Submitted by Juliano Torteli De Godoi Zucato (jtgzucato@gmail.com) on 2018-08-15T17:17:02Z No. of bitstreams: 1 Dissertação Juliano Zucato.pdf: 6062254 bytes, checksum: c2ecd162aff92215ef89a486bafa836f (MD5) / Approved for entry into archive by Cristina Alexandra de Godoy null (cristina@adm.feis.unesp.br) on 2018-08-15T20:07:28Z (GMT) No. of bitstreams: 1 zucato_jtg_me_ilha.pdf: 6062254 bytes, checksum: c2ecd162aff92215ef89a486bafa836f (MD5) / Made available in DSpace on 2018-08-15T20:07:28Z (GMT). No. of bitstreams: 1 zucato_jtg_me_ilha.pdf: 6062254 bytes, checksum: c2ecd162aff92215ef89a486bafa836f (MD5) Previous issue date: 2018-07-03 / O trabalho consiste em um estudo da soldagem sobre uma placa da liga de titânio ASTM (Ti-6Al-4V) de espessura 1,44 mm, utilizando o processo de soldagem à laser Nd:YAG na condição autógena, realizando alterações de parâmetros no processo de soldagem afim de alterar o aporte térmico, encontrando propriedades características como a dureza, tensão de escoamento e microestrutura do material. Os ensaios realizados para a pesquisa foram: análise macrográfica, ensaio de tração, ensaio de microdureza e caracterização microestrutural. Para revelação dos detalhes no metal de solda, foi utilizado um ataque químico com o reagente Kroll. As medidas de geometria (largura e profundidade de penetração) dos cordões de solda, assim como a presença de descontinuidades, foram realizadas através de imagens obtidas pelo microscópio estéreo Zeiss Discovery.V8. O processamento e medição das imagens foi realizado através do software "AxioVision", um software associado ao microscópio utilizado. A análise da microestrutura foi realizada através do Microscópio Óptico Neophot 21, já o ensaio de tração foi realizado através de uma Máquina Universal de Ensaios, além do ensaio de microdureza, que foi realizado na escala Vickers. As análises das propriedades mecânicas foram confrontadas com a microestrutura obtida de acordo com a variação do aporte térmico. Como resultados, foram encontradas várias características essenciais para uma boa soldagem da liga, pois a cada incremento de aporte térmico, o cordão de solda aumenta em largura, profundidade e dureza, porém isto tem vantagem até determinado valor, pois conforme há o aumento do aporte térmico, a soldagem se fragiliza, pelo fato de existir vaporização do material e inclusão de poros na zona fundida. / The work consists of a study of the welding on a plate of titanium alloy ASTM (Ti-6Al-4V) of thickness 1.44 mm, using the welding process Nd: YAG in the autogenous condition, making changes of parameters in the process of welding in order to change the thermal input, finding characteristic properties such as hardness, yield stress and microstructure of the material. The tests carried out for the research were: macrographic analysis, tensile test, microhardness test and microstructural characterization. To reveal the details in the weld metal, a chemical attack was used with the Kroll reagent. The measurements of the geometry (width and depth of penetration) of the weld beads, as well as the presence of discontinuities, were made through images obtained by the stereo microscope Zeiss Discovery.V8. The images were processed and measured using the "AxioVision" software, a software associated with the microscope used. The analysis of the microstructure was performed through the Optical Microscope Neophot 21, and the tensile test was performed through a Universal Testing Machine, in addition to the microhardness test, which was performed on the Vickers scale. The analysis of the mechanical properties were compared with the microstructure obtained according to the variation of the thermal input. As a result, several essential characteristics have been found for a good welding of the alloy, because with each increment of thermal input, the weld bead increases in width, depth and hardness, however this has advantage until a certain value, since as there is increase of the contribution thermal, welding becomes fragile, due to the fact that there is vaporization of the material and inclusion of pores in the molten zone.

Les films minces luminescents dopés terres rares offrent des propriétés intéressantes pour la conversion spectrale UV-bleu, en particulier pour une meilleure adaptation du spectre solaire aux cellules solaires en silicium. Deux matériaux luminophores ont été étudiés dans cette thèse : Y2O3 dope Eu3+ et CaYAlO4 codopé Ce3+, Pr3+. L'utilisation de ces luminophores pour les applications sous forme de films minces est limitée car ils possèdent un faible coefficient d'absorption. Deux pistes ont été examinées pendant cette thèse pour pallier ce problème : (i) l'effet plasmonique a été étudié en réalisant des films avec une architecture multicouche couplant les films luminophores et des nanostructures métalliques d'aluminium et d'argent qui possèdent une résonnance plasmon dans la gamme UV et bleu respectivement ; (ii) l'effet photonique a été évalué en réalisant une structuration du film luminophore via une croissance sur des membranes macro-poreuses. La méthode de synthèse choisie est le dépôt par ablation laser pulsé / Rare earth luminescent thin film offers attractive properties for down shifting application, particularly for a better adaptation of the solar spectrum to silicon solar cells. In this thesis, we studied two phosphor materials : Y2O3 doped Eu3+ and CaYAlO4 codoped Ce3+, Pr3+. One issue identified for the use of these phosphors as thin films is their low absorption coefficient. We examined two tracks during this thesis to meet these needs : (i) the plasmonic effect was studied by making films with a multilayer architecture coupling the phosphor films and aluminium or silver metallic nanostructures which have a plasmon resonance in the UV range and blue respectively ; (ii) the photonic effect was evaluated by structuring the phosphor layer by self-organization growth on macroporous membranes. We did the syntheses by pulsed laser deposition

Cette thèse présente l'élaboration et l'étude de nanofils ferromagnétiques de cobalt, nickel et d'alliages cobalt-nickel épitaxiés en matrice de titanate de strontium et de baryum. Les fils sont élaborés par auto-assemblage lors de dépôts séquentiels par ablation laser pulsé. Tout d'abord, les paramètres de croissance permettant de contrôler le diamètre des fils et leur densité sont mis en évidence en modélisant la croissance de l'hétéro-structure par simulations Monte-Carlo cinétique. Ensuite, on montre que les fils sont dilatés axialement et relaxés radialement. L'origine de l'état dilaté est expliquée en adaptant le modèle de Frenkel-Kontorova à notre situation et les inhomogénéités de déformation des nanofils sont décrites en analysant des cartographies de l'espace réciproque. La dilatation crée une anisotropie magnétique, par couplage magnéto-élastique, qui, dans le cas du nickel, peut compenser l'anisotropie de forme des fils. Enfin, pour des fils de Co0.4Ni0.6 de diamètre supérieur à quatre nanomètres, la température de blocage de l'assemblée de fils est supérieure à la température ambiante et la barrière d'énergie du renversement magnétique est de l'ordre d'un électronvolt, ce qui est intéressant pour d'éventuelles applications, par exemple en enregistrement de données. / In this PhD thesis, we study the growth and the properties of ferromagnetic nanowires made of cobalt, nickel and cobalt-nickel, embedded in a matrix made of of strontium and baryum titanate. The nanowires are grown taking advantage of self-assembly processes occurring during sequential pulsed laser deposition. First, we model the growth with a kinetic Monte-Carlo code to highlight the parameters that control the diameter and the density of the nanowires. Then, it is shown that the nanowires are strained along their axis, and relaxed perpendicular to it. The origin of the strained state is explained in the framework of the Frenkel-Kontorova model, and its inhomogeneities are described through analysis of mappings of the reciprocal space. Furthermore, it is shown that the strain is high enough to shift the magnetic easy axis of the nickel nanowires, through magneto-elastic coupling. Finally, for Co0.4Ni0.6 nanowires with a diameter greater than four nanometers, the blocking temperature of the assembly is above room temperature and the energy barrier for the magnetic reversal of the nanowires is of the order of one electronvolt. This is interesting for potential applications in data storage, for example.

Moderne Lasereinrichtungen stellen hochintensives Licht mit sehr kurzer zeitlicher Struktur zur Verfügung. Damit bringen diese Einrichtungen die Phänomene in die Laboratorien, welche normalerweise nur in der Nähe von stark strahlenden Sternen im Weltall zu finden sind. Bezüglich der Streuprozesse von Teilchen innerhalb dieser extremen Lichtquellen gibt es eine Vielzahl an theoretischen Untersuchungen. Vorwiegend geschehen diese unter der Verwendung der Starkfeld-Quantenelektrodynamik, einer Theorie zur quanten- theoretischen Beschreibung von elektromagnetischen Wechselwirkungen innerhalb eines kohärenten hochintensiven Feldes, welches als semi-klassisches Hintergrundfeld beschrieben wird. Zum Beispiel zeigte die theoretische Behandlung des Compton-Prozesses (die inelastis- che Elektron-Photon-Streuung) oder des Breit-Wheeler-Prozesses (der Paarproduktion in der Kollision von zwei Photonen) innerhalb der Starkfeld-Quantenelektrodynamik eine große Menge an neuen nicht-linearen Effekten und Phänomen, welche stellenweise in zukun- ftsweisenden Experimenten nachgewiesen werden konnten. Von großem Interesse und auch zentrales Untersuchungsobjekt der vorliegenden Arbeit ist ebenso der Trident-Prozess: ein Prozess zweiter Ordnung in der (Starkfeld-) Quan- tenelektrodynamik, bei dem ein Elektron-Positron-Paar innerhalb der Kollision eines Photonstrahls (z.B. erzeugt von einem Laser) und eines gegenläufigen Elektronenstrahls entsteht. Allerdings ist der Trident-Prozess im Zusammenhang mit hochintensiven Feldern nicht ausschließlich das Produkt seiner Teile, den erwähnten Compton- und Breit-Wheeler- Prozessen, vielmehr erzeugt das Vorhandensein des intermediären Photons durch seine virtuellen und reellen Beträge überaus komplizierte Strukturen. In den letzten Jahren gab es daher eine große Menge an theoretischen Beiträgen zur nicht-linearen Behandlung des Trident-Prozesses bezüglich eines weiten Bereichs an Eigenschaften der verwendeten Lichtquelle. Jedoch ist der nicht-lineare Trident-Prozess wegen seiner anspruchsvollen mathematischen Natur bisher nicht als völlig verstanden anzusehen. In der vorliegen- den Arbeit liegt der Fokus auf der Abhängigkeit des Trident-Prozesses von den kurzen zeitlichen Strukturen der verwendeten Lichtquellen bei hohen Energien. Grob gesprochen bedeutet dies, dass die kurz gepulsten Strukturen der modernen Lichtquellen zu breiten Spektren der Photonstrahlen führen, welche sich dann auch in den betrachteten Prozessen widerspiegeln. Demfolgend wird in der vorliegenden Arbeit eine neue Approximation an die Starkfeld-Quantenelektrodynamik erarbeitet, welche in der Lage ist, die spektralen Abhängigkeiten in den Prozessen zu beschreiben, die in Laser-Elektron-Kollisionen bei hohen Energien vorzufinden sind. Diese neue Approximation wird dann auf den Trident- Prozess angewendet und es werden die neuen Strukturen herausgearbeitet, welche durch das breite Spektrum der betrachteten Lichtquelle entstehen. Ferner werden bestehende oder geplante extreme Lichtquellen dahingehend untersucht, in welcher Weise diese, kombiniert mit einem passendem Elektronenstrahl, sensitiv für die vorgestellten spektralen Effekte im Trident-Prozess sind. Abschließend werden weitere mögliche Anwendungsbereiche der neuen Approximation diskutiert.:1 Introduction 1 2 Strong-field quantum electrodynamics 11 2.1 Description of the laser field 12 2.2 Background field approximation 18 2.3 Momentum space rules of strong-field QED 25 2.4 Ward identity and gauge invariance 34 2.5 Strong-field trident process 36 3 Pulsed-perturbative quantum electrodynamics 43 3.1 Approaches and approximations to strong-field QED 43 3.2 Momentum space rules in pulsed-perturbative QED 46 3.3 Spectrum of the background field 52 4 Pulsed-perturbative trident process 57 4.1 Matrixelement and cross section 57 4.2 Total cross section 72 4.3 Inclusive positron distributions 75 4.4 Exclusive electron distributions 81 4.5 Experimental capability 93 5 Summary and Outlook 97 Appendix 101 A Relativistic Kinematics 103 A.1 Preliminary remarks 103 A.2 Coordinate systems 104 A.3 Frames of reference 109 A.4 Kinematics of 2→3 processes 111 B Feynman rules of QED 121 C Perturbative trident pair production 125 C.1 Matrixelement and cross section 125 C.2 Numerical implementation and comparison to literature 129 C.3 Differential cross sections in transverse coordinates 132 C.4 Darkphotons 134 D Useful mathematical statements 139 Bibliography 153 / Modern laser facilities provide highly intense light with a very short temporal structure, which brings the phenomena originally found near the strong radiating stars in the universe into the laboratory. Accordingly, there are, among others, wide theoretical investigations w.r.t. scattering processes of particles impinging this extreme light sources. This has been done by applying the strong-field quantum electrodynamics, which is a theory of electromagnetic interactions within coherent highly intense light treated as a semi-classical background field. For instance, the treatment of the Compton process (inelastic electron- photon scattering) and the Breit-Wheeler process (pair production of a collision of two photons) with strong-field quantum electrodynamics revealed a vast amount of novel non-linear structures and phenomena, which were to some extent experimentally verified. Of particular interest and the central object of investigation within this thesis is also the trident process: a second order process in (strong-field) quantum electrodynamics producing an electron-positron pair within the collision of a photon beam (e.g. produced by a laser) with a counter-propagating electron. However, in the context of highly intense fields, the trident process is more than the product of its parts, the mentioned Compton and Breit-Wheeler process, since the intermediate photon yields both virtual and real contributions producing exceedingly complicated structures. Over the last years, there are several theoretical contributions to the non-linear treatment of the trident process w.r.t. a wide range of laser properties, but the trident process has not yet been fully understood due to its demanding mathematical nature. Within the present thesis, we focus on the dependence of the trident process to the short temporal structures of the involved light source at high energies. Loosely speaking, this means the short pulsed structure of modern light sources provide a wide energy spectrum of the respective photons, which is imprinted on the considered scattering processes. Accordingly, we elaborate a new approximation to strong-field quantum electrodynamics capable to describe the spectral dependence of processes within laser-electron collisions at high energies. Then we apply this new approximation to the trident process and reveal the novel structures generated by the spectrum of the light source. Therefore, we provide an analysis of the spectral impact to the trident process involving the total cross section as well as several inclusive and exclusive distributions of its final particles. Consequently, we examine in principle the experimental capabilities of present or planed extreme light sources by combining them with a suitable electron beam, whether they are sensitive to the encountered spectral effects of the trident process and discuss further applications of the newly introduced approximation.:1 Introduction 1 2 Strong-field quantum electrodynamics 11 2.1 Description of the laser field 12 2.2 Background field approximation 18 2.3 Momentum space rules of strong-field QED 25 2.4 Ward identity and gauge invariance 34 2.5 Strong-field trident process 36 3 Pulsed-perturbative quantum electrodynamics 43 3.1 Approaches and approximations to strong-field QED 43 3.2 Momentum space rules in pulsed-perturbative QED 46 3.3 Spectrum of the background field 52 4 Pulsed-perturbative trident process 57 4.1 Matrixelement and cross section 57 4.2 Total cross section 72 4.3 Inclusive positron distributions 75 4.4 Exclusive electron distributions 81 4.5 Experimental capability 93 5 Summary and Outlook 97 Appendix 101 A Relativistic Kinematics 103 A.1 Preliminary remarks 103 A.2 Coordinate systems 104 A.3 Frames of reference 109 A.4 Kinematics of 2→3 processes 111 B Feynman rules of QED 121 C Perturbative trident pair production 125 C.1 Matrixelement and cross section 125 C.2 Numerical implementation and comparison to literature 129 C.3 Differential cross sections in transverse coordinates 132 C.4 Darkphotons 134 D Useful mathematical statements 139 Bibliography 153

This thesis deals with the synthesis and characterization of Ge-Te-Sb (GST) thin films. The films were deposited using a Pulsed Laser Deposition (PLD) method and mainly characterized with XRD, SEM, AFM and TEM. For amorphous and polycrystalline films, un-etched Si(100) was used. The amorphous films showed a similar crystallization behavior as films deposited with sputtering and evaporation techniques. When depositing GST on un-etched Si(100) substrates at elevated substrate temperatures (130-240°C), polycrystalline but highly textured films were obtained. The preferred growth orientation was either GST(111) or GST(0001) depending on if the films were cubic or hexagonal. Epitaxial films were prepared on crystalline substrates. On KCl(100), a mixed growth of hexagonal GST(0001) and cubic GST(100) was observed. The hexagonal phase dominates at low temperatures whereas the cubic phase dominates at high temperatures. The cubic phase is accompanied with a presumed GST(221) orientation when the film thickness exceeds ~70 nm. Epitaxial films were obtained with deposition rates as high as 250 nm/min. On BaF2(111), only (0001) oriented epitaxial hexagonal GST films are found, independent of substrate temperature, frequency or deposition background pressure. At high substrate temperatures there is a loss of Ge and Te which shifts the crystalline phase from Ge2Sb2Te5 towards GeSb2Te4. GST films deposited at room temperature on BaF2(111) were in an amorphous state, but after exposure to an annealing treatment they crystallize in an epitaxial cubic structure. Film deposition on pre-cleaned and buffered ammonium fluoride etched Si(111) show growth of epitaxial hexagonal GST, similar to that of the deposition on BaF2(111). When the Si-substrates were heated directly to the deposition temperature films of high crystal-line quality were obtained. An additional heat treatment of the Si-substrates prior to deposition deteriorated the crystal quality severely. The gained results show that PLD can be used as a method in order to obtain high quality epitaxial Ge-Sb-Te films from a compound target and using high deposition rates.

UV and deep-UV selective photodiodes from visible-blind to solar-blind were realized based on a Si-doped (InxGa1–x)2O3 thin film with a monotonic lateral variation of 0.0035<x<0.83. Such layer was deposited by employing a continuous composition spread approach relying on the ablation of a single segmented target in pulsed-laser deposition. The photo response signal is provided from a metal-semiconductor-metal structure upon backside illumination. The absorption onset was tuned from 4.83 to 3.22 eV for increasing x. Higher responsivities were observed for photodiodes fabricated from indium-rich part of the sample, for which an internal gain mechanism could be identified. VC 2016 AIP Publishing LLC.

In recent years, ultra-wide bandgap semiconductors have increasingly moved into scientific focus due to their outstanding material properties, making them promising candidates for future applications within high-power electronics or solar-blind photo detectors. The group-III-sesquioxides can appear in various polymorphs, which influences, for instance, the energy of the optical bandgap. In gallium oxide, the optical bandgap ranges between 4.6 and 5.3 eV depending on the polymorph. For each polymorph it can be increased or decreased by alloying with aluminum oxide (8.8 eV) or indium oxide (2.7–3.75 eV), respectively, enabling bandgap engineering and thus leading to an extended application field. For this purpose, an overview of miscibility limits, the variation of bandgap and lattice constants as a function of the alloy composition are reviewed for the rhombohedral, monoclinic, orthorhombic and cubic polymorph. Further, the effect of formation and desorption of volatile suboxides on growth rates is described with respect to chemical trends of the discussed ternary materials.

This dissertation develops a computational method for simulating laser-induced cavitation and investigates the mechanism behind the formation of non-spherical bubbles induced by long-pulsed lasers. The proposed computational method accounts for the laser emission and absorption, phase transition, and the dynamics and thermodynamics of a two-phase fluid flow. In this new method, the model combines the Navier-Stokes (NS) equations for a compressible inviscid two-phase fluid flow, a new laser radiation equation, and a novel local thermodynamic model of phase transition. The Navier-Stokes equations are solved using the FInite Volume method with Exact two-phase Riemann solvers (FIVER). Following this method, numerical fluxes across phase boundaries are computed by constructing and solving one-dimensional bi-material Riemann problems. The new laser radiation equation is derived by customizing the radiative transfer equation (RTE) using the special properties of laser, including monochromaticity, directionality, high intensity, and a measurable focusing or diverging angle. An embedded boundary finite volume method is developed to solve the laser radiation equation on the same mesh created for the NS equations. The fluid mesh usually does not resolve the boundary and propagation directions of the laser beam, leading to the challenges of imposing the boundary conditions on the laser domain. To overcome this challenge, ghost nodes outside the laser domain are populated by mirroring and interpolation techniques. The existence and uniqueness of the solution are proved for the two-dimensional case, leveraging the special geometry of the laser domain. The method is up to second-order accuracy, which is also proved, and verified using numerical tests. A method of latent heat reservoir is developed to predict the onset of vaporization, which accounts for the accumulation and release of latent heat. In this work, the localized level set method is employed to track the bubble surface. Furthermore, the continuation of phase transition is possible in laser-induced cavitation problems, especially for long-pulsed lasers. A method of local correction and reinitialization is developed to account for continuous phase transitions. Several numerical tests are presented to verify the convergence of these methods. This multiphase laser-fluid coupled computational model is employed to simulate the formation and expansion of bubbles with different shapes induced by different long-pulsed lasers. The simulation results show that the computational method can capture the key phenomena in the laser-induced cavitation problems, including non-spherical bubble expansion, shock waves, and the ``Moses effect''. Additionally, the observed complex non-spherical shapes of vapor bubbles generated by long-pulsed laser reflect some characteristics (e.g., direction, width) of the laser beam. The dissertation also investigates the relation between bubble shapes and laser parameters and explores the transition between two commonly observed shapes -- namely, a rounded pear-like shape and an elongated conical shape -- using the proposed computational model. Two laboratory experiments are simulated, in which Holmium:YAG and Thulium fiber lasers are used respectively to generate bubbles of different shapes. In both cases, the predicted bubble nucleation and morphology agree reasonably well with the experimental observation. The full-field results of laser radiance, temperature, velocity, and pressure are analyzed to explain bubble dynamics and energy transmission. It is found that due to the lasting energy input, the vapor bubble's dynamics is driven not only by advection, but also by the continued vaporization at its surface. Vaporization lasts less than 1 microsecond in the case of the pear-shaped bubble, compared to over 50 microseconds for the elongated bubble. It is thus hypothesized that the bubble's morphology is determined by a competition between the speed of bubble growth due to advection and continuous vaporization. When the speed of advection is higher than that of vaporization, the bubble tends to grow spherically. Otherwise, it elongates along the laser beam direction. To test this hypothesis, the two speeds are defined analytically using a model problem and then estimated for the experiments using simulation results. The results support the hypothesis and also suggest that when the laser's power is fixed, a higher laser absorption coefficient and a narrower beam facilitate bubble elongation. / Doctor of Philosophy / Laser-induced cavitation is a process where laser beams create bubbles in a liquid. This phenomenon is widely applied in research and microfluidic applications for precise control of bubble dynamics. It also naturally occurs in various laser-based processes involving liquid environments. Understanding laser-induced cavitation is important for enhancing the effectiveness and safety of related technologies. However, experimental studies encounter limitations, highlighting the development of numerical methods to advance the understanding of laser-induced cavitation. The laser-induced cavitation can be roughly described as localized boiling through thermal radiation. The detailed physics involves the absorption of laser light by a liquid, the formation of vapor bubbles due to localized heating, and the dynamics of both the bubbles and the surrounding liquid. The first part of the dissertation introduces a new computational method for modeling these phenomena. The dynamics of the two-phase flow are modeled by the Navier-Stokes equations, which are solved using the FInite Volume method with Exact two-phase Riemann solvers (FIVER). The absorption of the laser light is modeled by a new laser radiation equation, which is derived from laser energy conservation and special properties of the laser. An embedded boundary finite volume method is developed to solve this equation on the same mesh created for the NS equations. Additionally, a method of latent heat reservoir is developed to predict the onset of vaporization. In this work, the level set method is employed to track the bubble surface, and a method of local correction and reinitialization is developed to account for possible continuous phase transitions. After developing this new method, several test cases are simulated. The simulation results show that the method can capture the key phenomena in the laser-induced cavitation problems, including the absorption of laser light, non-spherical bubble expansion, and shock waves. When the laser pulse is comparable to or longer than the acoustic time scale (long-pulsed laser), vapor bubbles generated often have complex non-spherical shapes. The bubble shapes reflect some characteristics (e.g., direction, width) of the laser beam. The second part of the dissertation investigates the relation between bubble shapes and laser parameters. Two laboratory experiments are simulated, in which two different lasers are used to generate bubbles of different shapes, namely, a rounded pear-like shape and an elongated conical shape. In both cases, the simulated bubbles exhibit shapes and sizes that reasonably match the experimental results. The simulation results of temperature, pressure, and velocity fields are analyzed to explain bubble dynamics and energy transmission. The analysis shows that the expansion of bubbles induced by long-pulsed lasers is determined not only by advection but also by the continued vaporization at its surface. Vaporization lasts less than $1$ microsecond in the case of the pear-shaped bubble, compared to over $50$ microseconds for the elongated bubble. It is thus hypothesized that the bubble expansion is determined by a competition between the speed of bubble growth due to advection and continuous vaporization. When the speed of advection is higher than that of vaporization, the bubble tends to grow spherically. Otherwise, it elongates along the laser beam direction. To test this hypothesis, the two speeds are defined analytically using a model problem and then estimated for the experiments using simulation results. The results support the hypothesis and also suggest that when the laser's power is fixed, a higher laser absorption coefficient and a narrower beam facilitate bubble elongation.

In dieser Arbeit werden das Wachstum und die Charakterisierung der Heterostruktur eines FeFET auf der Grundlage von BaSnO3, LaInO3 und (K,Na)NbO3 Schichten untersucht. Für jedes Material wurden die Wachstumsbedingungen bestimmt und im Hinblick auf die strukturellen und elektrischen Eigenschaften optimiert. Epitaktische BaSnO3 Filme, die auf SrTiO3 Substraten gewachsen sind, weisen eine hohe Dichte an Versetzungen auf, die ihre elektrischen Eigenschaften beeinträchtigen. Die Verwendung von NdScO3 Substraten und Einführung einer SrSnO3 Pufferschicht verbesserten die strukturellen und elektrischen Eigenschaften der BaSnO3 Schichten. Dies ermöglichte schließlich Untersuchungen an der LaInO3/BaSnO3 Grenzfläche. Schon eine geringe La-Dotierung der BaSnO3 Schicht von 0,3 % führte zur Bildung eines 2DEG nach der Grenzflächenbildung und damit zum Einschluss von Elektronen an der Grenzfläche. Dies konnte durch C-V, Van-der-Pauw und Hall-Effekt-Messungen eindeutig nachgewiesen werden. Eine deutliche Verbesserung der strukturellen und elektrischen Eigenschaften der BaSnO3 Schichten wurde durch die Verwendung von LaInO3:Ba Substraten erreicht. Diese sind gitterangepasst an BaSnO3, sodass zum ersten Mal vollständig verspannte Schichten ohne Versetzungen gewachsen werden konnten. Strukturelle und elektrische Eigenschaften von (K,Na)NbO3 Schichten wurden auf SrRuO3/DyScO3 und SrTiO3:Nb-Substraten untersucht. Auf diese Weise wurden der Einfluss der Gitterdehnung auf die kritische Schichtdicke und die Prozesse der plastischen Relaxation des Gitters bestimmt. Die elektrische Charakterisierung ergab einen hohen Leckstrom, der durch strukturelle Defekte verursacht wird. Die gesamte FeFET Heterostruktur wurde auf LaInO3:Ba Substraten gewachsen und untersucht. BaSnO3 und LaInO3 Schichten wuchsen kohärent, während (K,Na)NbO3 Schichten eine plastische Gitterrelaxation aufwiesen. Das führte zur Bildung von Strukturdefekten und zu einer Verschlechterung der ferroelektrischen Eigenschaften. / In this thesis, the design, growth and characterisation of the heterostructure of a FeFET based on BaSnO3, LaInO3 and (K,Na)NbO3 thin films are investigated. For each material, the growth conditions were determined and optimised with respect to their structural and electrical properties. Epitaxial BaSnO3 thin films grown on SrTiO3 substrates exhibit a high density of threading dislocations, which degrade their electrical properties. The use of NdScO3 substrates and the introduction of a SrSnO3 buffer layer improved the structural and electrical properties of the BaSnO3 thin films. This finally allowed investigations on the LaInO3/BaSnO3 heterointerface. Even a low La doping of the BaSnO3 layer of 0.3 % led to the formation of a 2DEG after interface formation and thus to the confinement of electrons at the interface. This could be clearly demonstrated by C-V, Van-der-Pauw and Hall effect measurements. A significant improvement of the structural and electrical properties of the BaSnO3 thin films was achieved by using LaInO3:Ba substrates. These are lattice-matched to BaSnO3 so that, for the first time, fully strained thin films could be grown without dislocations. Structural and electrical properties of (K,Na)NbO3 thin films were investigated on SrRuO3/DyScO3 and SrTiO3:Nb substrates. In this way, the influence of lattice strain on the critical film thickness and plastic lattice relaxation were determined. Their electrical characterisation revealed a high leakage current caused by structural defects. Therefore, the entire FeFET heterostructure was grown and investigated on LaInO3:Ba substrates. The BaSnO3 and LaInO3 thin films were grown coherently, while the (K,Na)NbO3 thin films exhibited plastic lattice relaxation. This led to the formation of structural defects and consequently to a deterioration of their ferroelectric properties.

No description available.