The formation of base pair radical anions and cations is closely related to many fascinating research fields in biology and chemistry such as genetic mutation, radiation-induced DNA damage and dynamics of charge transfer in DNA. However, the relevant knowledge so far mainly comes from studies on isolated base pair radical anions and cations, and their behavior in the DNA environment is less understood. In this study, we focus on how the nucleobase sequence affects the properties of the guanine¡Vcytosine (G:C) base pair radical anion and cation. The energetic barrier and reaction energy for the proton transfer along the N1(G)¡VH¡E¡E¡EN3(C) hydrogen bond and the stability of (G:C)¡E (i.e., electron affinity and ionization potential of G:C) embedded in different sequences of base-pair trimer were evaluated using density functional theory and two-layer ONIOM method. The computational results demonstrated that the presence of neighboring base pairs has an important influence on the behavior of (G:C)¡E in the gas phase. The excess electron and positive hole were found to be localized on the embedded G:C and the charge leakage to neighboring base pairs was very minor in all of the investigated sequences. Accordingly, the sequence behavior of the proton transfer reaction and the stability of (G:C)¡E is chiefly governed by electrostatic interactions with adjacent base pairs. However, the effect of base stacking, due to its electrostatic nature, is severely screened upon hydration, and thus, the sequence dependence of the properties of (G:C)¡E in aqueous environment becomes relatively weak and less than that observed in the gas phase. The effect of geometry relaxation associated with neighboring base pairs as well as the possibility of proton transfer along the N2(G)¡VH¡E¡E¡EO2(C) channel have also been investigated. The implications of the present findings to the electron transport and radiation damage of DNA are discussed.

No description available.

Single-particle Green's function method is a direct way of calculating electron binding energy, which relies on expanding the Fock subspace in a finite single-particle basis. However, these methods suffer from slow asymptotic decay of basis set incompleteness error. An energy-dependent explicitly correlated (F12) formalism for Green's function is presented that achieves faster convergence to the basis set limit. The renormalized second-order Green's function method (NR2-F12) scales as iterative N^5 where N is the system size. These methods are tested on a set of small (O21) and medium-sized (OAM24) organic molecules. The basis set incompleteness error in ionization potential (IP) obtained from the NR2-F12 method and aug-cc-pVDZ basis for OAM24 is 0.033 eV compared to 0.067 eV for NR2 method and aug-cc-pVQZ basis. Hence, accurate electron binding energies can be calculated at a lower cost using NR2-F12 method. For aug-cc-pVDZ basis, the electron binding energies obtained from NR2-F12 are comparable to EOM-IP-CCSD method that uses a CCSD reference and scales as iterative N^6. / Master of Science / Solving the non-relativistic time-independent Schrödinger equation is a central problem in quantum chemistry with the primary goal of finding the exact electronic wave function. Like all many-body problems, the applications of highly accurate electronic structure methods are limited to small molecules since they are computationally expensive. With scalable algorithms and parallel implementation of computer programs, the chemistry of large molecular systems can be investigated. Electron binding energies give an insight into the orbital picture of a molecule, which is manifested in chemical structure and properties of a molecule. Green’s function provides an alternative to wave function based methods to calculate ionization potential and electron affinity directly rather than solving for the wave function itself. For accurate electron binding energies, the wave function needs to be represented by large number of basis functions, which make these methods computationally expensive. Explicitly correlated electronic structure methods are designed to produce accurate results at a smaller basis set. This work investigates the use of explicitly correlated Green’s function methods to calculate electron binding energies of small and medium sized organic molecules. These results are compared to coupled cluster methods, which are known to provide accurate benchmarks in quantum chemistry.

Neutral gas-phase metal-carbide clusters are generated by laser ablation and are detected in the constructed time-of-flight mass-spectrometer by laser ionisation. Photo-ionisation efficiency (PIE) experiments are performed on the metal-carbide clusters to determine their ionisation potentials (IPs). Complimentary density functional theory (DFT) calculations are performed on the energetically favorable structural isomers of the metalcarbide clusters. Comparison between the calculated IPs of the isomers and the experimental IP allows the carrier of the observed ionisation onset for a metal-carbide cluster to be assigned. The niobium-carbide clusters Nb₃Cy (y = 0–4), Nb₄Cy (y = 0–6) and Nb₅Cy (y = 0–6) are examined by PIE experiments and DFT calculations. The IPs of the niobium-carbide clusters are found to be either left reasonably unchanged from the IPs of the bare metal clusters or moderately reduced. The clusters Nb₃C₂, Nb₄C₄, Nb₅C₂ and Nb₅C₃ display the largest IP reductions for their corresponding cluster series. The structures assigned to the IPs of the Nb₃Cy (y = 1–3) clusters are based on the carbon atoms attaching to the niobium faces and/or niobium-niobium edges of the triangular Nb₃ cluster. However, for Nb₃C₄ the ionisation onset is assigned to a low-lying isomer, which contains a molecular C₂ unit, rather than the lowest energy isomer, a niobium atom deficient 2×2×2 face-centred cubic (fcc) nanocrystal structure. The structures assigned to the IPs of the Nb₄Cy (y = 1–4) clusters are based on the carbon atoms attaching in turn to the niobium faces of the tetrahedral Nb₄ cluster, developing a 2×2×2 fcc nanocrystal structure for Nb₄C₄. For Nb₄C₃ two ionisation onsets are observed; one weak onset at low energy and another more intense onset at high energy. It is proposed that the two onsets are due to ionisation from both a metastable ³A₁ state and the ground ¹A₁ state of the lowest energy isomer. The ionisation onsets of Nb₄C₅ and Nb₄C₆ are also proposed to originate from metastable triplet states of the lowest energy isomers, with the transitions from the ground singlet states calculated to be greater than the highest achievable photon energy in the laboratory. The structures of Nb₄C₅ and Nb₄C₆ have one and two carbon atoms in a 2×2×2 fcc nanocrystal substituted with molecular C₂ units, respectively. The structures assigned to the IPs of the Nb₅Cy (y = 1–6) clusters are based on the underlying Nb₅ cluster being in either a “prolate” or “oblate” trigonal bipyramid geometry; the former has six niobium faces available for carbon addition, while the latter has two niobium butterfly motifs and two niobium faces available for carbon addition. Both the structures of Nb₅C₅ and Nb₅C₆ have the underlying Nb₅ cluster in the oblate trigonal bipyramid geometry and contain one and two molecular C₂ units, respectively. The tantalum-carbide clusters Ta₃Cy (y = 0–3), Ta₄Cy (y = 0–4) and Ta₅Cy (y = 0–6) are examined by PIE experiments and DFT calculations. The IPs of the tantalum-carbide clusters in each series show trends that are very similar to the corresponding iso-valent niobium-carbide cluster series, although the IP reductions upon carbon addition are smaller for the former. For the vast majority of tantalum-carbide clusters, the same structural isomer is assigned to the ionisation onset as that assigned for the corresponding niobium-carbide cluster. Bimetallic tantalum-zirconium-carbide clusters are generated using a constructed double ablation cluster source. The Ta₃ZrCy (y = 0–4) clusters are examined by PIE experiments and DFT calculations. The IP trend for the Ta₃ZrCy cluster series is reasonably similar to that of the Ta₄Cy cluster series, although the IP reductions upon carbon addition are greater for the former. The structures assigned to the IPs of the Ta₃ZrCy (y = 1–4) clusters are based on the carbon atoms attaching in turn to the metal faces of the tetrahedral Ta₃Zr cluster. In summary, the work presented in this thesis demonstrates that the structures of metalcarbide clusters can be inferred by the determination of their IPs through PIE experiments in combination with DFT calculations on candidate structural isomers. / http://proxy.library.adelaide.edu.au/login?url= http://library.adelaide.edu.au/cgi-bin/Pwebrecon.cgi?BBID=1347219 / Thesis (Ph.D.) - University of Adelaide, School of Chemistry and Physics, 2008

Neutral gas-phase metal-carbide clusters are generated by laser ablation and are detected in the constructed time-of-flight mass-spectrometer by laser ionisation. Photo-ionisation efficiency (PIE) experiments are performed on the metal-carbide clusters to determine their ionisation potentials (IPs). Complimentary density functional theory (DFT) calculations are performed on the energetically favorable structural isomers of the metalcarbide clusters. Comparison between the calculated IPs of the isomers and the experimental IP allows the carrier of the observed ionisation onset for a metal-carbide cluster to be assigned. The niobium-carbide clusters Nb₃Cy (y = 0–4), Nb₄Cy (y = 0–6) and Nb₅Cy (y = 0–6) are examined by PIE experiments and DFT calculations. The IPs of the niobium-carbide clusters are found to be either left reasonably unchanged from the IPs of the bare metal clusters or moderately reduced. The clusters Nb₃C₂, Nb₄C₄, Nb₅C₂ and Nb₅C₃ display the largest IP reductions for their corresponding cluster series. The structures assigned to the IPs of the Nb₃Cy (y = 1–3) clusters are based on the carbon atoms attaching to the niobium faces and/or niobium-niobium edges of the triangular Nb₃ cluster. However, for Nb₃C₄ the ionisation onset is assigned to a low-lying isomer, which contains a molecular C₂ unit, rather than the lowest energy isomer, a niobium atom deficient 2×2×2 face-centred cubic (fcc) nanocrystal structure. The structures assigned to the IPs of the Nb₄Cy (y = 1–4) clusters are based on the carbon atoms attaching in turn to the niobium faces of the tetrahedral Nb₄ cluster, developing a 2×2×2 fcc nanocrystal structure for Nb₄C₄. For Nb₄C₃ two ionisation onsets are observed; one weak onset at low energy and another more intense onset at high energy. It is proposed that the two onsets are due to ionisation from both a metastable ³A₁ state and the ground ¹A₁ state of the lowest energy isomer. The ionisation onsets of Nb₄C₅ and Nb₄C₆ are also proposed to originate from metastable triplet states of the lowest energy isomers, with the transitions from the ground singlet states calculated to be greater than the highest achievable photon energy in the laboratory. The structures of Nb₄C₅ and Nb₄C₆ have one and two carbon atoms in a 2×2×2 fcc nanocrystal substituted with molecular C₂ units, respectively. The structures assigned to the IPs of the Nb₅Cy (y = 1–6) clusters are based on the underlying Nb₅ cluster being in either a “prolate” or “oblate” trigonal bipyramid geometry; the former has six niobium faces available for carbon addition, while the latter has two niobium butterfly motifs and two niobium faces available for carbon addition. Both the structures of Nb₅C₅ and Nb₅C₆ have the underlying Nb₅ cluster in the oblate trigonal bipyramid geometry and contain one and two molecular C₂ units, respectively. The tantalum-carbide clusters Ta₃Cy (y = 0–3), Ta₄Cy (y = 0–4) and Ta₅Cy (y = 0–6) are examined by PIE experiments and DFT calculations. The IPs of the tantalum-carbide clusters in each series show trends that are very similar to the corresponding iso-valent niobium-carbide cluster series, although the IP reductions upon carbon addition are smaller for the former. For the vast majority of tantalum-carbide clusters, the same structural isomer is assigned to the ionisation onset as that assigned for the corresponding niobium-carbide cluster. Bimetallic tantalum-zirconium-carbide clusters are generated using a constructed double ablation cluster source. The Ta₃ZrCy (y = 0–4) clusters are examined by PIE experiments and DFT calculations. The IP trend for the Ta₃ZrCy cluster series is reasonably similar to that of the Ta₄Cy cluster series, although the IP reductions upon carbon addition are greater for the former. The structures assigned to the IPs of the Ta₃ZrCy (y = 1–4) clusters are based on the carbon atoms attaching in turn to the metal faces of the tetrahedral Ta₃Zr cluster. In summary, the work presented in this thesis demonstrates that the structures of metalcarbide clusters can be inferred by the determination of their IPs through PIE experiments in combination with DFT calculations on candidate structural isomers. / http://proxy.library.adelaide.edu.au/login?url= http://library.adelaide.edu.au/cgi-bin/Pwebrecon.cgi?BBID=1347219 / Thesis (Ph.D.) - University of Adelaide, School of Chemistry and Physics, 2008

Nos últimos 20 anos, a espectroscopia de emissão ótica com plasma induzido a laser (LIBS) tem se tornado uma das mais promissoras ferramentas em química analítica, cujas aplicações são destinadas às análises multi-elementares em amostras nos estados sólido, líquido e gasoso. Suas aplicações são as mais diversas, pois sua instrumentação é relativamente simples e pode ser portátil. Em especial, a LIBS apresenta grande potencial de uso na agricultura, com diversas publicações que exploram, principalmente, a concentração de carbono em solos. Entretanto, a construção de modelos gerais de calibração é uma das maiores dificuldades da técnica, pois ela está suscetível aos efeitos de matriz que adicionam comportamentos não-lineares às intensidades das emissões. Com intuito de compreender quais são as principais causas dessa dependência, este trabalho avaliou relações entre propriedades físicas do plasma LIBS e as inclinações das curvas de calibração para cinco emissões de carbono em amostras sintéticas de diferentes potenciais de ionização, sendo elas KCl e H3BO3 com 1% de CuSO4 e concentrações entre 0 e 10 % de carbono. Constatou-se que temperatura e densidade de elétrons dependem inversamente da concentração de carbono nas amostras, o que provavelmente está associado às taxas de ablação de material da amostra e recombinação no interior do plasma. Ademais, esses parâmetros em plasmas originados das amostras de KCl + CuSO4 são maiores do que para a matriz de H3BO3 + CuSO4, além de que apenas plasmas originados da primeira matriz satisfizeram o critério de McWhirter para C I, Cu I e Cu II em todas as concentrações de carbono, indicando que eles devem apresentar condições de equilíbrio termodiâmico local. O mesmo não foi obtido para o caso da matriz de H3BO3 + CuSO4, o que pode explicar suas elevadas incertezas nos valores da temperatura e densidade de elétrons. Verificou-se ainda que as inclinações das curvas de calibração para o carbono foram maiores para o caso da matriz com elementos majoritários de menor potencial de ionização e que isso está diretamente relacionado às propriedades intrínsecas dos plasmas originados, o que corrobora a hipótese deste trabalho. Além disso, cálculos de correlação entre a área do pico de carbono em 247,89 nm e cada ponto dos espectros LIBS mostraram que a emissão de Cu II em 224,72 nm linearizou as curvas de calibração, minimizando os efeitos de matriz. Por fim, este trabalho contribuiu tanto com avanços no conhecimento até então existente a respeito dos efeitos de matriz quanto com um eficiente conjunto de técnicas analíticas para espectros, cujo potencial de aplicação é enorme. / In the last 20 years, laser-induced breakdown spectroscopy (LIBS) has been one of the main tools in analytical chemistry, whose applications are destinated to multi-elementar analysis in solid, liquid or gaseous samples. Its use is diverse, since its instrumentation is relatively simple and can be portable. In particular, LIBS has a great potential for use in agriculture, with many publications that explore mainly the carbon concentration in soils. However, the construction of general calibration models is one of the greatest difficulties of the technique, since it is susceptible to matrix effects that add non-linear behaviors to the emission intensities. In order to understand the main causes of this dependence, this study evaluated the relationships between physical properties of the LIBS plasma and the slope of the calibration curves for carbon emissions in synthetic samples with different ionization potentials. Those samples were made of KCl and H3BO3 with 1% of CuSO4 and carbon concentrations ranging from 0 to 10%. It was found that the plasma temperature and electron density are inversely proportional to the carbon concentration in the samples, which is probably associated with rates of sample ablation and recombination within the plasma. In addition, these parameters in plasmas originating from the samples of KCl + CuSO4 are larger than those originating from the matrix of H3BO3 + CuSO4 at all carbon concentrations, indicating that the first matrix must be in local thermodynamics equilibrium. However, similar results were not found for the other matrix which may explain its high uncertainties in the values of temperature and electron density. It was verified that the slope of the carbon calibration curves were higher for the matrix with elements of low ionization potential than for the other matrix and that this is directly related to the intrinsic properties the plasmas originated, which corroborates the hypothesis of this study. Furthermore, the analysis of correlation between the carbon peak area at 247.89 nm and each point of the LIBS spectra have shown that the Cu II emission at 224.72 nm linearized the calibration curves, minimizing the matrix effects. Finally, this study contributed with advances in the knowledge about matrix effects and with an efficient set of analytical tools for spectra whose application potential is huge.

Nos últimos 20 anos, a espectroscopia de emissão ótica com plasma induzido a laser (LIBS) tem se tornado uma das mais promissoras ferramentas em química analítica, cujas aplicações são destinadas às análises multi-elementares em amostras nos estados sólido, líquido e gasoso. Suas aplicações são as mais diversas, pois sua instrumentação é relativamente simples e pode ser portátil. Em especial, a LIBS apresenta grande potencial de uso na agricultura, com diversas publicações que exploram, principalmente, a concentração de carbono em solos. Entretanto, a construção de modelos gerais de calibração é uma das maiores dificuldades da técnica, pois ela está suscetível aos efeitos de matriz que adicionam comportamentos não-lineares às intensidades das emissões. Com intuito de compreender quais são as principais causas dessa dependência, este trabalho avaliou relações entre propriedades físicas do plasma LIBS e as inclinações das curvas de calibração para cinco emissões de carbono em amostras sintéticas de diferentes potenciais de ionização, sendo elas KCl e H3BO3 com 1% de CuSO4 e concentrações entre 0 e 10 % de carbono. Constatou-se que temperatura e densidade de elétrons dependem inversamente da concentração de carbono nas amostras, o que provavelmente está associado às taxas de ablação de material da amostra e recombinação no interior do plasma. Ademais, esses parâmetros em plasmas originados das amostras de KCl + CuSO4 são maiores do que para a matriz de H3BO3 + CuSO4, além de que apenas plasmas originados da primeira matriz satisfizeram o critério de McWhirter para C I, Cu I e Cu II em todas as concentrações de carbono, indicando que eles devem apresentar condições de equilíbrio termodiâmico local. O mesmo não foi obtido para o caso da matriz de H3BO3 + CuSO4, o que pode explicar suas elevadas incertezas nos valores da temperatura e densidade de elétrons. Verificou-se ainda que as inclinações das curvas de calibração para o carbono foram maiores para o caso da matriz com elementos majoritários de menor potencial de ionização e que isso está diretamente relacionado às propriedades intrínsecas dos plasmas originados, o que corrobora a hipótese deste trabalho. Além disso, cálculos de correlação entre a área do pico de carbono em 247,89 nm e cada ponto dos espectros LIBS mostraram que a emissão de Cu II em 224,72 nm linearizou as curvas de calibração, minimizando os efeitos de matriz. Por fim, este trabalho contribuiu tanto com avanços no conhecimento até então existente a respeito dos efeitos de matriz quanto com um eficiente conjunto de técnicas analíticas para espectros, cujo potencial de aplicação é enorme. / In the last 20 years, laser-induced breakdown spectroscopy (LIBS) has been one of the main tools in analytical chemistry, whose applications are destinated to multi-elementar analysis in solid, liquid or gaseous samples. Its use is diverse, since its instrumentation is relatively simple and can be portable. In particular, LIBS has a great potential for use in agriculture, with many publications that explore mainly the carbon concentration in soils. However, the construction of general calibration models is one of the greatest difficulties of the technique, since it is susceptible to matrix effects that add non-linear behaviors to the emission intensities. In order to understand the main causes of this dependence, this study evaluated the relationships between physical properties of the LIBS plasma and the slope of the calibration curves for carbon emissions in synthetic samples with different ionization potentials. Those samples were made of KCl and H3BO3 with 1% of CuSO4 and carbon concentrations ranging from 0 to 10%. It was found that the plasma temperature and electron density are inversely proportional to the carbon concentration in the samples, which is probably associated with rates of sample ablation and recombination within the plasma. In addition, these parameters in plasmas originating from the samples of KCl + CuSO4 are larger than those originating from the matrix of H3BO3 + CuSO4 at all carbon concentrations, indicating that the first matrix must be in local thermodynamics equilibrium. However, similar results were not found for the other matrix which may explain its high uncertainties in the values of temperature and electron density. It was verified that the slope of the carbon calibration curves were higher for the matrix with elements of low ionization potential than for the other matrix and that this is directly related to the intrinsic properties the plasmas originated, which corroborates the hypothesis of this study. Furthermore, the analysis of correlation between the carbon peak area at 247.89 nm and each point of the LIBS spectra have shown that the Cu II emission at 224.72 nm linearized the calibration curves, minimizing the matrix effects. Finally, this study contributed with advances in the knowledge about matrix effects and with an efficient set of analytical tools for spectra whose application potential is huge.

No description available.

Submitted by Cláudia Bueno (claudiamoura18@gmail.com) on 2015-10-29T18:35:28Z No. of bitstreams: 2 Tese - Jose Higino Damasceno Junior - 2015.pdf: 2058291 bytes, checksum: ed4c947cd5e0f908dddc93570ac84dbb (MD5) license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) / Approved for entry into archive by Luciana Ferreira (lucgeral@gmail.com) on 2015-11-03T14:21:33Z (GMT) No. of bitstreams: 2 Tese - Jose Higino Damasceno Junior - 2015.pdf: 2058291 bytes, checksum: ed4c947cd5e0f908dddc93570ac84dbb (MD5) license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) / Made available in DSpace on 2015-11-03T14:21:33Z (GMT). No. of bitstreams: 2 Tese - Jose Higino Damasceno Junior - 2015.pdf: 2058291 bytes, checksum: ed4c947cd5e0f908dddc93570ac84dbb (MD5) license_rdf: 23148 bytes, checksum: 9da0b6dfac957114c6a7714714b86306 (MD5) Previous issue date: 2015-09-25 / Fundação de Amparo à Pesquisa do Estado de Goiás - FAPEG / Clusters systems are very different from molecules or their bulk materials, since they exhibit many specific properties. As example, the bond in metallic clusters of metallic atoms is intermediate between metallic and covalent bonding. In general, the structural and electronic properties of these systems are very difficult to measure experimentally, and therefore theoretical modeling is very important in characterizing them. In this thesis, we employed ab initio methods to study metallic clusters such as the aluminum hydride clusters as well as a few aromatic metal clusters. The optimized geometries of the studied clusters have been determined using DFT. The electronic structures of these systems were investigated using the QMC methods. The calculations were carried out within the Variational (VMC) and fixed-node diffusion (DMC) quantum Monte Carlo methods. The calculations are also performed in the Hartree-Fock (HF) approximation in order to analyze the impact of electron correlation. With regards the aluminum hydride clusters, the total atomic binding energy impact varies from ~20% up to about ~50%, whereas for the electron binding energy it ranges from ~1% up to ~73%. The decomposition of the electron binding energies clearly shows that both charge redistribution and electron correlation are important in determining the detachment energies, whereas electrostatic and exchange interactions are responsible for the ionization potential. For the aromatic metal clusters, the presence of a dopant plays important role in their electronic properties enhancing their binding energy, electron affinity, hardness and resonance energy. / Clusters são sistemas bastante diferentes de moléculas e sólidos, pois exibem propriedades bastante peculiares. Por exemplo, a ligação em um cluster metálico tem intensidade intermediária entre as ligações covalentes e metálicas. Em geral, as propriedades eletrônicas e estruturais desses sistemas são bastante difíceis de serem medidas experimentalmente e, portanto, uma modelagem teórica é muito importante na caracterização desses. Nesta Tese, utilizamos métodos ab initio para estudar clusters metálicos, tal como clusters de hidretos de alumínio assim como também alguns clusters metálicos aromáticos. As estruturas geométricas dos clusters estudados foram otimizadas via DFT. A estrutura eletrônica desses clusters foi investigada usando o método de Monte Carlo Quântico Variacional (MCQD) e de difusão (MCQD) com aproximação de nós fixos. Os cálculos também foram realizados a partir da aproximação de Hartree-Fock, afim de se analisar o impacto da energia de correlação eletrônica. Para os hidretos de alumínio, a energia de correlação eletrônica tem impacto na energia total de ligação variando de 20% a 50%. Da mesma maneira, a energia de ligação de um elétron ao cluster tem grande contribuição da energia de correlação eletrônica, variando de 1% a 73%. A decomposição da energia de ligação mostra claramente que a relaxação e a correlação eletrônica são importantes na determinação da afinidade eletrônica, enquanto que a interação de troca eletrostática é responsável pelo potencial de ionização. Para os clusters aromáticos, a presença do dopante desempenha um importante papel nas propriedades desses clusters, uma vez que otimiza a energia de ligação, a afinidade eletrônica, a dureza e a energia de ressonância.

Aqueous solutions were studied using photoelectron and Auger spectroscopy, based on synchrotron radiation and a liquid micro-jet setup. By varying the photon energy in photoelectron spectra, we depth profiled an aqueous tetrabutylammonium iodide (TBAI) solution. Assuming uniform angular emission from the core levels, we found that the TBA+ ions were oriented at the surface with the hydrophobic butyl arms sticking into the liquid. We investigated the association between ions and their neighbors in aqueous solutions by studying the electronic decay after core ionization. The (2p)−1 decay of solvated K+ and Ca2+ ions was studied. The main features in the investigated decay spectra corresponded to two-hole final states localized on the ions. The spectra also showed additional features, related to delocalized two-hole final states with vacancies on a cation and a neighboring water molecule. These two processes compete, and by comparing relative intensities and using the known rate for the localized decay, we determined the time-scale for the delocalized process for the two ions. We compared to delocalized electronic decay processes in Na+, Mg2+, and Al3+, and found that they were slower in K+ and Ca2+, due to different internal decay mechanisms of the ions, as well as external differences in the ion-solute distances and interactions. In the O 1s Auger spectra of aqueous metal halide solutions, we observed features related to delocalized two-hole final states with vacancies on a water molecule and a neighboring solvated anion. The relative intensity of these feature indicated that the strength of the interaction between the halide ions and water correlated with ionic size. The delocalized decay was also used to investigate contact ion pair formation in high concentrated potassium halide solutions, but no concrete evidence of contact ion pairs was observed. / Felaktigt tryckt som Digital Comprehensive Summaries of Uppsala Dissertations from the Faculty of Science and Technology 726