Unrestricted Kohn-Sham (broken symmetry) density functional calculations have been used to determine the low-energy geometries of the chromium dihalide molecules (CrX2) and their clusters, Cr2X4, Cr3X6, and Cr4X8. The monomers are also investigated at a higher level, including coupled-cluster and state-average CASSCF computations. Our calculations show that the monomers have a 5B2 ground state arising from the Renner-Teller distorted 5IIg transition state, leading to a bent geometry. The global minima of the gas-phase clusters of CrF2 and CrCl2 consist of two-dimensional, anti-ferromagnetically coupled chains of CrX2 units forming four-membered, doubly bridged Cr2X2 rings, closely resembling their solid-state structures. The global minima of the CrBr2 and CrI2 clusters consist of the same two-dimensional chain-like structures for their dimers, but their trimers and tetramers consist of three-dimensional ’triangular’ structures which contain two capping ligands bound to three chromium atoms along with a Cr-Cr bond. Each Cr atom within these clusters has spin quantum number S=2. There is approximately a constant change in energy, between 45-55 kcal/mol, with every new CrX2 unit during cluster formation. Information about the structure of the CrCl2 clusters is used in the reanalysis of high-temperature electron diffraction data. The vapor at 1170 K contains about 77% monomeric molecules, 19% dimers, and a small amount of trimers. Monomeric CrCl2 is found to be bent with a bond angle of 149(10)degrees, in good agreement with our computations. Solid-state DFT calculations are performed on alpha-CrCl2 to determine the lattice structure and spin-coupling constants for the Cr atoms within the crystals. The GGA (PW91) method produces a structure in good agreement with the literature. In the lowest energy structure, the spins of the Cr atoms within the chains along the crystallographic c-axis are anti-ferromagnetically coupled with four parallel spins situated almost exclusively in the d-bands of Cr along these chains. This anti-ferromagnetic coupling is also seen in the CrX2 clusters.

This study concerns the synthesis, structure and reactivity of nitrosyl complexes of ruthenium and osmium. Attempts have been made to prepare coordinatively saturated and unsaturated complexes and a study of their oxidative addition reactions bears considerable resemblance to the more familiar carbonyl complexes M(CO)3(PPh3)2. A number of interesting atom transfer reactions, generally involving oxygen, have been observed. The d8 complex RuCl(CO)(NO)(PPh3)2 results from the interaction of RuHCl(CO)(PPh3)3 with N-methyl-N-nitrosotoluene-p-sulphonamide. The labile halide ligand is readily displaced by a large range of anions and it is believed that both linear and bent nitrosyl linkages may exist for different members of this series. The structures of these complexes are discussed in the light of recent X-ray crystal structure data. Halogens and hydrogen halides add to give the familiar RuX3(NO)(PPh3)2; RuCl3(NO)(PPh2Me)2 is prepared in a direct reaction and also by phosphine exchange and 1H n.m.r. data confirm that the phosphine ligands are trans. The complexes RuX(CO)(NO)(PPh3)2 react readily with O2 to form the dioxygen complexes Ru(O2)X(NO)(PPh3)2. Halogens and hydrogen halides produce RuX3(NO)(PPh3)2. The dioxygen complexes react with SO2 and N2O4 to give sulphato and dinitrato complexes respectively. The reaction with CO results in the intramolecular oxidation of the nitrosyl group to coordinated nitrate accompanied by the incorporation of two moles of CO, i.e. RuX(NO3)(CO)2(PPh3)2 is formed. The dioxygen complexes catalytically oxidise triphenylphosphine or triphenylarsine to the respective oxides and RuX(NO)(PPh3)2 can be isolated from this cycle. Reactions of these four-coordinated complexes with O2, CO, Cl2 and NOBF4 are recorded. The dinitrosyl complex Ru(NO)2(PPh3)2 is reported from a number of syntheses, the most successful being via a ligand reaction when RuCl2(CO)2(PPh3)2 is heated with NaNO2 and Ph3P in dimethyl formamide. The P-tolyldiphenylphosphine analogue is also reported and the mono-substituted product Ru(NO)2(PPh3)[P(OPh)3] is produced in an exchange reaction between Ru(NO)2(PPh3)2 and excess triphenylphosphite. This phosphite complex reacts with Ph3P and O2 to produce Ru(O2)(NO2)(NO)PPh3)2 by an atom transfer process. Ru(NO)2(PPh3)2 reacts with the acids HY (Y = BF4, PF6, ClO4) and O2 to give the dinitrosyl cations [Ru(OH)(NO)2(PPh3)2]+Y- in which the two nitrosyl groups are structurally and electronically inequivalent. [RuCl(NO)2(PPh3)2]BF4 is reported and reactions of these dinitrosyl cations with halide ions to give RuX2(NO3)(NO)(PPh3)2, with intramolecular oxidation of the NO group, are also described. OsCl2(OH)(NO)(PPh3)2 reacts irreversibly with alcohols to form OsCl2(OR)(NO)(PPh3)2 (R = CH3, C2H5, n-C3H7, (CH3O)CH2CH2) which readily undergo hydride abstraction to form OsHCl2(NO)(PPh3)2. Sodium borohydride converts this complex to the trihydrido species OsH3(NO)(PPh3)2 and if the reaction is performed in the presence of Ph3P, OsH(NO)(PPh3)3 results. The coordinated perchlorate complex OsHCl(OClO3)(NO)(PPh3)2 results form the reaction of OsHCl2(NO)(PPh3)2 with silver perchlorate; this is readily reversed by chloride ions or the solvents CH2Cl2 and CHCl3. This perchlorato complex also arises from the reaction of OsH(CO)(NO)(PPh3)2 with HClO4 and a related tetrafluoroborato complex, OsH(OC2H5)(FBF3)(NO)(PPh3)2 by substituting HBF4. This complex reacts with Ph3P to give [OsH(OH)(NO)(PPh3)3]BF4, CO to give [Os(CO)2(NO)(PPh3)2]BF4 and LiX (X = Br, I) to give OsHX2(NO)(PPh3)2. OsHCl(OClO3)(NO)(PPh3)2 reacts with NaOH in methanol, in the presence of O2 to produce Os(O2)Cl(NO)(PPh3)2. This dioxygen complex is far less stable than the ruthenium analogue but it undergoes similar reactions. Ph3P is oxidised, SO2 and CO give sulphato and a nitratodicarbonyl complex respectively. Infra-red, 1H n.m.r., conductivity, molecular weight data and elemental analysis have been used in formulation and structural assignment.

Data is presented for a range of experiments that have been performed using a selected ion flow tube (SIFT) instrument operated at room temperature (~ 298K) with carrier gas pressures typically in the range of 0.3 – 0.6 Torr. The majority of the experiments discussed are performed on a Voice100 instrument that has not been described in detail previously. The Voice100 is a novel instrument that has been designed particularly for quantitative trace gas analysis using the SIFT-MS technique. A mixture of helium and argon carrier gases are employed in the Voice100 flow tube. By mixing carrier gases, the flow dynamics and diffusion characteristics of a flow tube are altered when compared to classic single carrier gas models. Therefore firstly, optimal flow conditions for the operation of a Voice100 are characterised. The diffusion of an ion in a mixture of carrier gases is then characterised using theoretical models and experimental techniques. This research requires that a new parameter Mp be defined regarding the mass discrimination of an ion in the non-field-free region near the downstream ion sampling orifice. Furthermore, a new method is described for the simultaneous measurement of rate coefficients for the reactions of H₃O⁺.(H₂O)n (n = 1, 2, 3) ions with analytes. Rate coefficients and branching ratios for the reactions of SIFT-MS precursor ions with specific analytes related to four individual applications are presented. For each application, the kinetic parameters are determined so as to facilitate the quantitative detection of the analytes relevant to that application. The GeoVOC application involves the measurement of hydrocarbon concentrations in the headspace of soil and water across a range of humidities. Alkyl esters are investigated to allow for the quantitative detection of each compound in fruits and vegetables. Chemical warfare agents, their surrogates and precursor compounds are studied which allows for the quantitative or semi-quantitative detection of a range of highly toxic compounds. Finally, 17 compounds classified by the US-EPA as hazardous air pollutants are studied that enables SIFT-MS instruments to replicate sections of the TO-14A and TO-15 methods.

This study concerns the synthesis, structure and reactivity of nitrosyl complexes of ruthenium and osmium. Attempts have been made to prepare coordinatively saturated and unsaturated complexes and a study of their oxidative addition reactions bears considerable resemblance to the more familiar carbonyl complexes M(CO)3(PPh3)2. A number of interesting atom transfer reactions, generally involving oxygen, have been observed. The d8 complex RuCl(CO)(NO)(PPh3)2 results from the interaction of RuHCl(CO)(PPh3)3 with N-methyl-N-nitrosotoluene-p-sulphonamide. The labile halide ligand is readily displaced by a large range of anions and it is believed that both linear and bent nitrosyl linkages may exist for different members of this series. The structures of these complexes are discussed in the light of recent X-ray crystal structure data. Halogens and hydrogen halides add to give the familiar RuX3(NO)(PPh3)2; RuCl3(NO)(PPh2Me)2 is prepared in a direct reaction and also by phosphine exchange and 1H n.m.r. data confirm that the phosphine ligands are trans. The complexes RuX(CO)(NO)(PPh3)2 react readily with O2 to form the dioxygen complexes Ru(O2)X(NO)(PPh3)2. Halogens and hydrogen halides produce RuX3(NO)(PPh3)2. The dioxygen complexes react with SO2 and N2O4 to give sulphato and dinitrato complexes respectively. The reaction with CO results in the intramolecular oxidation of the nitrosyl group to coordinated nitrate accompanied by the incorporation of two moles of CO, i.e. RuX(NO3)(CO)2(PPh3)2 is formed. The dioxygen complexes catalytically oxidise triphenylphosphine or triphenylarsine to the respective oxides and RuX(NO)(PPh3)2 can be isolated from this cycle. Reactions of these four-coordinated complexes with O2, CO, Cl2 and NOBF4 are recorded. The dinitrosyl complex Ru(NO)2(PPh3)2 is reported from a number of syntheses, the most successful being via a ligand reaction when RuCl2(CO)2(PPh3)2 is heated with NaNO2 and Ph3P in dimethyl formamide. The P-tolyldiphenylphosphine analogue is also reported and the mono-substituted product Ru(NO)2(PPh3)[P(OPh)3] is produced in an exchange reaction between Ru(NO)2(PPh3)2 and excess triphenylphosphite. This phosphite complex reacts with Ph3P and O2 to produce Ru(O2)(NO2)(NO)PPh3)2 by an atom transfer process. Ru(NO)2(PPh3)2 reacts with the acids HY (Y = BF4, PF6, ClO4) and O2 to give the dinitrosyl cations [Ru(OH)(NO)2(PPh3)2]+Y- in which the two nitrosyl groups are structurally and electronically inequivalent. [RuCl(NO)2(PPh3)2]BF4 is reported and reactions of these dinitrosyl cations with halide ions to give RuX2(NO3)(NO)(PPh3)2, with intramolecular oxidation of the NO group, are also described. OsCl2(OH)(NO)(PPh3)2 reacts irreversibly with alcohols to form OsCl2(OR)(NO)(PPh3)2 (R = CH3, C2H5, n-C3H7, (CH3O)CH2CH2) which readily undergo hydride abstraction to form OsHCl2(NO)(PPh3)2. Sodium borohydride converts this complex to the trihydrido species OsH3(NO)(PPh3)2 and if the reaction is performed in the presence of Ph3P, OsH(NO)(PPh3)3 results. The coordinated perchlorate complex OsHCl(OClO3)(NO)(PPh3)2 results form the reaction of OsHCl2(NO)(PPh3)2 with silver perchlorate; this is readily reversed by chloride ions or the solvents CH2Cl2 and CHCl3. This perchlorato complex also arises from the reaction of OsH(CO)(NO)(PPh3)2 with HClO4 and a related tetrafluoroborato complex, OsH(OC2H5)(FBF3)(NO)(PPh3)2 by substituting HBF4. This complex reacts with Ph3P to give [OsH(OH)(NO)(PPh3)3]BF4, CO to give [Os(CO)2(NO)(PPh3)2]BF4 and LiX (X = Br, I) to give OsHX2(NO)(PPh3)2. OsHCl(OClO3)(NO)(PPh3)2 reacts with NaOH in methanol, in the presence of O2 to produce Os(O2)Cl(NO)(PPh3)2. This dioxygen complex is far less stable than the ruthenium analogue but it undergoes similar reactions. Ph3P is oxidised, SO2 and CO give sulphato and a nitratodicarbonyl complex respectively. Infra-red, 1H n.m.r., conductivity, molecular weight data and elemental analysis have been used in formulation and structural assignment.

This study concerns the synthesis, structure and reactivity of nitrosyl complexes of ruthenium and osmium. Attempts have been made to prepare coordinatively saturated and unsaturated complexes and a study of their oxidative addition reactions bears considerable resemblance to the more familiar carbonyl complexes M(CO)3(PPh3)2. A number of interesting atom transfer reactions, generally involving oxygen, have been observed. The d8 complex RuCl(CO)(NO)(PPh3)2 results from the interaction of RuHCl(CO)(PPh3)3 with N-methyl-N-nitrosotoluene-p-sulphonamide. The labile halide ligand is readily displaced by a large range of anions and it is believed that both linear and bent nitrosyl linkages may exist for different members of this series. The structures of these complexes are discussed in the light of recent X-ray crystal structure data. Halogens and hydrogen halides add to give the familiar RuX3(NO)(PPh3)2; RuCl3(NO)(PPh2Me)2 is prepared in a direct reaction and also by phosphine exchange and 1H n.m.r. data confirm that the phosphine ligands are trans. The complexes RuX(CO)(NO)(PPh3)2 react readily with O2 to form the dioxygen complexes Ru(O2)X(NO)(PPh3)2. Halogens and hydrogen halides produce RuX3(NO)(PPh3)2. The dioxygen complexes react with SO2 and N2O4 to give sulphato and dinitrato complexes respectively. The reaction with CO results in the intramolecular oxidation of the nitrosyl group to coordinated nitrate accompanied by the incorporation of two moles of CO, i.e. RuX(NO3)(CO)2(PPh3)2 is formed. The dioxygen complexes catalytically oxidise triphenylphosphine or triphenylarsine to the respective oxides and RuX(NO)(PPh3)2 can be isolated from this cycle. Reactions of these four-coordinated complexes with O2, CO, Cl2 and NOBF4 are recorded. The dinitrosyl complex Ru(NO)2(PPh3)2 is reported from a number of syntheses, the most successful being via a ligand reaction when RuCl2(CO)2(PPh3)2 is heated with NaNO2 and Ph3P in dimethyl formamide. The P-tolyldiphenylphosphine analogue is also reported and the mono-substituted product Ru(NO)2(PPh3)[P(OPh)3] is produced in an exchange reaction between Ru(NO)2(PPh3)2 and excess triphenylphosphite. This phosphite complex reacts with Ph3P and O2 to produce Ru(O2)(NO2)(NO)PPh3)2 by an atom transfer process. Ru(NO)2(PPh3)2 reacts with the acids HY (Y = BF4, PF6, ClO4) and O2 to give the dinitrosyl cations [Ru(OH)(NO)2(PPh3)2]+Y- in which the two nitrosyl groups are structurally and electronically inequivalent. [RuCl(NO)2(PPh3)2]BF4 is reported and reactions of these dinitrosyl cations with halide ions to give RuX2(NO3)(NO)(PPh3)2, with intramolecular oxidation of the NO group, are also described. OsCl2(OH)(NO)(PPh3)2 reacts irreversibly with alcohols to form OsCl2(OR)(NO)(PPh3)2 (R = CH3, C2H5, n-C3H7, (CH3O)CH2CH2) which readily undergo hydride abstraction to form OsHCl2(NO)(PPh3)2. Sodium borohydride converts this complex to the trihydrido species OsH3(NO)(PPh3)2 and if the reaction is performed in the presence of Ph3P, OsH(NO)(PPh3)3 results. The coordinated perchlorate complex OsHCl(OClO3)(NO)(PPh3)2 results form the reaction of OsHCl2(NO)(PPh3)2 with silver perchlorate; this is readily reversed by chloride ions or the solvents CH2Cl2 and CHCl3. This perchlorato complex also arises from the reaction of OsH(CO)(NO)(PPh3)2 with HClO4 and a related tetrafluoroborato complex, OsH(OC2H5)(FBF3)(NO)(PPh3)2 by substituting HBF4. This complex reacts with Ph3P to give [OsH(OH)(NO)(PPh3)3]BF4, CO to give [Os(CO)2(NO)(PPh3)2]BF4 and LiX (X = Br, I) to give OsHX2(NO)(PPh3)2. OsHCl(OClO3)(NO)(PPh3)2 reacts with NaOH in methanol, in the presence of O2 to produce Os(O2)Cl(NO)(PPh3)2. This dioxygen complex is far less stable than the ruthenium analogue but it undergoes similar reactions. Ph3P is oxidised, SO2 and CO give sulphato and a nitratodicarbonyl complex respectively. Infra-red, 1H n.m.r., conductivity, molecular weight data and elemental analysis have been used in formulation and structural assignment.

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This study concerns halogen bonding between small molecules. Except where otherwise stated herein this investigation was performed exclusively using the M06-2X density functional, in conjunction with the 6-31+G* basis set except for iodine and astatine which were treated using the aug-cc-pVDZ-PP basis set with relativistic pseudopotentials. All calculations were performed in the gas phase. The counterpoise procedure was employed for all full geometry optimisations. Statistical analysis of the Cambridge Structural Database, wherein the frequency of structures as a function of halogen bond angle and distance constituted the sole part of this study not to be based on density functional theory. Except in chapter 5, all halogens from fluorine to astatine are investigated. In chapter 3, halogen bonding between halobenzene and a single water molecule is discussed. Competition between R – X•••OH2 halogen bonding and R – X•••H-O-H hydrogen bonding interactions is described. This system is analogous to the more elaborate microsolvated 1- methyl-5-halouracil system described in chapter 4. In this latter system one 1-methyl-5- halouracil molecule interacts with either one or two water molecules. A central feature of the investigation into this system is competition between R – X•••OH2 and R=O•••H-O-H hydrogen bonding. In chapter 5, halogen bonding is discussed in the context of the thyroid system. In particular halogen bonding between a thyroxine iodine atom and the protein backbone as well as crystal water molecules is the subject of this chapter. The effect of substitution of the iodine atom with an astatine atom is presented. Chapter 6 is concerned with halogen bonding in halogenated DNA base pairs. Interaction energies are compared with those of the canonical base pairs, and the effect of halogen bonding on geometry is also discussed. For each system, halogen bonding was found to become stronger and more tolerant of non- linear bond angles going down the halogen group.

The technology employed by human beings for the generation, storage and usage of energy is presently undergoing the fastest and most profound change since the industrial revolution. The changes in the generation and usage of energy necessitate the development of new methods of energy storage. In these systems, electrochemical energy storage will play a crucial role and to this end new electrolytes need to be explored to complement these changes. One such class of liquids is ionic liquids, a class of salts that are molten at room temperature. These liquids have a broad applicability to batteries and supercapacitors. This thesis details work where molecular dynamics simulations have been used to explore the nanostructure of ionic liquids and their mixtures with various molecular solvents at simplistic electrodes. The thesis has two broad sections. The first is covered in Chapter 3, and explores the nanostructure of ionic liquid propylene carbonate solutions, developing a framework through which these nanostructures can be understood. The section concludes that the increasing dilution of ionic liquids decreases the surface charge at which the characteristic ionic liquid oscillatory interfacial structure gives way to a different structure featuring monotonic charge decay. The behaviour of ionic liquids at interfaces is found to be correlated to ion size and type, as well as concentration. A wide divergence in the observed behaviour is shown at positive and negative electrodes due to the asymmetry of propylene carbonate. The second section, consisting of two chapters, explores the interfacial nanostructure of solvate ionic liquids using two different boundary conditions to model the electrode. This work is the first simulation of solvate ionic liquids at electrified interfaces. This section will explore the effect of electrode model on the behaviour of these ionic liquids at the electrode. Chapter 4 uses a fixed charge electrode, whereas Chapter 5 uses one with a fixed potential. The section concludes that regardless of electrode model, the idealised portrait of a solvate ionic liquid - one where the liquid behaves exactly as an aprotic ionic liquid - is not applicable. In Chapter 4's exploration of fixed charged electrodes, the formation of 2 glyme to lithium complexes contradicts the idealised portrait of the liquid. A different change is observed in Chapter 5's exploration of fixed potential electrodes, with both lithium glyme and lithium anion clusters forming at the interface. The key difference between the two studies is that lithium does not coordinate to the electrode in the fixed charge simulations, while in the fixed potential case it does. At the end of Chapter 5 the results are compared against experimental data, with the efficacy of the two models discussed. The aim of both studies is to look at the nanostructure of ionic liquids, when the symmetry between co-ion and cation repulsion - and related effects - is broken by the presence of a non ionic constituent in the liquid.

abstract: The absorption spectra of metal-centered phthalocyanines (MPc's) have been investigated since the early 1960's. With improved experimental techniques to characterize this class of molecules the band assignments have advanced. The characterization remains difficult with historic disagreements. A new push for characterization came with a wave of interest in using these molecules for absorption/donor molecules in organic photovoltaics. The use of zinc phthalocyanine (ZnPc) became of particular interest, in addition to novel research being done for azaporphyrin analogs of ZnPc. A theoretical approach is taken to research the excited states of these molecules using time-dependent density functional theory (TDDFT). Most theoretical results for the first excited state in ZnPc are in only limited agreement with experiment (errors near 0.1 eV or higher). This research investigates ZnPc and 10 additional porphyrin analogs. Excited-state properties are predicted for 8 of these molecules using ab initio computational methods and symmetry breaking for accurate time- dependent self-consistent optimization. Franck-Condon analysis is used to predict the Q-band absorption spectra for all 8 of these molecules. This is the first time that Franck-Condon analysis has been reported in absolute units for any of these molecules. The first excited-state energy for ZnPc is found to be the closest to experiment thus far using a range-separated meta-GGA hybrid functional. The theoretical results are used to find a trend in the novel design of new porphyrin analog molecules. / Dissertation/Thesis / Doctoral Dissertation Materials Science and Engineering 2014