The growth of Pb film on Si(111) is an unusual metal-semiconductor system. For a certain temperature range, Pb films have been found to grow in steep-edge and flat-top islands with uniform height on Si(111). This specific film morphology has been correlated to Quantum Size Effect (QSE) that the object size or film thickness affects the electronic structure of the films and results in certain thicknesses more stable than others. The X-ray diffraction technique has the advantages of long penetration length and high statistics, therefore it has been used to investigate the influence of QSE on the growth of Pb on the Si(111) 7x7 surface. It is demonstrated that the structure of Pb islands and the associated wetting layer are consistent with effects of quantum confinement. Specular reflectivity of 3 monolayer (ML) Pb films grown on the substrate at 227K has conclusively shown that the Pb islands do not reside on top of a Pb wetting layer, but directly on top of the Si substrate. The nucleating Pb nanocrystals transform the highly disordered Pb wetting layer beneath the islands into well-ordered fcc Pb. The surface then consists of fcc Pb islands directly on top of the Si surface with the disordered wetting layer between the islands. Moreover, it is found that QSE leads to novel behavior for the coarsening evolution of the Pb islands. The diffuse X-ray scattering experiments have been carried out as functions of temperature, deposition rate and coverage. A structural evolution of Pb islands was observed after deposition at very low coverages (0.2 -- 1.0 ML above the wetting layer coverage). Contrary to the classical scaling theory of nucleation and Ostwald ripening, a much lower island density is achieved with coarsening after deposition at high rather than low flux rates. The time constants of coarsening are found to be orders of magnitudes shorter than what is expected from the Gibbs-Thompson analysis. The rapid evaporation of unstable 3-layer islands shown in complementary STM suggests the role of QSE in the more efficient decay mechanism operating at low temperatures. These results have important applications for the controlled growth of nanostructures.

In the work presented in this dissertation, extensive molecular dynamics (MD) simulations have been performed to investigate various physical problems related to the solid-liquid transitions over a wide range of supercooling and superheating temperatures in model Lennard-Jones systems. The major focus of this work is to investigate the thermodynamics, kinetics, and underlying mechanisms of these problems. There are five topics in this work: (1) The classical nucleation theory (CNT) was tested for both liquid supercooling and solid superheating via different solid-liquid coexistence models. It is found that the CNT is valid for liquid supercooling but invalid for solid superheating. The arising elastic energy plays a significant role in affecting the liquid nucleation in a superheated solid. A new nucleation theory was proposed for describing the internal liquid nucleation of solid superheating. (2) Based on CNT, a new and accurate method was developed for calculating the crystal-melt interfacial free energy and its anisotropy. Our result is very close to Turnbulls experimental results. (3) The face, temperature, and size dependences of the crystallization rate were investigated in this work. The results show that the crystallization rate decreases substantially with the increasing system size. Different from the conventional models, a new model is developed to describe these dependences. (4) Melting from internal nanovoids was investigated in this work. It is found that the mechanism of void melting is quite different from bulk melting and nanoparticle melting. There are four different stages and three local melting temperatures in void melting. The mechanism of the complex melting sequence is systematically explained. (5) The homogenous melting at the upper limit of superheating was investigated in this work. For the first time, the ring diffusion is found to take place in superheated crystals and causes the spontaneous melting. The prevailing instability theories are unsuitable to describe this type of melting. The mechanism of the diffusion-loop mediated melting is carefully discussed in this work.

No description available.

<p>Theoretical studies based on first-principles theory are presented for a number of different magnetic systems. The first part of the thesis concerns spin dynamics and the second part concerns properties of magnetic multilayers. The theoretical treatment is based on electronic structure calculations performed by means of density functional theory.</p><p>A method is developed for simulating atomistic spin dynamics at finite temperatures, which is based on solving the equations of motion for the atomic spins by means of Langevin dynamics. The method relies on a mapping of the interatomic exchange interactions from density functional theory to a Heisenberg Hamiltonian. Simulations are performed for various magnetic systems and processes beyond the reach of conventional micromagnetism. As an example, magnetization dynamics in the limit of large magnetic and anisotropy fields is explored. Moreover, the method is applied to studying the dynamics of systems with complex atomic order such as the diluted magnetic semiconductor MnGaAs and the spin glass alloy CuMn. The method is also applied to a Fe thin film and a Fe/Cr/Fe trilayer system, where the limits of ultrafast switching are explored. Current induced magnetization dynamics is investigated by calculating the current induced spin-transfer torque by means of density functional theory combined with the relaxation time approximation and semi-classical Boltzmann theory. The current induced torque is calculated for the helical spin-density waves in Er and fcc Fe, where the current is found to promote a rigid rotation of the magnetic order.</p><p>Properties of magnetic multilayers composed of magnetic and nonmagnetic layers are investigated by means of the Korringa-Kohn-Rostocker interface Green's function method. Multilayer properties such as magnetic moments, interlayer exchange coupling and ordering temperatures are calculated and compared with experiments, with focus on understanding the influence of interface quality. Moreover, the influence on the interlayer exchange coupling of alloying the nonmagnetic spacer layers with small amounts of a magnetic impurity is investigated.</p>

Theoretical studies based on first-principles theory are presented for a number of different magnetic systems. The first part of the thesis concerns spin dynamics and the second part concerns properties of magnetic multilayers. The theoretical treatment is based on electronic structure calculations performed by means of density functional theory. A method is developed for simulating atomistic spin dynamics at finite temperatures, which is based on solving the equations of motion for the atomic spins by means of Langevin dynamics. The method relies on a mapping of the interatomic exchange interactions from density functional theory to a Heisenberg Hamiltonian. Simulations are performed for various magnetic systems and processes beyond the reach of conventional micromagnetism. As an example, magnetization dynamics in the limit of large magnetic and anisotropy fields is explored. Moreover, the method is applied to studying the dynamics of systems with complex atomic order such as the diluted magnetic semiconductor MnGaAs and the spin glass alloy CuMn. The method is also applied to a Fe thin film and a Fe/Cr/Fe trilayer system, where the limits of ultrafast switching are explored. Current induced magnetization dynamics is investigated by calculating the current induced spin-transfer torque by means of density functional theory combined with the relaxation time approximation and semi-classical Boltzmann theory. The current induced torque is calculated for the helical spin-density waves in Er and fcc Fe, where the current is found to promote a rigid rotation of the magnetic order. Properties of magnetic multilayers composed of magnetic and nonmagnetic layers are investigated by means of the Korringa-Kohn-Rostocker interface Green's function method. Multilayer properties such as magnetic moments, interlayer exchange coupling and ordering temperatures are calculated and compared with experiments, with focus on understanding the influence of interface quality. Moreover, the influence on the interlayer exchange coupling of alloying the nonmagnetic spacer layers with small amounts of a magnetic impurity is investigated.

Afin de développer de nouvelles applications aux couches minces d’oxydes fonctionnels, il est nécessaire de comprendre les corrélations entre leurs modes de croissance, leur microstructure, leur structure à l’interface avec le substrat, et leurs contraintes et propriétés physiques. Pour cela, une étude par spectroscopie infrarouge et THz des systèmes modèles films/substrats a été exécutée, et confrontée à des calculs théoriques, en particulier sur des couches épitaxiales de SrTiO3/Si(001), VO2/Gd2O3/Si(111) et des couches d’alumine sur alliage d’aluminium. Les caractéristiques vibrationnelles des couches minces sont ici étudiées dans l’infrarouge moyen et lointain sur la ligne AILES du Synchrotron SOLEIL, et simulées à l’aide de la Théorie de la Fonctionnelle de la Densité (DFT), permettant ainsi la première détermination de la structure cristalline de ces couches. Ainsi, une comparaison entre la structure bidimensionnelle et tridimensionnelle des matériaux est effectuée. L’effet des contraintes dans les couches est évalué grâce aux variations des énergies de vibration par rapport au matériau massif. L’influence des conditions expérimentales de l’épitaxie dans la structure locale interatomique de couches minces de SrTiO3/Si(001) est évaluée. D’autre part, la nature de l’interface STO-Si peut être caractérisée par les modes de vibration du réseau cristallin. Enfin, la transition métal-isolant (MIT) des couches minces de VO2 sur des substrats de Gd2O3/Si(111) est étudié par spectroscopie IR ; les variations de propriétés optiques et diélectriques pendant la transition, ainsi que les changements d’intensité des modes de vibration, indiquent que la transition est entraînée par une corrélation électronique et une basse température. La phase monoclinique M1 de VO2 est un isolant de Mott. Ce résultat peut aider à un meilleur contrôle des MIT de couches minces de VO2 pour de futures applications. / In order to understand the relations between growth, microstructure, interface structure, strain, and physical properties in functional oxide thin films for further applications, a study of infrared and THz spectroscopy combined with theoretical calculation has been performed on the films/substrates model systems, in particular epitaxial SrTiO3/Si(001), VO2/Gd2O3/Si(111) films and alumina/alloy films. The vibrational characteristics of the crystal structure of films have been investigated in the mid and far infrared ranges on the AILES beamline at Synchrotron SOLEIL. This experimental vibrational study has been combined with Density Functional Theory (DFT) simulation to allow for the first measure of the crystalline structure of these thin films. The 2-dimensional lattice modification compared with the bulk materials has been discussed. The strain effect in the films can be evaluated on the phonon shifts compared with the crystal spectrum. The influences of epitaxial conditions on the local interatomic structure of SrTiO3/Si(001) thin films have been estimated. The nature of STO-Si interface can be characterized by the phonon modes. The metal–insulator transition (MIT) of VO2 thin films on Gd2O3/Si(111) substrate have been studied by IR spectroscopy. The variations of optical and dielectric properties during the MIT, as well as the phonon intensities, indicate that the MIT is driven by electron correlation and the low temperature M1 monoclinic phase of VO2 is a Mott insulator. This result may help to better understand and control the MITs of VO2 thin films in the device applications.

This work investigates the growth dynamic of the reactive molecular beam epitaxy of Fe3O4 films, and its impact on the cation distribution as well as on the magnetic and structural properties at the surface and the interfaces. In order to study the structure and composition of Fe3O4 films during growth, time-resolved high-energy x-ray diffraction (tr-HEXRD) and time-resolved hard x-ray photoelectron spectroscopy (tr-HAXPES) measurements are used to monitor the deposition process of Fe3O4 ultrathin films on SrTiO3(001), MgO(001) and NiO/MgO(001). For Fe3O4\SrTiO3(001) is found that the film first grows in a disordered island structure, between thicknesses of 1.5nm to 3nm in FeO islands and finally in the inverse spinel structure of Fe3O4, displaying (111) nanofacets on the surface. The films on MgO(001) and NiO/MgO(001) show a similar result, with the exception that the films are not disordered in the early growth stage, but form islands which immediately exhibit a crystalline FeO phase up to a thickness of 1nm. After that, the films grown in the inverse spinel structure on both MgO(001) and NiO/MgO(001). Additionally, the tr-HAXPES measurements of Fe3O4/SrTiO3(001) demonstrate that the FeO phase is only stable during the deposition process, but turns into a Fe3O4 phase when the deposition is interrupted. This suggests that this FeO layer is a strictly dynamic property of the growth process, and might not be retained in the as-grown films. In order to characterize the as-grown films, a technique is introduced to extract the cation depth distribution of Fe3O4 films from magnetooptical depth profiles obtained by fitting x-ray resonant magnetic reflectivity (XRMR) curves. To this end, x-ray absorption (XAS) and x-ray magnetic circular dichroism (XMCD) spectra are recorded as well as XRMR curves to obtain magnetooptical depth profiles. To attribute these magnetooptical depth profiles to the depth distribution of the cations, multiplet calculations are fitted to the XMCD data. From these calculations, the cation contributions at the three resonant energies of the XMCD spectrum can be evaluated. Recording XRMR curves at those energies allows to resolve the magnetooptical depth profiles of the three iron cation species in Fe3O4. This technique is used to resolve the cation stoichiometry at the surface of Fe3O4/MgO(001) films and at the interfaces of Fe3O4/MgO(001) and Fe3O4/NiO. The first unit cell of the Fe3O4(001) surface shows an excess of Fe3+ cations, likely related to a subsurface cation-vacancy reconstruction of the Fe3O4(001) surface, but the magnetic order of the different cation species appears to be not disturbed in this reconstructed layer. Beyond this layer, the magnetic order of all three iron cation species in Fe3O4/MgO(001) is stable for the entire film with no interlayer or magnetic dead layer at the interface. For Fe3O4/NiO films, we unexpectedly observe a magnetooptical absorption at the Ni L3 edge in the NiO film corresponding to a ferromagnetic order throughout the entire NiO film, which is antiferromagnetic in the bulk. Additionally, the magnetooptical profiles indicate a single intermixed layer containing both Fe2+ and Ni2+ cations.