Gamma-ray Spectra and Enhancement Factors for Positron Annihilation with Core Electrons

Many-body theory is developed to calculate the γ spectra for positron annihilation in noble-gas atoms. Inclusion of electron-positron correlation effects and core annihilation gives spectra in excellent agreement with experiment [K. Iwata et al., Phys. Rev. Lett. 79, 39 (1997)]. The calculated correlation enhancement factors γnl for individual electron orbitals nl are found to scale with the ionization energy I_nl (in eV), as γnl=1+ √A/Inl+(B/I_nl)β, where A≈40  eV, B≈24  eV, and β≈2.3.

Valence and L-shell photoionization of Cl-like argon using R-matrix techniques

Photoionization cross-sections are obtained using the relativistic DiracAtomic R-matrix Codes (DARC) for all valence and L-shell energy ranges between 27 and 270 eV. A total of 557 levels arising from the dominant configurations 3s²3p⁴, 3s³p5, 3p⁶, 3s²3p³[3d, 4s, 4p], 3p⁵3d, 3s²3p²3d², 3s³p4³d, 3s³p3³d2 and 2s²2p⁵3s²3p⁵ have been included in the targetwavefunction representation of the Ar III ion, including up to 4p in the orbital basis. We also performed a smaller Breit-Pauli (BP) calculation containing the lowest 124 levels. Direct comparisons are made with previous theoretical and experimental work for both valence shell and L-shell photoionization. Excellent agreement was found for transitions involving the ²P^o initial state to all allowed final states for both calculations across a range of photon energies. A number of resonant states have been identified to help analyse and explain the nature of the spectra at photon energies between 250 and 270 eV.

Measurement of Fast Electrons Spectra Generated by Interaction between Solid Target and Peta Watt Laser

Fast electron energy spectra have been measured for a range of intensities between 1018 Wcm−2 and 1021 Wcm−2 and for different target materials using electron spectrometers. Several experimental campaigns were conducted on peta watt laser facilities at the Rutherford Appleton Laboratory and Osaka University. In these experimental campaigns, the pulse duration was varied from 0.5 ps to 5 ps. The laser incident angle was also changed from normal incidence to 40° in p-polarized. The results show a reduction from the ponderomotive scaling on fast electrons over 1020 Wcm−2.

M Dwarf Flare Continuum Variations on One-second Timescales: Calibrating and Modeling of ULTRACAM Flare Color Indices

We present a large data set of high-cadence dMe flare light curves obtained with custom continuum filters on the triple-beam, high-speed camera system ULTRACAM. The measurements provide constraints for models of the near-ultraviolet (NUV) and optical continuum spectral evolution on timescales of ≈1 s. We provide a robust interpretation of the flare emission in the ULTRACAM filters using simultaneously obtained low-resolution spectra during two moderate-sized flares in the dM4.5e star YZ CMi. By avoiding the spectral complexity within the broadband Johnson filters, the ULTRACAM filters are shown to characterize bona fide continuum emission in the NUV, blue, and red wavelength regimes. The NUV/blue flux ratio in flares is equivalent to a Balmer jump ratio, and the blue/red flux ratio provides an estimate for the color temperature of the optical continuum emission. We present a new “color-color” relationship for these continuum flux ratios at the peaks of the flares. Using the RADYN and RH codes, we interpret the ULTRACAM filter emission using the dominant emission processes from a radiative-hydrodynamic flare model with a high nonthermal electron beam flux, which explains a hot, T ≈ 104 K, color temperature at blue-to-red optical wavelengths and a small Balmer jump ratio as observed in moderate-sized and large flares alike. We also discuss the high time resolution, high signal-to-noise continuum color variations observed in YZ CMi during a giant flare, which increased the NUV flux from this star by over a factor of 100. Based on observations obtained with the Apache Point Observatory 3.5 m telescope, which is owned and operated by the Astrophysical Research Consortium, based on observations made with the William Herschel Telescope operated on the island of La Palma by the Isaac Newton Group in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astrofsica de Canarias, and observations, and based on observations made with the ESO Telescopes at the La Silla Paranal Observatory under programme ID 085.D-0501(A).

Caracterização e transformação de Lenhosulfonatos de Eucalyptus globulus

Os lenhosulfonatos representam um sub-produto formado durante o cozimento ao sulfito ácido, sendo queimados para a regeneração da base e recuperação de energia. No entanto, os lenhosulfonatos são também considerados uma importante matéria-prima para a produção de vários produtos de valor acrescentado. Os objectivos principais deste trabalho foram contribuir para uma melhor compreensão sobre a caracterização química e estrutural dos lenhosulfonatos do Eucalyptus globulus, assim como, para complementar a informação disponível sobre a síntese e a caracterização estrutural e térmica de materiais poliméricos obtidos a partir de compostos modelo dos produtos de oxidação dos lenhosulfonatos. O licor de cozimento ao sulfito foi analisado em termos do teor de cinzas, extractáveis, compostos voláteis, açúcares e lenhosulfonatos. O teor de cinzas e açúcares no licor de cozimento é muito elevado, tendo sido necessário purificar o mesmo (2,8-13,8 % e 3,2-9,1 %, respectivamente). A análise dos açúcares mostrou uma quantidade considerável de pentoses, sendo o açúcar predominante a xilose. Os lenhosulfonatos foram purificados, isolados e caracterizados por química molhada (titulação potenciométrica e oxidação com permanganato), análise elementar, espectroscopia de ultravioleta/visível (UV/Vis), espectroscopia de infravermelho de transformada de Fourier (FTIR), espectroscopia de ressonância magnética nuclear de protão (RMN de 1H) e carbono (RMN de 13C), espectrometria de massa de ionização por electrospray (ESI-MS), cromatografia de permeação em gel (GPC), termogavimetria (TGA) e calorimetria diferencial de varrimento (DSC). Os lenhosulfonatos são constituídos principalmente por unidades S, são parcialmente sulfonados e possuem um peso molecular relativamente baixo (Mw = 1250-2400 Da). A ruptura das ligações β-O-4 e α-O-4 da lenhina do Eucalyptus globulus após cozimento ao sulfito ácido originam olígomeros de baixo peso molecular cuja estrutura foi elucidada por RMN 1D/2D e ESI-MS. A degradação térmica dos lenhosulfonatos apresentou dois máximos de degradação a 188-190ºC e a 315-380ºC. As curvas de DSC mostraram um pico endotérmico para temperaturas inferiores a 130ºC e um pico exotérmico a 300-500ºC. Os lenhosulfonatos foram despolimerizados na presença de oxigénio molecular em meio alcalino. Os produtos de oxidação principais foram o aldeído siríngico, a vanilina, o ácido vanílico e o ácido siríngico. A adição do catalisador (sal de cobre) promoveu a oxidação dos lenhosulfonatos aumentando o rendimento dos aldeídos aromáticos (< 50%). A presença de açúcares nos lenhosulfonatos teve um efeito negativo no rendimento dos produtos de oxidação principais. Alguns compostos modelo dos produtos de oxidação dos lenhosulfonatos foram polimerizados por poliadição (catiónica e radicalar) e policondensação. Os monómeros e os polímeros foram caracterizados por espectroscopia de infravermelho de transformada de Fourier e reflectância total atenuada (FTIR-ATR), RMN em solução e no estado sólido, UV/Vis no estado sólido, GPC, difracção de raios-X (XRD), TGA e DSC. Os compostos modelo estudados foram os estirenos metoxi-substituídos (p-metoxiestireno e 3,4-dimetoxiestireno) e os ácidos hidroxi aromáticos metoxi-substituídos (ácido vanílico e ácido siríngico). O 3,4-dimetoxiestireno foi ainda copolimerizado com o éter isobutil vinílico e os seus copolímeros foram desmetilados, assim como, o poli(p-metoxiestireno) e o poli(3,4-dimetoxiestireno). A polimerização catiónica do p-metoxiestireno e 3,4-dimetoxiestireno é mais rápida e mais completa do que a polimerização radicalar produzindo polímeros com pesos moleculares elevados. O poli(p-metoxiestireno) (Mw = 235000 Da) possui um peso molecular maior do que o poli(3,4-dimetoxiestireno) (Mw = 18800 Da). A estabilidade térmica e a temperatura de transição vítrea diminuiram com a presença do segundo grupo metoxilo. A desmetilação dos homopolímeros foi bem sucedida, tendo sido corroborada por FTIR-ATR e RMN. A policondensação do ácido siríngico foi dificultada pela presença do segundo grupo metoxilo, tendo sido necessário adicionar uma maior quantidade do agente de condensação devido a factores estéricos. O poli(ácido vanílico) e poli(ácido siríngico) são insolúveis na maior parte dos solventes orgânicos, sendo parcialmente solúveis em clorofórmio, ácido triflúoracético, 1,1,2,2- tetracloroetano, dimetilsulfóxido, tetrahidrofurano, N,N’-dimetilformamida e 1,1,1,3,3,3-hexaflúor-2-propanol. A estabilidade térmica diminuiu com a presença do segundo grupo metoxilo e os dois polímeros não exibiram temperatura de transição vítrea. O poli(ácido vanílico) e poli(ácido siríngico) apresentaram uma estrutura muito cristalina (grau de cristalinidade 70% e 50%, respectivamente). O segundo grupo metoxilo aumentou o valor da absorvância, mas a forma do espectro de UV/Vis foi similar. A polimerização catiónica do éter isobutil vinílico resultou na produção de um polímero muito viscoso com peso molecular elevado (Mw = 20400 Da). A degradação térmica do polímero ocorreu em várias gamas de temperatura e foi completa (0% de resíduo a 800ºC). A copolimerização catiónica do 3,4-dimetoxiestireno com o éter isobutil vinílico foi realizada com proporções diferentes 80:20, 50:50 e 20:80. Os copolímeros apresentaram uma viscosidade elevada e um peso molecular baixo (Mw = 2000-4000 Da) que aumentou com a quantidade de éter isobutil vinílico. A degradação térmica dos copolímeros ocorreu também em várias gamas de temperatura, sendo a sua degradação completa (0,9-1,5% de resíduo a 800ºC). A desmetilação dos copolímeros não foi bem sucedida, tendo sido confirmada por FTIR-ATR e RMN.

Spectra of graphs obtained by a generalization of the join graph operation

Taking a Fiedler’s result on the spectrum of a matrix formed from two symmetric matrices as a motivation, a more general result is deduced and applied to the determination of adjacency and Laplacian spectra of graphs obtained by a generalized join graph operation on families of graphs (regular in the case of adjacency spectra and arbitrary in the case of Laplacian spectra). Some additional consequences are explored, namely regarding the largest eigenvalue and algebraic connectivity.

On the Faria's inequality for the Laplacian and signless Laplacian spectra: a unified approach

Let p(G)p(G) and q(G)q(G) be the number of pendant vertices and quasi-pendant vertices of a simple undirected graph G, respectively. Let m_L±(G)(1) be the multiplicity of 1 as eigenvalue of a matrix which can be either the Laplacian or the signless Laplacian of a graph G. A result due to I. Faria states that mL±(G)(1) is bounded below by p(G)−q(G). Let r(G) be the number of internal vertices of G. If r(G)=q(G), following a unified approach we prove that mL±(G)(1)=p(G)−q(G). If r(G)>q(G) then we determine the equality mL±(G)(1)=p(G)−q(G)+mN±(1), where mN±(1) denotes the multiplicity of 1 as eigenvalue of a matrix N±. This matrix is obtained from either the Laplacian or signless Laplacian matrix of the subgraph induced by the internal vertices which are non-quasi-pendant vertices. Furthermore, conditions for 1 to be an eigenvalue of a principal submatrix are deduced and applied to some families of graphs.

Numerical techniques for modeling Doppler ultrasound spectra systems

Evaluation of blood-flow Doppler ultrasound spectral content is currently performed on clinical diagnosis. Since mean frequency and bandwidth spectral parameters are determinants on the quantification of stenotic degree, more precise estimators than the conventional Fourier transform should be seek. This paper summarizes studies led by the author in this field, as well as the strategies used to implement the methods in real-time. Regarding stationary and nonstationary characteristics of the blood-flow signal, different models were assessed. When autoregressive and autoregressive moving average models were compared with the traditional Fourier based methods in terms of their statistical performance while estimating both spectral parameters, the Modified Covariance model was identified by the cost/benefit criterion as the estimator presenting better performance. The performance of three time-frequency distributions and the Short Time Fourier Transform was also compared. The Choi-Williams distribution proved to be more accurate than the other methods. The identified spectral estimators were developed and optimized using high performance techniques. Homogeneous and heterogeneous architectures supporting multiple instruction multiple data parallel processing were essayed. Results obtained proved that real-time implementation of the blood-flow estimators is feasible, enhancing the usage of more complex spectral models on other ultrasonic systems.

DRIFT and DRUV spectroscopy methods for studying the interaction of metal compounds with native cellulose

Dissertação de mestrado, Qualidade em Análises, Faculdade de Ciências e Tecnologia, Universidade do Algarve, 2015

Phonon spectra and thermodynamic properties of rare gas solids based on empirical and semi-empirical (ab initio) two-body potentials : a comparative study /

We study the phonon dispersion, cohesive and thermal properties of raxe gas solids Ne, Ar, Kr, and Xe, using a variety of potentials obtained from different approaches; such as, fitting to crystal properties, purely ab initio calculations for molecules and dimers or ab initio calculations for solid crystalline phase, a combination of ab initio calculations and fitting to either gas phase data or sohd state properties. We explore whether potentials derived with a certain approaxih have any obvious benefit over the others in reproducing the solid state properties. In particular, we study phonon dispersion, isothermal ajid adiabatic bulk moduli, thermal expansion, and elastic (shear) constants as a function of temperatiue. Anharmonic effects on thermal expansion, specific heat, and bulk moduli have been studied using A^ perturbation theory in the high temperature limit using the neaxest-neighbor central force (nncf) model as developed by Shukla and MacDonald [4]. In our study, we find that potentials based on fitting to the crystal properties have some advantage, particularly for Kr and Xe, in terms of reproducing the thermodynamic properties over an extended range of temperatiures, but agreement with the phonon frequencies with the measured values is not guaranteed. For the lighter element Ne, the LJ potential which is based on fitting to the gas phase data produces best results for the thermodynamic properties; however, the Eggenberger potential for Ne, where the potential is based on combining ab initio quantum chemical calculations and molecular dynamics simulations, produces results that have better agreement with the measured dispersion, and elastic (shear) values. For At, the Morse-type potential, which is based on M0ller-Plesset perturbation theory to fourth order (MP4) ab initio calculations, yields the best results for the thermodynamic properties, elastic (shear) constants, and the phonon dispersion curves.

Fluorescence spectra and ab initio theoretical studies of HCOOH /

A fluorescence excitation spectrum of formic acid monomer (HCOOH) , has been recorded in the 278-246 nm region and has been attributed to an n >7r* electron promotion in the anti conformer. The S^< S^ electronic origins of the HCOOH/HCOOD/DCOOH/DCOOD isotopomers were assigned to weak bands observed at 37431.5/37461.5/37445.5/37479.3 cm'''. From a band contour analysis of the 0°^ band of HCOOH, the rotational constants for the excited state were estimated: A'=1.8619, B'=0.4073, and C'=0.3730 cm'\ Four vibrational modes, 1/3(0=0), j/^(0-C=0) , J/g(C-H^^^) and i/,(0-H^yJ were observed in the spectrum. The activity of the antisymmetric aldehyde wagging and hydroxyl torsional modes in forming progressions is central to the analysis, leading to the conclusion that the two hydrogens are distorted from the molecular plane, 0-C=0, in the upper S. state. Ab initio calculations were performed at the 6-3 IG* SCF level using the Gaussian 86 system of programs to aid in the vibrational assignments. The computations show that the potential surface which describes the low frequency OH torsion (twisting motion) and the CH wagging (molecular inversion) motions is complex in the S^ excited electronic state. The OH and CH bonds were calculated to be twisted with respect to the 0-C=0 molecular frame by 63.66 and 4 5.76 degrees, respectively. The calculations predicted the existence of the second (syn) rotamer which is 338 cm'^ above the equilibrium configuration with OH and CH angles displaced from the plane by 47.91 and 41.32 degrees.

Coriolis effects in symmetric top spectra /

The "x-y Coriolis Coupling Theory" as presented by Dilauro and Mills (1966) is reformulated and extended to the determination of Raman intensities. Theoretical Raman and Infrared spectra are computed in order to understand the effects due to this coupling in both types of spectra. Both the Infrared and Raman spectra obtained indicate very real effects due to Coriolis coupling. In some of the cases chosen the computed spectra are grossly different from the normal spectra where coupling is absent. Such large effects can greatly impede the interpretation of experimental results. Theoretical spectra therefore aids in the interpretation of experimental results, as is clearly demonstrated in the results of this work.

The normal co-ordinate analysis, vibrational spectra and theoretical infrared intensities of some thiocarbonyl halide molecules /

TITLE: The normal co-ordinate analysis, vibrational spectra and theoretical infrared intensities of some thiocarbonyl halides. AUTHOR: J. L. Brema SUPERVISOR: Dr. D. C. Moule NUMBER OF PAGES: 89 ABSTRACT: The vibrational assignment of the five-in-plane fundamental modes of CSClBr has been made on the basis of infrared gas phase and liquid Raman spectral analyses to supplement our earlier vibrational studies. Even though the one out-of-plane fundamental was not observed spectroscopically an attempt has been made to predict its frequency. The vibrational spectra contained impurity bands and the CSClBr assignment was made only after a thorough analysis of the impurities themselves. A normal co-ordinate analysis calculation was performed assuming a Urey-Bradley force field. This calculation yielded the fundamental frequencies in good agreement with those observed after refinement of the originally transferred force constants. The theoretical frequencies are the eigenvalues of the secular equation and the calculation also gave the corresponding eigenvectors in the form of the very important LLj matrix. The [l] matrix is the transfoirmation between internal co-ordinates and normal co-ordinates and it is essential for Franck-Condon calculations on electronically excited molecules and for infrared Integrated band intensity studies. Using a self-consistent molecular orbital calculation termed "complete neglect of differential overlap" (CNDO/2) , theoretical values of equilibrium bond lengths and angleswere calcuted for a series of carbonyl and thlocarbonyl molecules. From these calculations valence force field force constants were also determined but with limited success. With the CNIX)/2 method theoretical dipole moment derivatives with respect to symmetrized internal co-ordinates were calculated and the results should be useful in a correlation with experimentally determined values.

Phonon spectra and thermal properties of some fcc metals using embedded-atom potentials /

By employing the embedded-atom potentials of Mei et ai.[l], we have calculated the dynamical matrices and phonon dispersion curves for six fee metals (Cu,Ag,Au,Ni,Pd and Pt). We have also investigated, within the quasiharmonic approximation, some other thermal properties of these metals which depend on the phonon density of states, such as the temperature dependence of lattice constant, coefficient of linear thermal expansion, isothermal and adiabatic bulk moduli, heat capacities at constant volume and constant pressure, Griineisen parameter and Debye temperature. The computed results are compared with the experimental findings wherever possible. The comparison shows a generally good agreement between the theoretical values and experimental data for all properties except the discrepancies of phonon frequencies and Debye temperature for Pd, Pt and Au. Further, we modify the parameters of this model for Pd and Pt and obtain the phonon dispersion curves which is in good agreement with experimental data.

An analysis of the photoelectron and Rydberg states of formaldehyde /|nby Carol R. Lessard. -- 260 St. Catharines [Ont.] : Dept. of Chemistry, Brock University,

Although it is generally accepted that Rydberg orbitals are very large and diffuse, and that electron promotion to a Rydberg orbital is not too different from ionization of the molecule, analysis of the two types of transitions proves otherwise. The photoelectron spectrum of the 2B2 (n) ion has very little vibrational structure attached to the origin band; on the other hand, several of the Rydberg transitions which involve the promotion of the n(bZ) electron exhibit a great deal of vibrational activity. In particular, the members of the n=3 Rydberg\ series interact with and perturb each other through pseudo-Jahn-Teller vibronic coupling. The vacuum ultraviolet spectrum contains a number of features which are difficult to explain, and two unusually sharp bands can only be identified as representing some form of electron promotion in formaldehyde.