京都大学 / 新制・課程博士 / 博士(理学) / 甲第22992号 / 理博第4669号 / 新制||理||1670(附属図書館) / 京都大学大学院理学研究科物理学・宇宙物理学専攻 / (主査)教授 高柳 匡, 教授 青木 慎也, 教授 田中 貴浩 / 学位規則第4条第1項該当 / Doctor of Science / Kyoto University / DFAM

What are substitutes for domestic money and what is their legal regime? Abstract The thesis deals with the position of substitutes for domestic money in the Czech legal system and the phenomenon of substitutes for state money in general. The work is divided into three parts, in the first the author analyzes the current legal regulation of domestic money substitutes in the Czech legal system, concluding that the current regulation is clearly obsolete, while its interpretation by modern legal science is considered not only restrictive but also very formalistic, and thus not completely fulfilling the role set desired by original legislator. At the end of the first part, the author concludes that some selected forms of non-state money (especially corporate money and LETS systems) correspond to the current concept of substitutes for domestic money, but they can not be considered part of modern economic reality. In the second part, the author analyzes modern forms of non-state money with a focus on cryptocurrencies, as the most relevant form of non-state money. The author describes the gradual development and acceptance of virtual currencies both from the perspective of European regulators and from the perspective of their real economic use. The author concludes that a significant part of virtual currencies falls...

We employ the AdS/CFT correspondence and hydrodynamics to analyze the transport properties of \(2+1\) dimensional electron fluids. In this way, we use theoretical methods from both condensed matter and high-energy physics to derive tangible predictions that are directly verifiable in experiment. The first research topic we consider is strongly-coupled electron fluids. Motivated by early results by Gurzhi on the transport properties of weakly coupled fluids, we consider whether similar properties are manifest in strongly coupled fluids. More specifically, we focus on the hydrodynamic tail of the Gurzhi effect: A decrease in fluid resistance with increasing temperature due to the formation of a Poiseuille flow of electrons in the sample. We show that the hydrodynamic tail of the Gurzhi effect is also realized in strongly coupled and fully relativistic fluids, but with modified quantitative features. Namely, strongly-coupled fluids always exhibit a smaller resistance than weakly coupled ones and are, thus, far more efficient conductors. We also suggest that the coupling dependence of the resistance can be used to measure the coupling strength of the fluid. In view of these measurements, we provide analytical results for the resistance as a function of the shear viscosity over entropy density \(\eta/s\) of the fluid. \(\eta/s\) is itself a known function of the coupling strength in the weak and infinite coupling limits. In further analysis for strongly-coupled fluids, we propose a novel strongly coupled Dirac material based on a kagome lattice, Scandium-substituted Herbertsmithite (ScHb). The large coupling strength of this material, as well as its Dirac nature, provides us with theoretical and experimental access to non-perturbative relativistic and quantum critical physics. A highly suitable method for analyzing such a material's transport properties is the AdS/CFT correspondence. Concretely, using AdS/CFT we derive an estimate for ScHb's \(\eta/s\) and show that it takes a value much smaller than that observed in weakly coupled materials. In turn, the smallness of \(\eta/s\) implies that ScHb's Reynolds number, \(Re\), is large. In fact, \(Re\) is large enough for turbulence, the most prevalent feature of fluids in nature, to make its appearance for the first time in electronic fluids. Switching gears, we proceed to the second research topic considered in this thesis: Weakly coupled parity-breaking electron fluids. More precisely, we analyze the quantitative and qualitative changes to the classical Hall effect, for electrons propagating hydrodynamically in a lead. Apart from the Lorentz force, a parity-breaking fluid's motion is also impacted by the Hall-viscous force; the shear-stress force induced by the Hall-viscosity. We show that the interplay of these two forces leads to a hydrodynamic Hall voltage with non-linear dependence on the magnetic field. More importantly, the Lorentz and Hall-viscous forces become equal at a non-vanishing magnetic field, leading to a trivial hydrodynamic Hall voltage. Moreover, for small magnetic fields we provide analytic results for the dependence of the hydrodynamic Hall voltage on all experimentally-tuned parameters of our simulations, such as temperature and density. These dependences, along with the zero of the hydrodynamic Hall voltage, are distinct features of hydrodynamic transport and can be used to verify our predictions in experiments. Last but not least, we consider how a distinctly electronic property, spin, can be included into the hydrodynamic framework. In particular, we construct an effective action for non-dissipative spin hydrodynamics up to first order in a suitably defined derivative expansion. We also show that interesting spin-transport effects appear at second order in the derivative expansion. Namely, we show that the fluid's rotation polarizes its spin. This is the hydrodynamic manifestation of the Barnett effect and provides us with an example of hydrodynamic spintronics. To conclude this thesis, we discuss several possible extensions of our research, as well as proposals for research in related directions. / Wir verwenden die AdS/CFT-Korrespondenz und die Theorie der Hydrodynamik, um die Transporteigenschaften von \(2+1\)-dimensionalen Elektronisches Flüssigkeiten zu untersuchen. Somit nutzen wir sowohl theoretische Methoden der Fest\-körper\-physik als auch der Hochenergiephysik, um konkrete Vorhersagen zu treffen, die unmittelbar in Experimenten verifiziert werden können. Zunächst betrachten wir das Forschungsfeld der stark gekoppelten Elektronischen Flüssigkeiten. Motiviert durch die frühen Ergebnisse für die Transporteigenschaften schwach gekoppelter Flüssigkeiten von Gurzhi untersuchen wir, ob sich ähnliche Eigenschaften auch in stark gekoppelten Flüssigkei\-ten manifestieren. Dabei konzentrieren wir uns insbesondere auf den hydrodynamischen Teil des Gurzhi-Effekts, in welchem der Widerstand der Flüssigkeit mit steigender Temperatur sinkt, weil sich im untersuchten Material ein Poiseuillefluss von Elektronen bildet. Wir zeigen, dass dieser hydrodynamische Teil des Gurzhi-Effekts auch in stark gekoppelten und vollständig relativistischen Flüssigkeiten realisiert ist, einige Eigenschaften sich hierbei aber quantitativ unterscheiden. Insbesondere zeigen stark gekoppelte Flüssigkeiten immer kleinere Widerstände als schwach gekoppelte, und sind damit wesentlich effektivere Leiter. Wir schlagen darüber hinaus vor, die Abhängigkeit des Widerstands von der Kopplung zu nutzen, um die Kopplungsstärke der Flüssigkeit zu messen. Für diese Messungen stellen wir analytische Ergebnisse bereit, welche den Widerstand als Funktion des Quotienten aus Scherviskosität und Entropiedichte \(\eta/s\) der Flüssigkeit ausdrücken. Dabei ist \(\eta/s\) selbst eine bekannte Funktion der Kopplungsstärke in den Grenzfällen schwacher und unendlich starker Kopplung. In einer weiteren Untersuchung stark gekoppelter Flüssigkeiten schlagen wir Scandium-substituiertes Herbertsmithit (ScHb) als neuartiges, stark gekoppeltes Diracmaterial vor, welches auf dem Kagome-Gitter basiert. Die hohe Kopplungsstärke und die Dirac-Eigenschaften dieses Materials vermitteln uns theoretischen und experimentellen Zugang zu nicht perturbativer relativistischer und quantenkritischer Physik. Um die Transporteigenschaften eines solchen Materials zu untersuchen, stellt die AdS/CFT-Korrespondenz eine hervorragend geeignete Methode dar. Konkret nutzen wir AdS/CFT, um eine Abschätzung von \(\eta/s\) in ScHb herzuleiten. Der so ermittelte Wert ist wesentlich kleiner als der entsprechende Messwert für schwach gekoppelte Materialien. Der kleine Wert von \(\eta/s\) wiederum impliziert, dass die Reynolds-Zahl \(Re\) in ScHb groß ist. Tatsächlich ist \(Re\) hinreichend groß, um erstmals Turbulenz in Elektronisches Flüssigkeiten beobachten zu können, ein Effekt, der auch in viele anderen Flüssigkeiten in der Natur vorkommt. Wir gehen zum zweiten Forschungsthema über, welches in der vorliegenden Arbeit besprochen wird: schwach gekoppelte, paritätsbrechende Elektronisches Flüssigkeiten. Wir betracthen die hydrodynamische Bewegung von Elektronen in einen zwei dimensionalen Kanal, und untersuchen die sich ergebenden quantitativen und qualitativen Änderungen gegenüber dem klassischen Hall-Effekt. Außer der Lorentzkraft ist die Bewegung einer paritätsbrechenden Flüss auch den Einflüssen der Hallviskositätskraft ausgesetzt, welche die von der Hall Viskosität induzierte Scherspannungskraft ist. Wir zeigen, dass das Wechselspiel dieser beiden Kräfte zu einer hydrodynamischen Hall-Spannung führt, die nicht linear vom magnetischen Feld abhängt. Noch wichtiger ist, dass Lorentz- sowie hallviskose Kraft für ein nicht verschwindendes Magnetfeld gleich werden und damit zu einer trivialen hydrodynamischen Hall-Spannung führen. Darüber hinaus geben wir für kleine Magnetfeldstärken analytische Ergebnisse an, die die Abhängigkeit der hydrodynamischen Hall-Spannung von allen experimentell festgelegten Parametern unserer Simulation, wie z.B. Temperatur und Dichte, beschreiben. Diese Abhängigkeiten sind zusammen mit der verschwindenden hydrodynamischen Hall-Spannung charakteristische Eigenschaften hydrodynamischen Transports und können daher verwendet werden, um unsere Vorhersagen experimentell zu verifizieren. Zu guter Letzt untersuchen wir, wie eine charakteristische Eigenschaft von Elektronen, der Spin, in die hydrodynamische Theorie einbezogen werden kann. Dazu konstruieren wir eine effektive Wirkung, die nicht dissipative Spin-Hydrodynamik bis zur ersten Ordnung in einer geeigneten Ableitungsentwicklung beschreibt. Wir zeigen darüber hinaus, dass in zweiter Ordnung dieser Entwicklung interessante Spin-Transporteffekte auftreten. Dabei stellt sich heraus, dass die Rotation der Flüssigkeit seinen Spin polarisiert. Dies ist die hydrodynamische Manifestation des Barnett-Effekts, die als Beispiel für hydrodynamische Spintronics dient. Zum Abschluss der vorliegenden Arbeit diskutieren wir mehrere mögliche Erweiterungen unserer Untersuchungen und unterbreiten Vorschläge für weitergehende Forschung in verschiedene Richtungen.

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In the following thesis, I will conduct a thermodynamic analysis of the Taub-NUT spacetime in various dimensions, as well as show uses for Taub-NUT and other Hyper-Kahler spacetimes. <br /><br /> Thermodynamic analysis (by which I mean the calculation of the entropy and other thermodynamic quantities, and the analysis of these quantities) has in the past been done by use of background subtraction. The recent derivation of the (A)dS/CFT correspondences from String theory has allowed for easier and quicker analysis. I will use Taub-NUT space as a template to test these correspondences against the standard thermodynamic calculations (via the N&ouml;ether method), with (in the Taub-NUT-dS case especially) some very interesting results. <br /><br /> There is also interest in obtaining metrics in eleven dimensions that can be reduced down to ten dimensional string theory metrics. Taub-NUT and other Hyper-Kahler metrics already possess the form to easily facilitate the Kaluza-Klein reduction, and embedding such metrics into eleven dimensional metrics containing M2 or M5 branes produces metrics with interesting Dp-brane results.

Este é um trabalho de revisão. Os principais formalismos no desenvolvimento da teoria de cordas são introduzidos e discutidos: a corda bosônica e as supercordas no formalismo de Ramond-Neveu-Schwarz e no formalismo de Green-Schwarz. São introduzidas também as açôes efetivas no limite de baixas energias das D-branas (ação DBI) e das teorias de supergravidade (D=10,11). Por fim, são analisados alguns aspectos da correspondência AdS/CFT, enunciando a conjectura e introduzindo algumas das entradas do dicionário. Os apêndices contêm tópicos de grande relevância para o texto e podem ajudar a esclarecer vários raciocínios e passagens ao longo do mesmo. / This is a review work. The main formalisms on the development of string theory are introduced and discussed: the bosonic string and the superstrings formalisms of Ramond-Never-Schwarz and Green-Schwarz. The effective actions in the low energy limit of the D-branes (DBI action) and supergravity theories (D=10,11) are introduced as well. Finally, some aspects of the AdS/CFT correspondence are analised, enunciating the conjecture and introducing some entries of the dictionary. The appendices contains some topics that are highly relevant for the whole text and may help clarify several ideas and arguments through it.

Esta tese é um estudo de estabilidade de modos quasinormais em um sistema que apresenta uma mudança de estabilidade ao variar continuamente os parâmetros físicos de um buraco negro. A mudança de estabilidade encontrada possui interpretações na correspondência AdS/CFT. A ferramenta principal utilizada neste trabalho para o cálculo de modos quasinormais foram métodos numéricos que podem ser utilizados em inúmeros trabalhos desta área de pesquisa, especialmente por não dependerem de suposições de simetria ou de comportamento conveniente do sistema físico. / This thesis is a study of stability of quasinormal modes in a system featuring a stability change if one continuously varies the physical parameters of a black hole. The stability change thus found has some possible interpretations in the AdS/CFT correspondence. The main tool used in this study for calculating quasinormal modes are numerical methods that can be used in numerous works in this area of research, especially because they do not depend on assumptions of symmetry or any convenient behavior of the physical system.

O escopo deste mestrado é de se familiarizar com a chamada {\\it correspondência AdS/CFT}, que tem sido um dos mais importantes desenvolvimentos na física teórica nas últimas décadas. De acordo com essa correspondência, deformações das geometrias do lado da gravidade (ou lado \"AdS\") devem ser mapeadas para operadores das teorias de calibre duais (ou lado \"CFT\"). Em particular, nos temos estado interessados em explorar uma entrada particular no dicionário AdS/CFT, a relação entre os operadores 1/2 BPS em ${\\cal N}=4$ super Yang-Mills, e as chamadas {\\it geometrias bubbling} no lado da gravidade. A fim de fazer isso, apresentamos primeiramente as noções de ${\\cal N}=4$ SYM e soluções de Supergravidade. Portanto, podemos expor mais claramente o sentido da correspondência AdS /CFT, e depois mostrar a derivação das geometrias 1/2 BPS duais a estados 1/2 BPS em ${\\cal N}=4$ SYM como um exemplo. / The scope of this Master program was to get acquainted with the so-called {\\it AdS/CFT correspondence}, which has been one of the most important developments in theoretical physics in the last decades. According to this correspondence, deformations of the geometries in the gravity side (or \"AdS\" side) must be mapped to states of the dual gauge theories (or \"CFT\" side). In particular, we have been interested in exploring a particular entry in the AdS/CFT dictionary, namely, the relation between 1/2 BPS operators in ${\\cal N}=4$ super Yang-Mills, and the so-called {\\it bubbling geometries} on the gravity side. In order to do that, we first present the notions of N=4 SYM and Supergravity solutions. In this way, we can expose the statement of the AdS/CFT correspondence, and later show the derivation of 1/2 BPS geometries dual to 1/2 BPS states in N=4 SYM as an example of this one.

The holographic principle has become an extraordinary tool in theoretical physics, most notably in the form of the Anti-deSitter Conformal Field Theory (AdS/CFT) correspondence, in which classical gravitational degrees of freedom in N-dimensions are related quantum field theory degrees of freedom in N − 1 dimensions in the limit of a large number of fields. Here we present an account of the AdS/CFT correspondence, also known as the gauge/gravity duality, from its origins in the large N 'tHooft expansion, up to Maldacena's proposal that type IIB string theory in the presences of D-branes at low energy is dual to an N = 4, d = 4, U(N) super Yang-Mills on AdS5 × S5 . We begin with an extensive review of (super)string theory including D-branes. We then present the general formulation of the AdS/CFT in the supergravity background of AdS5 × S5 , along with several examples of how it is used in terms of the identification of bulk fields with operators on the bound- ary of a CFT. We move on to discuss two applications of the gauge/gravity duality. The first is the application of the holographic gauge/gravity correspondence to the QCDk-string. The second applies the AdS/CFT formalism to a Kerr black hole solution embedded in 10-dimensional heterotic sting theory. These two applications of the holographic gauge/gravity duality comprise the original work presented here. We follow with summaries and discussions of the background material, the original work, and future investigations.