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RELIABLE PREDICTIONS OF THE PROPERTIES OF ACTINIDE COMPLEXES by VIRGIL ... PDF

242 Pages·2013·4.95 MB·English
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RELIABLE PREDICTIONS OF THE PROPERTIES OF ACTINIDE COMPLEXES by VIRGIL EDWARD JACKSON DAVID A. DIXON, COMMITTEE CHAIR SHANE C. STREET GREGORY SZULCZEWSKI LOWELL D. KISPERT TONYA M. KLEIN A DISSERTATION Submitted in partial fulfillment of the requirements for the degree of Doctor of Philosophy in the Department of Chemistry in the Graduate School of The University of Alabama TUSCALOOSA, ALABAMA 2013 Copyright Virgil Edward Jackson 2013 ALL RIGHTS RESERVED ABSTRACT A study of reactions of laser-ablated thorium atoms and O using matrix 2 isolation infrared spectroscopy has been conducted using electronic structure calculations to interpret the infrared spectra of three new thorium oxide species, ThO -, Th O , and Th O obtained in argon and neon matrixes. 2 2 2 2 4 The potential energy surface for the reaction of matrix isolated ThO with CH to give the 4 CH Th(O)H intermediate has been calculated at the CCSD(T) level, it reveals that the 3 CH Th(O)H molecule possesses a pyramidal structure with a closed shell singlet ground state. 3 Formation of the CH Th-(O)H molecule from the reaction of ThO and methane has an energy 3 barrier of 30 kcal/mol, which is consistent with the appearance of the 1CH Th(O)H absorptions 3 under broad band mercury arc UV irradiation. The 3Th + 1CH OH asymptote is predicted to be 3 119 kcal/mol above the reactant asymptote, 1ThO + CH ,utilizing the spin orbit correction to the 4 3Th atom which is in excellent agreement with the value of 118.7 ± 3.8 kcal/mol. The first reliable predictions of the frequencies of the isolated uranyl ion have been made to develop new techniques to determine how this important form of uranium is being complexed in the environment. A comprehensive computational study of UO 2+ complexed with the 2 phosphate anions H PO -, HPO 2-, and PO 3- and water ligands has been performed at the density 2 4 4 4 functional theory (DFT) and correlated molecular orbital theory levels in the gas phase and in aqueous solution. This study was done to aid the effort in developing solutions to the in situ remediation challenge posed by the nuclear waste stored in the tanks at the Hanford and ii Savannah River nuclear weapons production sites. This information can be used to provide a better understanding of the speciation of such species and to better our understanding of mobility issues of tank waste as well as stability concerns for waste matrices. iii DEDICATION To my mom, Virginia Jackson, and my dad, Edward Jackson, for their love and support; without which my success would not have been possible. iv LIST OF ABBREVIATIONS AND SYMBOLS ADE Adiabatic electron affinity ADF Amsterdam Density Functional software aug-cc-pVnZ Augmented, correlation consistent, polarized valence n zeta basis sets, where n = double (D), triple (T) or quadruple (Q) ANO-L Large atomic natural orbital basis sets ANO-S Small atomic natural orbital basis sets aug-cc-pVnZ-PP aug-cc-pVnZ basis sets with pseudopotentials for heavy atoms aug-cc-pwCVnZ Augmented, correlation consistent, polarized weighted core valence n (D, T, Q or 5) zeta basis sets aug-cc-pwCVTZ-PP aug-cc-pwCVTZ basis set with pseudopotentials for heavy atoms AVDZ E(n) = E + A exp[−(n − 1)] + B exp[−(n − 1)2] CBS n = 2 (aug-cc-pVDZ-PP) AVTZ E(n) = E + A exp[−(n − 1)] + B exp[−(n − 1)2] CBS n = 3 (aug-cc-pVDZ-PP) AVQZ E(n) = E + A exp[−(n − 1)] + B exp[−(n − 1)2] CBS n = 4 (aug-cc-pVDZ-PP) awCVTZ aug-cc-pwCVTZ basis sets B3LYP Becke 93 (exchange), Lee-Yang-Parr (correlation) DFT functional BLYP Becke 88 (exchange), Lee-Yang-Parr (correlation) DFT functional BDE Bond dissociation energy BP86 Becke 88 (exchange), Perdew 86 (correlation) DFT functional v CAS Complete active space CASPT2 Complete active space second-order perturbation theory CBS Complete basis set CCSD(T) Coupled cluster singles, doubles, and disconnected triples CCSD Coupled cluster singles, doubles COSMO Conductor-like screening model CI Configuration interaction CISD Configuration interaction singles and doubles CV Core valence DFT Density functional theory DHF Dirac–Hartree–Fock DZVP DFT optimized double zeta valence basis set with polarization functions (except H) DZVP2 DFT optimized double zeta valence basis set with polarization functions ΣD (ΣD ) Total atomization energy 0 0,0K G3MP2 Gaussian 3 theory calculation using 2nd order Møller Plesset perturbation theory (MP2) ΔE Complete basis set energy change CBS ΔE Core valence energy change CV ΔE Pseudopotential error correction energy exchange: ΔE = ΔE PP,corr PP,corr awCVTZ- - (ΔE + ΔE ). DK awCVTZ-PP SR ΔE Scalar relativistic energy change: ΔE = ΔE + ΔE = ΔE Rel Rel SR PP,corr awCVTZ- - ΔE DK awCVTZ-PP ΔE Spin orbit energy change SO ΔE Scalar relativistic correction calculated as the MVD expectation values SR vi ΔE Zero point energy change ZPE ΔE /ΔE BDE at 0 K/298 K 0K 298K ECP Effective core potential EA Electron affinity FA Fluoride affinity FCF Franck-Condon factors (FT-ICR-MS) Fourier transform ioncyclotron resonance mass spectrometry FTIR Fourier transform infrared spectroscopy FWAM Full widths at half maximum ΔG Aqueous deprotonation Gibbs free energy (solution free energy) aq ΔG Gas phase free energy gas ΔΔG Aqueous solvation free energy solv ΔG Gas phase Gibbs acidity 298K GIAO Gauge independent atomic orbital approximation ΔH Gas phase enthalpy acidity 298K HA Hydride affinity HF Hartee-Fock ΔH Heat of formation at 0K f,0K ΔH Heat of formation at 298K f,298K ΔH Reaction enthalpy change rxn I Intensities IR Infrared spectrscopy K Kelvin vii MO Molecular orbital MP2 2nd order Møller Plesset perturbation theory MVD Mass-velocity and Darwin operators NIST-JANAF National Institute of Standards and Technology - Joint Army-Navy-Air Force NMR Nuclear magnetic resonance PA Proton affinity PBE Perdew-Burke-Ernzerhof (exchange), Perdew-Burke-Ernzerhof (correlation) DFT functional PES Potential energy surface pK Negative logarithm of the acid dissociation constant a PP Pseudopetential PW91 Perdew-Wang 91 (exchange), Perdew-Wang 91 (correlation) DFT functional R Restricted method for the starting Hartree–Fock wavefunction R Gas constant ROHF Open-shell HF R/UCCSD(T) Open-shell CCSD(T) SCF Self consistent field SCRF Self consistent reaction field SO Spin orbit SP Square pyramidal SR Scalar relativistic T Temperature viii TAE Total atomization energy TZ2P Triple zeta basis set with 2 polarization functions UV Ultraviolet VTZP Valence high triple zeta basis set with polarized function ZORA Zeroth order regular approximation to the Dirac equation ZPE Zero point energy > Greater than < Less than = Equal to Å Angstrom ° Degrees ± Plus or minus ix

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To my mom, Virginia Jackson, and my dad, Edward Jackson, for their love and support; without . Shane C. Streets, Prof Gregory J. Szculczewski, Prof Lowell D. Kispert and Prof Tonya M. Klein for their supportive contributions.
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