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First--principles electronic structure calculations have been performed to help identify and direct the synthesis of new superhard compounds. An improved figure of merit for hardness is identified and used to show that carbon nitrides are not likely to be harder than diamond. / Ph. D.

Feldspar minerals are framework aluminosilicates that comprise approximately 60 percent of the Earth's crust. The elastic and thermodynamic properties of this important mineral group are needed for the interpretation of seismic wave velocities, for understanding cation partioning patterns and for the determination of phase boundaries and reactions involving feldspars in the Earth's crust. Until recently, no systematic approach has been applied to describe the structural behavior of feldspars as a function of pressure, temperature and composition. In this thesis, high-pressure and high-temperature X-ray diffraction data were collected for feldspars over a range of compositions which has led to the development a structural model that allows one to predict the structural evolution of feldspars at depth in the Earth's crust. Specifically, the equations of state have been determined for two plagioclase feldspars (An20 and An78) with different states of Al/Si ordering using single-crystal X-ray diffraction. This study has shown that the introduction of Al,Si disorder into plagioclase structures at constant composition softens the structure by 4(1)% for An0, 2.5(9)% for An20 and is essentially zero for An78 compositions. The effect of pressure on the structure of an ordered An20 was also determined up to 9.15 GPa using single-crystal X-ray diffraction and it was found that the dominant compression mechanism involves tilting of the AlO4 and SiO4 tetrahedra. Similarly, high-temperature single-crystal X-ray diffraction data collected from an ordered An26 plagioclase and powder X-ray diffraction collected on a suite of Na-rich plagioclases that were refined using the Rietveld method indicate that the major structural response to increased temperature involves tilting of the tetrahedra. Building on ideas originally proposed by Dr. Helen Megaw, the changes in the conformation of the tetrahedral framework of feldspars can be described in terms of four distinct tilt systems of rigid tetrahedra. This model demonstrates that the fundamental reason for the observed anisotropy and volume change of feldspars lies in the topology of the tetrahedral framework with the greatest contribution attributed to tilt systems 2 and 3. / Ph. D.

A comprehensive study on the effect of composition on the structural and elastic properties of MPO4 (M = Ce3+, Gd3+, Tb3+, Y3+, Sc3+) compounds has been completed. CePO4 and GdPO4 are isostructural with monazite (P21/n), and TbPO4, YPO4, and ScPO4, are isostructural with xenotime (I41/amd). Raman spectra are consistent with previous studies and high-pressure spectra showed no phase transitions up to 10 GPa under hydrostatic conditions. The spectra were used to develop Kieffer-type lattice vibrational models to calculate heat capacities of CePO4 and YPO4 and the results lie within 1-3% of experimental values. Equations of state were calculated from high-pressure single-crystal X-ray diffraction data. Bulk moduli (K0) determined from a 3rd-order Birch-Murnaghan equation of state are: 109(3) GPa for CePO4, 128.1(8) GPa for GdPO4, 141(1) GPa for TbPO4 and 166(1) GPa for ScPO4. The inverse relationship observed between K0 and the ionic radius of the RE3+ is shown to be linear. This equation can be used to predict K0 for other rare-earth phosphates. Comparison of these studies, performed under hydrostatic conditions, with previous studies show that MPO4 structures are sensitive to shear stresses created from non-hydrostatic environments. The first structural study of a monazite, GdPO4, is also reported. Compression mechanisms are comprised of "squishing" the GdO9 polyhedra and inter-polyhedral movement. This study and the axial compressibility data for Ce-, Tb-, Gd- and ScPO4 suggest that the compression mechanisms favored by MPO4 compounds are those which remain rigid parallel to polyhedral chains. / Master of Science

The objective of this work was to determine the effect of high pressure processing (HPP) on fresh tomato-associated outbreak isolates of Salmonella enterica in broth and on green mature tomato fruits. Nalidixic acid resistant (to 50 ppm) cultures of Salmonella enterica ser. Newport and Salmonella enterica ser. Braenderup were suspended in tryptic soy broth to a concentration of approximately 8 log CFU/ml and subjected to 350, 450, and 550 MPa for 120 s. Samples were serially diluted in peptone water, and surface plated onto tryptic soy agar supplemented with nalidixic acid (50 ppm; TSAN) and incubated at 35°C for 48 h. Reductions of 5.64, 6.30, and 6.61 log CFU/ml in S. Newport, and reductions of 4.10, 5.22, and 6.35 log CFU/ml in S. Braenderup at 350, 450, and 550 MPa, respectively, were observed. Green tomato fruits inoculated with S. Newport or S. Braenderup to an initial concentration of approximately 6 log CFU/g were sealed in a bag containing 350 ml of 1% CaCl2 and subjected to the same pressure treatments described above. The whole tomato fruits were pummeled in a stomacher and samples were surface plated onto TSAN supplemented with 1% pyruvic acid. Reductions of 1.55, 2.89, and 4.26 log CFU/g for S. Newport and 1.22, 2.26, and 3.77 log CFU/g for S. Braenderup at 350, 450, and 550 MPa, respectively, were observed. Bagged (350 ml 1% CaCl₂) samples of non-inoculated green tomato fruits were subjected to the same conditions described above. HPP treated tomatoes were then subjected to an ethylene gas (125 ppm; 0.7 cc/min) for 5 to 6 days. Pressured tomato fruits did not ripen. Even though HPP effectively reduced populations of S. enterica, it adversely affects the ripening characteristics of green mature tomato fruits. / Master of Science in Life Sciences

Moderne Hochdruckforschung entwickelt sich rasant zu einer der vielfältigstens und überraschensten Disziplinen der Festkörperphysik. Unter Benutzung von Diamantstempelzellen können Drücke erreicht werden, die den Bedingungen im Inneren unserer Erde ähneln. Eine Anwendung von Kernmagnetischen Resonanzexperimenten (NMR) in Diamantstempelzellen galt jedoch fur lange Zeit als unmöglich. In der vorliegenden Arbeit wird ein neuartiger Ansatz weiterentwickelt, der Radiofrequenz-(RF)-Mikrospulen benutzt, die direkt zwischen den Diamantstempeln platziert werden, und somit zu einer signififikanten Sensitivitatssteigerung führen. Es ist gelungen, Hochdruckzellen zu entwickeln, die fur die speziellen Anforderungen der NMR zugeschnitten sind. Des Weiteren konnte eine nicht metallische, nicht magnetische Dichtung entwickelt werden, die zudem zu einer signififikanten Stabilisierung des Probenvolumens führt. Eine breit angelegte Analyse der Leistungsfähigkeit dieser neuartigen NMR-Hochdruckprobenköpfe zeigt deren Leistungsfähigkeit mit sehr hohen Empfifindlichkeiten sowie einer exzellenten RF Anregung und Zeitauflösung. Drei Anwendungsbeispiele, die das Potenzial dieses Ansatzes in dieser Arbeit unterstreichen, werden vorgestellt. Bei Drücken von bis zu 4 GPa werden die elektronischen und dynamischen Eigenschaften von elementarem Gallium untersucht. Unter höheren Drücken ist es gelungen, einen druckinduzierten Isolator-Metall-Übergang in dem ternaren Chalkogenid AgInTe2 zu beobachten. Schlussendlich ist es gelungen, die strukturellen und elektronischen Eigenschaften von Rubin bei Drücken von bis zu 30.5 GPa zu untersuchen, was einer Verdreifachung des bisher zugänglichen experimentellen Druckbereiches entspricht und die NMR fur moderne Hochdruckanwendungen möglich macht.

A Walker-type multianvil high-pressure facility is capable of high-pressure syntheses and measurements beyond 10 GPa and has been utilized in my research to synthesize the 4d Ruthenium and Rhodium and the 5d Iridium oxides with the perovskite-related structures. Under high-pressure and high-temperature conditions, these families of oxides can be enlarged to a great extent so that enables us not only to address the long-standing problem about ferromagnetism in the perovskite ruthenates but also explore new phenomena associated with the structural and electronic properties in the iridates and rhodates. In the perovskite ruthenates ARuO₃ (A= Ca, Sr, and Ba), a systematic study of the variations of the ferromagnetic transition temperature T[subscript c] and the critical isothermal magnetization as a function of the average A-site cation size and the size variance as well as external high pressures reveals explicitly the crucial role of the local lattice strain and disorder on T[subscript c] and the nature of the localized-electron ferromagnetism. However, such a steric effect is dominated by the electronic effect in another perovskite ruthenate PbRuO₃, which is a paramagnetic metal down to 1.8 K and undergoes a first-order structural transition to a low-temperature Imma phase at Tt [almost equal to] 90 K. Bandwidth broadening due to orbital hybridization between Pb-6s and Ru-4d plays an important role in suppressing the ferromagnetism in the Sr1-zPbzRuO₃ system. The high-pressure sequence of the 9R-BaIrO₃ was explored and three more polytypes, i.e. 5H, 6H and 3C, were identified under 10 GPa. With increasing fraction of the corner- to face-sharing IrO₆/₂ octahedra, the ground states of BaIrO₃ evolve from a ferromagnetic insulator with T[subscript c] [almost equal to] 180 K in the 9R phase to a ferromagnetic metal with T[subscript c] [almost equal to] 50 K in the 5H phase, and finally to an exchange-enhanced paramagnetic metal near a quantum critical point in the 6H phase. In addition to the perovskite SrRhO₃, a new 6H polytype was synthesized for the first time under high pressure and a pressure-temperature phase diagram was given for the 6H-perovskite transformation. Restoration of the Curie-Weiss behavior in the high-temperature magnetic susceptibility [chi](T) of the perovskite SrRhO₃ resolves the puzzle about unusual dependence of [chi]⁻¹ [symbol] T² reported earlier and highlights the importance of spin-orbit coupling in the 4d and 5d transition-metal oxides. / text

Transition metal oxides have been extensively studied during past decades. The purpose of this research was to synthesize new or little characterised transition metal oxides using high-pressure/high-temperature (HPHT) techniques. Various ternary vanadium oxides have been synthesised at ambient and high pressure conditions. All compounds have been studied by neutron and laboratory X-ray powder diffraction and magnetisation measurements. In some cases resistivity and synchrotron X-ray powder diffraction measurements were also carried out. The MnVO3 perovskite containing localized 3d5 Mn2+ and itinerant 3d1 V4+ states has been synthesised at 8 GPa and 1100°C. MnVO3 crystallises in Pnma space group (a = 5.2741(6) Å, b = 7.4100(11) Å, and c = 5.1184(8) Å at 300 K) and is metallic at temperatures of 2 – 300 K and at pressures of up to 67 kbar. Synchrotron X-ray powder diffraction study on the combined sample of several high pressure products showed slight variation in the stoichiometry of MnVO3. Incommensurate Mn spin order was discovered in the neutron powder diffraction measurements, which reveal a (0.29 0 0) magnetic vector below the 46 K spin ordering transition, and both helical and spin density wave orderings are consistent with the diffraction intensities. Electronic structure calculations show large exchange splittings of the Mn and V 3d bands, and (kx 0 0) crossings of the Fermi energy by spin up and down V 3d bands may give rise to Ruderman-Kittel-Kasuya-Yosida coupling of Mn moments, in addition to their superexchange interactions. The new compound CoVO4 has been discovered in a high pressure synthesis experiment. Magnetic susceptibility measurement, synchrotron X-ray and neutron powder diffraction studies were carried out. Refinements of the synchrotron X-ray and neutron data show CoVO4 to crystallise in space group Pbcn (a = 4.5012(2) Å, b = 5.5539(3) Å, and c = 4.8330(2) Å at 300 K (synchrotron X-ray data)). The magnetic susceptibility measurement reveals that Co3+ is most likely in a low spin state in CoVO4. Monoclinic brannerite type CoV2O6 was synthesised in ambient pressure. Neutron powder diffraction measurements were carried out and an antiferromagnetic order with an a x b x 2c supercell was observed below TN = 15 K. High spin Co2+ moments of magnitude 4.77(4) μB at 4 K lie in the ac plane and are ferromagnetically coupled within chains of edge-sharing CoO6 octahedra parallel to b axis. No structural transition is observed down to 4 K, but a magnetostriction accompanying antiferromagnetic order at TN = 15 K was discovered. A field-induced 1/3 magnetisation plateau and corresponding changes in the magnetic structure were studied by carrying out neutron powder diffraction measurements at 2 K in applied magnetic fields of 0, 2.5 and 5.0 T. Three collinear magnetic phases were observed as field increases; the above antiferromagnetic state with propagation vector (0 0 ½), a ferrimagnetic (¯⅓ 1 ⅓) phase, and a (0 0 0) ferromagnetic order. Co2+ moments of 4.4 - 5.0 μB have a large orbital component and are aligned close to the c-axis direction in all cases. Spin-lattice coupling leads to a magnetostriction and volume expansion as field increases. The ferrimagnetic phase accounts for the previously reported 1/3 magnetisation plateau, and demonstrates that monoclinic CoV2O6 behaves as an accidental triangular antiferromagnetic lattice in which further frustrated orders may be accessible. Orthorhombic columbite-type NiV2O6 and CoV2O6 compounds were synthesised at 6 GPa and 900°C. Metamagnetism and magnetic transitions were found in magnetic measurements. Powder neutron diffraction studies in zero and applied field were carried out. Both compounds were refined in space group Pbcn and the following lattice parameters were obtained at 300 K, CoV2O6: a = 13.4941(20) Å, b = 5.5736(9) Å, and c = 4.8082(8) Å and NiV2O6: a = 13.3725(17) Å, b = 5.5344(7) Å, and c = 4.8162(7) Å. Neutron powder diffraction studies in zero field did not reveal any magnetic peaks for either of the compounds but magnetic order emerges in applied fields between 1 and 4 T.