Kronig analysis the absolute reflectance was used to calculate the optical conductivity of the sample. The real part of the calculated complex conductivity 0-(w) ofCeColns indicates a possible opening of an energy gap close to 50 em-I.

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A new Ultra-High Vacuum (UHV) reflectance spectrometer was successfully designed, making use of a Janis Industries ST-400 sample cryostat, IR Labs bolometer, and Briiker IFS 66 v/S spectrometer. Two of the noteworthy features include an in situ gold evaporator and internal reference path, both of which allow for the experiment to progress with a completely undisturbed sample position. As tested, the system was designed to operate between 4.2 K and 325 K over a frequency range of 60 - 670 cm~^. This frequency range can easily be extended through the addition of appUcable detectors. Tests were performed on SrTiOa, a highly ionic incipient ferroelectric insulator with a well known reflectance. The presence and temperatmre dependence of the lowest frequency "soft" mode were measured, as was the presence of the other two infrared modes. During the structural phase transition from cubic to tetragonal perovskite, the splitting of the second phonon mode was also observed. All of the collected data indicate good agreement with previous measurements, with a minor discrepency between the actual and recorded sample temperatures.

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The optical response to far infrared radiation has been measured on a mosaic of heavy fermion CeCoIns single crystals. The superconducting transition temperature of the crystals has been determined by van der Pauw resistivity and ac-susceptibility measurements as Tc = 2.3 K. The optical measurements were taken above and below the transition temperature using a ^He cryostat and step and integrate Martin-Puplett type polarizing interferometer. The absolute reflectance of the heavy fermion CeCoIns in the superconducting state in range (0, 100)cm~^ was calculated from the measured thermal reflectance, using the normal state data of Singley et al and a low frequency extrapolation for a metallic material in the Hagen-Rubens regime. By means of Kramers-Kronig analysis the absolute reflectance was used to calculate the optical conductivity of the sample. The real part of the calculated complex conductivity a{u)) of CeCoIns indicates a possible opening of an energy gap close to 50 cm~^.

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Low temperature (77K) linear dichroism spectroscopy was used to characterize pigment orientation changes accompanying the light state transition in the cyanobacterium, Synechococcus sp. pee 6301, and cold-hardening in winter rye (Secale cereale L. cv. Puma). Samples were oriented for spectroscopy using the gel squeezing method (Abdourakhmanov et aI., 1979) and brought to 77K in liquid nitrogen. The linear dichroism (LD) spectra of Synechococcus 6301 phycobilisome/thylakoid membrane fragments cross-linked in light state 1 and light state 2 with glutaraldehyde showed differences in both chlorophyll a and phycobilin orientation. A decrease in the relative amplitude of the 681nm chlorophyll a positive LD peak was observed in membrane fragments in state 2. Reorientation of the phycobilisome (PBS) during the transition to state 2 resulted in an increase in core allophycocyanin absorption parallel to the membrane, and a decrease in rod phycocyanin parallel absorption. This result supports the "spillover" and "PBS detachment" models of the light state transition in PBS-containing organisms, but not the "mobile PBS" model. A model was proposed for PBS reorientation upon transition to state 2, consisting of a tilt in the antenna complex with respect to the membrane plane. Linear dichroism spectra of PBS/thylakoid fragments from the red alga, Porphyridium cruentum, grown in green light (containing relatively more PSI) and red light (containing relatively more PSll) were compared to identify chlorophyll a absorption bands associated with each photosystem. Spectra from red light - grown samples had a larger positive LD signal on the short wavelength side of the 686nm chlorophyll a peak than those from green light - grown fragments. These results support the identification of the difference in linear dichroism seen at 681nm in Synechococcus spectra as a reorientation of PSll chromophores. Linear dichroism spectra were taken of thylakoid membranes isolated from winter rye grown at 20°C (non-hardened) and 5°C (cold-hardened). Differences were seen in the orientation of chlorophyll b relative to chlorophyll a. An increase in parallel absorption was identified at the long-wavelength chlorophyll a absorption peak, along with a decrease in parallel absorption from chlorophyll b chromophores. The same changes in relative pigment orientation were seen in the LD of isolated hardened and non-hardened light-harvesting antenna complexes (LHCII). It was concluded that orientational differences in LHCII pigments were responsible for thylakoid LD differences. Changes in pigment orientation, along with differences observed in long-wavelength absorption and in the overall magnitude of LD in hardened and non-hardened complexes, could be explained by the higher LHCII monomer:oligomer ratio in hardened rye (Huner et ai., 1987) if differences in this ratio affect differential light scattering properties, or fluctuation of chromophore orientation in the isolated LHCII sample.

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Three cores from the Kearl Lake Oil Sands area within the Athabasca deposit of northeastern Alberta have been analyzed to understand the thermal history of the McMurray and Clearwater formations of the Lower Cretaceous Mannville Group. The approach involves the integration of vitrinite reflectance (VR), Rock-Eval pyrolysis, fluorescence microscopy, and palynology. Mean VR varies between 0.21 and 0.43% Ro and indicates thermally immature levels equivalent to the rank of lignite to sub-bituminous coal. Although differing lithologies have influenced VR to some extent (i.e., coals and bitumen-rich zones), groundwater influence and oxidation seem not to have measurably altered YR. Rock-Eval analysis points to Type III/IV kerogen, and samples rich in amorphous organic matter (ADM) show little to no fluorescence characteristics, implying a terrestrial source of origin. Palynology reveals the presence of some delicate macerals but lack of fluorescence and abundant ADM suggests some degradation and partial oxidation of the samples.

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High chromium content in kimberlite indicator minerals such as pyrope garnet and diopside is often correlated with the presence of diamonds. In this study, kimberlite indicator minerals were examined using visible light reflectance spectroscopy to determine if chromium content can be correlated with spectral absorption features. The depth of absorption features in the visible spectral region were correlated with the molecular percentage of chromium and other first series transition metal elements obtained by electron microprobe data. In the visible part of the spectrum, chromium is evident by 3 absorption features in the pyrope reflectance spectrum; one isolated and narrow feature at the wavelength 689 nm was used to correlate with the chromium mol %. The isolation of this feature in the pyrope spectra is advantageous since it is not directly affected by other proximal absorption bands that could be caused by other transition metals. Analysis of the feature indicates that as grain volume increases the depth of the absorption feature will also increase. Clustering grain volumes into fractions yields better correlation between absorption depth and mol % chromium. Other types of garnet (almandine, grossular, spessartine) and kimberlite indicator minerals (olivine, diopside, chromite, ilmenite) were analyzed to determine if other absorption features could be used to predict the proportion of specific transition metal elements. Diopside in particular illustrates the same isolated chromium absorption feature as pyrope and may indicate mol percent but needs further study with larger sample sets.