977 resultados para Ab initio electronic structure


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Dissertation to obtain the academic degree of Master in materials engineering submitted to the Faculty of science and engineering of Universidade Nova de Lisboa

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Este trabalho, no âmbito da física atómica e molecular, é essencialmente um estudo experimental, por fotoionização, da estrutura electrónica de moléculas e átomos de elevada instabilidade, relevantes na indústria, atmosfera terrestre e astrofísica. Os estudos de física molecular compreendem a caracterização em fase gasosa, à temperatura ambiente e a decomposição térmica controlada até 1100 K, por fotoionização com radiação de ultravioleta de vácuo usando a fonte de He I (21.22 eV), das seguintes moléculas: azidoformato de metilo, N3COOCH3; azidoformato de etilo, N3COOCH2CH3; azidoacetato de etilo, N3CH2COOCH2CH3; azidoetanol, N3CH2CH2OH;2-azidopropionitrilo, CH3CH(N3)CN; e 3-azidopropionitrilo, N3CH2CH2CN. Os resultados de espectroscopia de fotoelectrões, para cada uma destas moléculas, são comparados com os resultados do estudo de pirólise pela técnica de isolamento em matriz de azoto molecular, à temperatura de 12 K, assistida por espectroscopia de infravermelho. Os compostos intermediários e produtos finais observados permitem propor mecanismos de decomposição térmica para cada um dos sistemas. A interpretação e atribuição das bandas espectrais relativas a cada molécula têm por base os cálculos ab initio (HF e MP2) e de funcional da densidade (BLYP e B3LYP) das propriedades moleculares dos seus confórmeros de equilíbrio. A radiação de sincrotrão de ultravioleta de vácuo é usada nos estudos, por fotoionização, do oxigénio e azoto atómicos e dos radicais OH e OD, os quais são produzidos in situ por descarga de microondas e/ou reacção rápida átomo molécula. Para cada um destes sistemas, apresentam-se medidas da secção eficaz parcial de fotoionização, σ i, e do parâmetro de assimetria, β. Nestes estudos é usada a radiação da estação de trabalho 4.2 do Sincrotrão Elettra, em Itália.

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Zn1−xCoxO films with different Co concentrations (with x=0.00, 0.10, 0.15, and 0.30) were grown by pulsed laser deposition (PLD) technique. The structural and optical properties of the films were investigated by grazing incidence X-ray diffraction (GIXRD), Raman spectroscopy and photoluminescence (PL). The magnetic properties were measured by conventional magnetometry using a SQUID and simulated by ab-initio calculations using Korring–Khon–Rostoker (KKR) method combined with coherent potential approximation (CPA). The effect of Co-doping on the GIXRD and Raman peaks positions, shape and intensity is discussed. PL studies demonstrate that Co-doping induces a decrease of the bandgap energy and quenching of the UV emission. They also suggest the presence of Zn interstitials when x≥0.15. The 10% Co-doped ZnO film shows ferromagnetism at 390 K with a spontaneous magnetic moment ≈4×10−5 emu and coercive field ≈0.17 kOe. The origin of ferromagnetism is explained based on the calculations using KKR method.

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El objetivo es aportar parámetros cinéticos de interés en la Fotoquímica de la Atmósferica, relacionada con la comprensión de los procesos de abstracción de átomo de cloro de halometanos, con radicales asimétricos del tipo C2FxCly (donde x + y = 5). La fuente de radicales (ICF2CFECl Y ICF2CFC12) son ioduros asimétricos sintetizados y purificados con cromatografía gaseosa y caracterizado por espectroscopía IR, UV y espectrometría de masa. Se utiliza un sistema de medición para reacciones competitivas en la determinación de las constantes de velocidad, con análisis de los productos mediante cromatografía gaseosa. Se calcularán además algunas funciones termodinámicas de los radicales involucrados y de los procesos de transferencia de átomo de cloro de las reacciones directas e inversas. Los factores experimentales son reproducidos por el método de Benson. Para explicar la correlación entre las energías de activación, estructura electrónica y geometría del estado de transición se utilizarán métodos ab-initio y semiempíricos que pueden dar una explicación satisfactoria de los valores experimentales.

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Los estudios realizados a través de este proyecto pretenden abarcar dos aspectos fundamentales en la Física Experimental y Teórica, los cuales son: a) Realizar estudios en investigación básica, orientados a acrecentar el conocimiento en ramas de la Física Molecular, utilizando la técnica de Resonancia Magnética Nuclear (RMN). Para ello se obtienen e interpretan los parámetros magnéticos moleculares característicos y se desarrollan e implementan métodos de cálculo de gran potencia y tiempo de cómputo a fin de correlacionar los estudios de tales parámetros con la estructura geométrica y electrónica molecular y/o con las diversas interacciones moleculares que se puedan presentar. b) Presentar y desarrollar tecnología adicional que permita aplicaciones de la RMN a otras líneas de estudio y también la consolidación de la infraestructura experimental existente en la Universidad Nacional de Río Cuarto. Objetivos generales y específicos: Se plantea como objetivo global, el acrecentar el conocimiento de un conjunto de propiedades moleculares, estudiando una familia de compuestos orgánicos mediante la técnica de la RMN de alta resolución y el empleo de métodos de cálculo tipo ab-initio. (...) Se mencionan a continuación los objetivos específicos más importantes a alcanzar: * Proponer modelos y leyes empíricas que describan el comportamiento de los parámetros magnéticos pertenecientes a familias de compuestos orgánicos heterocíclicos en relación a su estructura electrónica y conformacional. * Compatibilizar los estudios empíricos con resultados teóricos. * Desarrollar nuevos métodos de cálculo a fin de obtener una función de onda que mejor aproxime lo anterior. * Orientar parte del trabajo experimental a diversas aplicaciones de la RMN, adaptando el equipamiento existente a otras técnicas y/o adquiriendo equipamiento para tal fin.

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Estudi realitzat a partir d’una estada a la School of Chemistry de la University of Bristol, Gran Bretanya, entre 2006 i 2008. La reacció d’activació del pre-catalitzador CH3-Fe(P(iPr)2CH2)3B-Ph, que es dóna en presència de H2 i P(CH3)3, és una reacció spin-prohibida ja que els reactius i els productes tenen diferents estat d’espín en el seu estat fonamental: el pre-catalitzador és quintet, mentre que el producte format després de l’eliminació de metà, PMe3(H3)-Fe[(P(iPr)2CH2)3B-Ph, és singlet. Un dels intermedis d’aquesta reacció és d’especial interès ja que catalitza la hidrogenació d’olefines. Intermedi que experimentalment s’ha proposat com a H-Fe[(P(iPr)2CH2)3B-Ph] o el Hx-Fe[(P(iPr)2CH2)3B-Ph]. Aquestes espècies han estat estudiades computacionalment, mitjançant la combinació de mètodes del funcional de la densitat calibrats mitjançant càlculs ab initio. Els resultats obtinguts mostren que les superfícies d’energia potencial singlet, triplet i quintet es creuen al llarg de les reaccions descrites. La reacció d’activació del pre-catalitzador és una reacció multi spin-prohibida (més d’un canvi d’espín), en la que el mecanisme preferit addiciona primer hidrogen i després la fosfina, el pas determinant de la velocitat és el creuament de la superfície d’energia potencial quintet a la triplet a la geometria del reactiu, que es produeix amb una barrera d’aproximadament 18 kcal/mol. La reacció d’hidrogenació d’olefines en canvi pot ser o no una reacció espín prohibida depenent de les condicions en que es dugui a terme. En cas de que la reacció es dugui a terme en un excés d’hidrogen, en el mecanisme principal l’espècie activa seria el (H2)H-Fe[(P(iPr)2CH2)3B-Ph] singlet en el seu estat fonamental que hidrogenaria l’olefina sense cap pas espín prohibit. Aquest mecanisme és el de barrera més baixa però s’espera que estigui més desafavorit entropicament. Si les condicions no són d’un important excés d’hidrogen, llavors l’espècie activa s’espera que sigui H-Fe[(P(iPr)2CH2)3B-Ph], la reacció llavors seria multi espín prohibida amb una barrera de unes 13 kcal/mol corresponents al creuament entre la superfície quintet i triplet a la geometria del H-Fe[(P(iPr)2CH2)3B-Ph].

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The computational approach to the Hirshfeld [Theor. Chim. Acta 44, 129 (1977)] atom in a molecule is critically investigated, and several difficulties are highlighted. It is shown that these difficulties are mitigated by an alternative, iterative version, of the Hirshfeld partitioning procedure. The iterative scheme ensures that the Hirshfeld definition represents a mathematically proper information entropy, allows the Hirshfeld approach to be used for charged molecules, eliminates arbitrariness in the choice of the promolecule, and increases the magnitudes of the charges. The resulting "Hirshfeld-I charges" correlate well with electrostatic potential derived atomic charges

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Selected configuration interaction (SCI) for atomic and molecular electronic structure calculations is reformulated in a general framework encompassing all CI methods. The linked cluster expansion is used as an intermediate device to approximate CI coefficients BK of disconnected configurations (those that can be expressed as products of combinations of singly and doubly excited ones) in terms of CI coefficients of lower-excited configurations where each K is a linear combination of configuration-state-functions (CSFs) over all degenerate elements of K. Disconnected configurations up to sextuply excited ones are selected by Brown's energy formula, ΔEK=(E-HKK)BK2/(1-BK2), with BK determined from coefficients of singly and doubly excited configurations. The truncation energy error from disconnected configurations, Δdis, is approximated by the sum of ΔEKS of all discarded Ks. The remaining (connected) configurations are selected by thresholds based on natural orbital concepts. Given a model CI space M, a usual upper bound ES is computed by CI in a selected space S, and EM=E S+ΔEdis+δE, where δE is a residual error which can be calculated by well-defined sensitivity analyses. An SCI calculation on Ne ground state featuring 1077 orbitals is presented. Convergence to within near spectroscopic accuracy (0.5 cm-1) is achieved in a model space M of 1.4× 109 CSFs (1.1 × 1012 determinants) containing up to quadruply excited CSFs. Accurate energy contributions of quintuples and sextuples in a model space of 6.5 × 1012 CSFs are obtained. The impact of SCI on various orbital methods is discussed. Since ΔEdis can readily be calculated for very large basis sets without the need of a CI calculation, it can be used to estimate the orbital basis incompleteness error. A method for precise and efficient evaluation of ES is taken up in a companion paper

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A comparative systematic study of the CrO2F2 compound has been performed using different conventional ab initio methodologies and density functional procedures. Two points have been analyzed: first, the accuracy of results yielded by each method under study, and second, the computational cost required to reach such results. Weighing up both aspects, density functional theory has been found to be more appropriate than the Hartree-Fock (HF) and the analyzed post-HF methods. Hence, the structural characterization and spectroscopic elucidation of the full CrO2X2 series (X=F,Cl,Br,I) has been done at this level of theory. Emphasis has been given to the unknown CrO2I2 species, and specially to the UV/visible spectra of all four compounds. Furthermore, a topological analysis in terms of charge density distributions has revealed why the valence shell electron pair repulsion model fails in predicting the molecular shape of such CrO2X2 complexes

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An overview is given on a study which showed that not only in chemical reactions but also in the favorable case of nontotally symmetric vibrations where the chemical and external potentials keep approximately constant, the generalized maximum hardness principle (GMHP) and generalized minimum polarizability principle (GMPP) may not be obeyed. A method that allows an accurate determination of the nontotally symmetric molecular distortions with more marked GMPP or anti-GMPP character through diagonalization of the polarizability Hessian matrix is introduced

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The level of ab initio theory which is necessary to compute reliable values for the static and dynamic (hyper)polarizabilities of three medium size π-conjugated organic nonlinear optical (NLO) molecules is investigated. With the employment of field-induced coordinates in combination with a finite field procedure, the calculations were made possible. It is stated that to obtain reasonable values for the various individual contributions to the (hyper)polarizability, it is necessary to include electron correlation. Based on the results, the convergence of the usual perturbation treatment for vibrational anharmonicity was examined

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Recently, the surprising result that ab initio calculations on benzene and other planar arenes at correlated MP2, MP3, configuration interaction with singles and doubles (CISD), and coupled cluster with singles and doubles levels of theory using standard Pople’s basis sets yield nonplanar minima has been reported. The planar optimized structures turn out to be transition states presenting one or more large imaginary frequencies, whereas single-determinant-based methods lead to the expected planar minima and no imaginary frequencies. It has been suggested that such anomalous behavior can be originated by two-electron basis set incompleteness error. In this work, we show that the reported pitfalls can be interpreted in terms of intramolecular basis set superposition error (BSSE) effects, mostly between the C–H moieties constituting the arenes. We have carried out counterpoise-corrected optimizations and frequency calculations at the Hartree–Fock, B3LYP, MP2, and CISD levels of theory with several basis sets for a number of arenes. In all cases, correcting for intramolecular BSSE fixes the anomalous behavior of the correlated methods, whereas no significant differences are observed in the single-determinant case. Consequently, all systems studied are planar at all levels of theory. The effect of different intramolecular fragment definitions and the particular case of charged species, namely, cyclopentadienyl and indenyl anions, respectively, are also discussed

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The completion of the sequencing of the mouse genome promises to help predict human genes with greater accuracy. While current ab initio gene prediction programs are remarkably sensitive (i.e., they predict at least a fragment of most genes), their specificity is often low, predicting a large number of false-positive genes in the human genome. Sequence conservation at the protein level with the mouse genome can help eliminate some of those false positives. Here we describe SGP2, a gene prediction program that combines ab initio gene prediction with TBLASTX searches between two genome sequences to provide both sensitive and specific gene predictions. The accuracy of SGP2 when used to predict genes by comparing the human and mouse genomes is assessed on a number of data sets, including single-gene data sets, the highly curated human chromosome 22 predictions, and entire genome predictions from ENSEMBL. Results indicate that SGP2 outperforms purely ab initio gene prediction methods. Results also indicate that SGP2 works about as well with 3x shotgun data as it does with fully assembled genomes. SGP2 provides a high enough specificity that its predictions can be experimentally verified at a reasonable cost. SGP2 was used to generate a complete set of gene predictions on both the human and mouse by comparing the genomes of these two species. Our results suggest that another few thousand human and mouse genes currently not in ENSEMBL are worth verifying experimentally.

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The methodology for generating a homology model of the T1 TCR-PbCS-K(d) class I major histocompatibility complex (MHC) class I complex is presented. The resulting model provides a qualitative explanation of the effect of over 50 different mutations in the region of the complementarity determining region (CDR) loops of the T cell receptor (TCR), the peptide and the MHC's alpha(1)/alpha(2) helices. The peptide is modified by an azido benzoic acid photoreactive group, which is part of the epitope recognized by the TCR. The construction of the model makes use of closely related homologs (the A6 TCR-Tax-HLA A2 complex, the 2C TCR, the 14.3.d TCR Vbeta chain, the 1934.4 TCR Valpha chain, and the H-2 K(b)-ovalbumine peptide), ab initio sampling of CDR loops conformations and experimental data to select from the set of possibilities. The model shows a complex arrangement of the CDR3alpha, CDR1beta, CDR2beta and CDR3beta loops that leads to the highly specific recognition of the photoreactive group. The protocol can be applied systematically to a series of related sequences, permitting the analysis at the structural level of the large TCR repertoire specific for a given peptide-MHC complex.