Thermalization, the evolution of an interacting many-body system towards a thermal Gibbs ensemble after initialization in an arbitrary non-equilibrium state, is currently a phenomenon of great interest, both in theory and experiment. As the time evolution of a quantum system is unitary, the proposed mechanism of thermalization in quantum many-body systems corresponds to the so-called eigenstate thermalization hypothesis (ETH) and the typicality of eigenstates. Although this formally solves the contradiction of thermalizing but unitary dynamics in a closed quantum many-body system, it does neither make any statement on the dynamical process of thermalization itself nor in which way the coupling of the system to an environment can hinder or modify the relaxation dynamics. In this thesis, we address both the question whether or not a quantum system driven away from equilibrium is able to relax to a thermal state, which fulfills detailed balance, and if one can identify universal behavior in the non-equilibrium relaxation dynamics. As a first realization of driven quantum systems out of equilibrium, we investigate a system of Ising spins, interacting with the quantized radiation field in an optical cavity. For multiple cavity modes, this system forms a highly entangled and frustrated state with infinite correlation times, known as a quantum spin glass. In the presence of drive and dissipation, introduced by coupling the intra-cavity radiation field to the photon vacuum outside the cavity via lossy mirrors, the quantum glass state is modified in a universal manner. For frequencies below the photon loss rate, the dissipation takes over and the system shows the universal behavior of a dissipative spin glass, with a characteristic spectral density $\\mathcal{A}(\\omega)\\sim\\sqrt{\\omega}$. On the other hand, for frequencies above the loss rate, the system retains the universal behavior of a zero temperature, quantum spin glass. Remarkably, at the glass transition, the two subsystems of spins and photons thermalize to a joint effective temperature, even in the presence of photon loss. This thermalization is a consequence of the strong spin-photon interactions, which favor detailed balance in the system and detain photons from escaping the cavity. In the thermalized system, the features of the spin glass are mirrored onto the photon degrees of freedom, leading to an emergent photon glass phase. Exploiting the inherent photon loss of the cavity, we make predictions of possible measurements on the escaping photons, which contain detailed information of the state inside the cavity and allow for a precise, non-destructive measurement of the glass state. As a further set of non-equilibrium systems, we consider one-dimensional quantum fluids driven out of equilibrium, whose universal low energy theory is formed by the so-called Luttinger Liquid description, which, due to its large degree of universality, is of intense theoretical and experimental interest. A set of recent experiments in research groups in Vienna, Innsbruck and Munich have probed the non-equilibrium time-evolution of one-dimensional quantum fluids for different experimental realizations and are pushing into a time regime, where thermalization is expected. From a theoretical point of view, one-dimensional quantum fluids are particular interesting, as Luttinger Liquids are integrable and therefore, due to an infinite number of constants of motion, do not thermalize. The leading order correction to the quadratic theory is irrelevant in the sense of the renormalization group and does therefore not modify static correlation functions, however, it breaks integrability and will therefore, even if irrelevant, induce a completely different non-equilibrium dynamics as the quadratic Luttinger theory alone. In this thesis, we derive for the first time a kinetic equation for interacting Luttinger Liquids, which describes the time evolution of the excitation densities for arbitrary initial states. The resonant character of the interaction makes a straightforward derivation of the kinetic equation, using Fermi\'s golden rule, impossible and we have to develop non-perturbative techniques in the Keldysh framework. We derive a closed expression for the time evolution of the excitation densities in terms of self-energies and vertex corrections. Close to equilibrium, the kinetic equation describes the exponential decay of excitations, with a decay rate $\\sigma^R=\\mbox\\Sigma^R$, determined by the self-energy at equilibrium. However, for long times $\\tau$, it also reveals the presence of dynamical slow modes, which are the consequence of exactly energy conserving dynamics and lead to an algebraic decay $\\sim\\tau^$ with $\\eta_D=0.58$. The presence of these dynamical slow modes is not contained in the equilibrium Matsubara formalism, while they emerge naturally in the non-equilibrium formalism developed in this thesis. In order to initialize a one-dimensional quantum fluid out of equilibrium, we consider an interaction quench in a model of interacting, dispersive fermions in Chap.~\\ref. In this scenario, the fermionic interaction is suddenly changed at time $t=0$, such that for $t>0$ the system is not in an eigenstate and therefore undergoes a non-trivial time evolution. For the quadratic theory, the stationary state in the limit $t\\rightarrow\\infty$ is a non-thermal, or prethermal, state, described by a generalized Gibbs ensemble (GGE). The GGE takes into account for the conservation of all integrals of motion, formed by the eigenmodes of the Hamiltonian. On the other hand, in the presence of non-linearities, the final state for $t\\rightarrow\\infty$ is a thermal state with a finite temperature $T>0$. . The spatio-temporal, dynamical thermalization process can be decomposed into three regimes: A prequench regime on the largest distances, which is determined by the initial state, a prethermal plateau for intermediate distances, which is determined by the metastable fixed point of the quadratic theory and a thermal region on the shortest distances. The latter spreads sub-ballistically $\\sim t^$ in space with $0<\\alpha<1$ depending on the quench. Until complete thermalization (i.e. for times $t<\\infty$), the thermal region contains more energy than the prethermal and prequench region, which is expressed in a larger temperature $T_{t}>T_$, decreasing towards its final value $T_$. As the system has achieved local detailed balance in the thermalized region, energy transport to the non-thermal region can only be performed by the macroscopic dynamical slow modes and the decay of the temperature $T_{t}-T_\\sim t^$ again witnesses the presence of these slow modes. The very slow spreading of thermalization is consistent with recent experiments performed in Vienna, which observe a metastable, prethermal state after a quench and only observe the onset of thermalization on much larger time scales. As an immediate indication of thermalization, we determine the time evolution of the fermionic momentum distribution after a quench from non-interacting to interacting fermions. For this quench scenario, the step in the Fermi distribution at the Fermi momentum $k\\sub$ decays to zero algebraically in the absence of a non-linearity but as a stretched exponential (the exponent being proportional to the non-linearity) in the presence of a finite non-linearity. This can serve as a proof for the presence or absence of the non-linearity even on time-scales for which thermalization can not yet be observed. Finally, we consider a bosonic quantum fluid, which is driven away from equilibrium by permanent heating. The origin of the heating is atomic spontaneous emission of laser photons, which are used to create a coherent lattice potential in optical lattice experiments. This process preserves the system\'s $U(1)$-invariance, i.e. conserves the global particle number, and the corresponding long-wavelength description is a heated, interacting Luttinger Liquid, for which phonon modes are continuously populated with a momentum dependent rate $\\partial_tn_q\\sim\\gamma |q|$. In the dynamics, we identify a quasi-thermal regime for large momenta, featuring an increasing time-dependent effective temperature. In this regime, due to fast phonon-phonon scattering, detailed balance has been achieved and is expressed by a time-local, increasing temperature. The thermal region emerges locally and spreads in space sub-ballistically according to $x_t\\sim t^{4/5}$. For larger distances, the system is described by an non-equilibrium phonon distribution $n_q\\sim |q|$, which leads to a new, non-equilibrium behavior of large distance observables. For instance, the phonon decay rate scales universally as $\\gamma_q\\sim |q|^{5/3}$, with a new non-equilibrium exponent $\\eta=5/3$, which differs from equilibrium. This new, universal behavior is guaranteed by the $U(1)$ invariant dynamics of the system and is insensitive to further subleading perturbations. The non-equilibrium long-distance behavior can be determined experimentally by measuring the static and dynamic structure factor, both of which clearly indicate the exponents for phonon decay, $\\eta=5/3$ and for the spreading of thermalization $\\eta_T=4/5$. Remarkably, even in the presence of this strong external drive, the interactions and their aim to achieve detailed balance are strong enough to establish a locally emerging and spatially spreading thermal region. The physical setups in this thesis do not only reveal interesting and new dynamical features in the out-of-equilibrium time evolution of interacting systems, but they also strongly underline the high degree of universality of thermalization for the classes of models studied here. May it be a system of coupled spins and photons, where the photons are pulled away from a thermal state by Markovian photon decay caused by a leaky cavity, a one-dimensional fermionic quantum fluid, which has been initialized in an out-of-equilibrium state by a quantum quench or a one-dimensional bosonic quantum fluid, which is driven away from equilibrium by continuous, external heating, all of these systems at the end establish a local thermal equilibrium, which spreads in space and leads to global thermalization for $t\\rightarrow\\infty$. This underpins the importance of thermalizing collisions and endorses the standard approach of equilibrium statistical mechanics, describing a physical system in its steady state by a thermal Gibbs ensemble.

No description available.

In unserem täglichen Leben begegnen wir Tropfen oft in physikalischen Systems, beispielsweise als Öltropfen in Salatsoße. Diese Tropfen sind meist chemisch inaktiv. In biologischen Zellen bilden Proteine und RNA zusammen Tropfen. Zellen sind chemisch aktiv, so dass die Tropfenkomponenten neu gebildet, abgebaut und modifiziert werden können. In dieser Doktorarbeit wird das dynamische Verhalten von chemisch aktiven Tropfen mit analytischen und numerischen Methoden untersucht. Um das dynamische Verhalten von solchen aktiven Tropfen zu untersuchen, benutzen wir ein Minimalmodell mit zwei Komponenten, die zwei Phasen bilden und durch chemische Reaktionen ineinander umgewandelt werden. Die chemischen Reaktionen werden durch das Brechen von Detailed Balance aus dem Gleichgewicht gehalten, so dass die Tropfen chemisch aktiv sind. Wir konzentrieren uns auf den Fall, in dem Tropfenmaterial im Tropfen in die äußere Komponente umgewandelt wird, und in der äußeren Phase erzeugt wird. Wir finden ein vielfältiges dynamisches Phasendiagramm mit Regionen, in denen Tropfen schrumpfen und verschwinden, Regionen, in denen Tropfen eine stabile stationäre Größe besitzen, und Regionen, in denen eine Forminstabilität zu komplexer Tropfen-Dynamik führt. In der letzten Region deformieren sich Tropfen typischenweise prolat, verformen sich zu einer Hantel, und teilen sich in zwei Tochtertropfen, die wieder anwachsen. Dies kann zu Zyklen von Wachstum und Teilung von Tropfen führen, bis die Tropfen das gesamte Volumen füllen. Während spherische Tropfen durch die chemischen Reaktionen entgegen ihrer Oberflächenspannung deformiert werden, können Tropfen- Zylinder und Platten durch chemische Reaktionen stabilisiert werden. Generell ist die Dynamik von Tropfen ein hydrodynamisches Problem, da die Oberflächenspannung von deformierten Tropfen hydrodynamische Flüsse erzeugt. Wir finden, dass chemische Reaktionen entgegen die Oberflächenspannung Arbeit verrichten können, so dass die Tropfenteilung auch unter Berücksichtigung hydrodynamischer Flüsse möglich ist. Diese Doktorarbeit zeigt, dass die Kombination von chemische Reaktionen und Phasenseparation unter Nichtgleichgewichtsbedingungen zu neuem dynamischen Verhalten führen kann. Die Ergebnisse zeigen die Relevanz von chemischen Reaktionen zum Verständnis von Phasenseparation in biologischen Systemen auf, und können bei der Umsetzung der diskutierten Phänomene in experimentellen Systemen helfen. Die Tropfenteilung, die in dieser Doktorarbeit diskutiert wird, erinnert an die Teilung von biologischen Zellen. Davon motiviert schlagen wir vor, dass die Teilung von chemisch aktiven Tropfen ein Mechanismus für die Replikation von Tropfen-artigen Protozellen am Ursprung des Lebens gewesen sein könnte.:1. Introduction 2. Theory of multi-component phase-separating systems with chemical reactions 3. Minimal model for chemically active droplets in two formulations 4. Shape instability of spherical droplets with chemical reactions 5. Dynamical behavior of chemically active droplets 6. Shape instability of droplets with various geometries 7. Role of hydrodynamic flows in chemically driven droplet division 8. Chemically active droplets as a model for protocells at the origin of life 9. Conclusion Appendices / In our everyday environment, we regularly encounter liquid-liquid phase separation in physical systems such as oil droplets in vinegar. These droplets tend to be chemically inert. In biological cells, protein and RNA may together form liquid droplets. Cells are chemically active, so that droplet components can be created, degraded and modified. In this thesis we study the influence of nonequilibrium chemical reactions on the shape dynamics of a droplet theoretically, using analytical and numerical methods. To discuss the dynamical behavior that results from combining phase separation and chemical reactions in sustained nonequilibrium conditions, we introduce a minimal model with only two components that separate into distinct phases. These two components are converted into each other by chemical reactions. The reactions are kept out of equilibrium by breaking of detailed balance, so that the droplet becomes active. We concentrate on the case where the reaction inside the droplet degrades droplet material into the outer component, and where the reaction outside creates new droplet material. We find that chemically active droplets have a rich dynamic phase space, with regions where droplets shrink and vanish, regions where droplets have a stable stationary size, and regions where the flux-driven instability leads to complex dynamic behavior of droplets. In the latter, droplets typically elongate into a dumbbell shape and then split into two symmetrical daughter droplets. These droplets then grow until they have the same size as the initial droplet. This can lead to cycles of growth and division, so that an initial droplet divides until droplets fill the simulation volume. We analyze the stationary spherical state of the droplet, which is created by a balance of the fluxes driven by the chemical reactions. We find that stationary droplets may have a shape instability, which is driven by the continuous fluxes across the droplet interface and which may trigger the division. We also find that while reactions may destabilize spherical droplet shapes despite the surface tension of the droplet, they can have stabilizing effects on cylindrical droplets and droplet plates. Generally, the shape dynamics of droplets is a hydrodynamic problem because surface tension in non-spherical droplets drives hydrodynamic flows that redistribute material and deform the droplet shape. We therefore study the influence of hydrodynamic flows on the shape changes of chemically active droplets. We find that chemical reactions in active droplets can perform work against surface tension and flows, so that the droplet division is possible even in the presence of hydrodynamic flows. The present thesis highlights how the combination of basic physical behaviors – phase separation and chemical reactions – may create novel dynamic behavior under sustained nonequilibrium conditions. The results demonstrate the importance of considering chemical reactions for understanding the dynamics of droplets in biological systems, as well as proposes a minimalist model for experimentalists that are interested in creating a system of dividing droplets. Finally, the division of chemically active droplets is reminiscent of the division of biological cells, and it motivates us to propose that chemically active droplets could have provided a simple mechanism for the self-replication of droplet-like protocells at the origin of life.:1. Introduction 2. Theory of multi-component phase-separating systems with chemical reactions 3. Minimal model for chemically active droplets in two formulations 4. Shape instability of spherical droplets with chemical reactions 5. Dynamical behavior of chemically active droplets 6. Shape instability of droplets with various geometries 7. Role of hydrodynamic flows in chemically driven droplet division 8. Chemically active droplets as a model for protocells at the origin of life 9. Conclusion Appendices

Thermalization, the evolution of an interacting many-body system towards a thermal Gibbs ensemble after initialization in an arbitrary non-equilibrium state, is currently a phenomenon of great interest, both in theory and experiment. As the time evolution of a quantum system is unitary, the proposed mechanism of thermalization in quantum many-body systems corresponds to the so-called eigenstate thermalization hypothesis (ETH) and the typicality of eigenstates. Although this formally solves the contradiction of thermalizing but unitary dynamics in a closed quantum many-body system, it does neither make any statement on the dynamical process of thermalization itself nor in which way the coupling of the system to an environment can hinder or modify the relaxation dynamics. In this thesis, we address both the question whether or not a quantum system driven away from equilibrium is able to relax to a thermal state, which fulfills detailed balance, and if one can identify universal behavior in the non-equilibrium relaxation dynamics. As a first realization of driven quantum systems out of equilibrium, we investigate a system of Ising spins, interacting with the quantized radiation field in an optical cavity. For multiple cavity modes, this system forms a highly entangled and frustrated state with infinite correlation times, known as a quantum spin glass. In the presence of drive and dissipation, introduced by coupling the intra-cavity radiation field to the photon vacuum outside the cavity via lossy mirrors, the quantum glass state is modified in a universal manner. For frequencies below the photon loss rate, the dissipation takes over and the system shows the universal behavior of a dissipative spin glass, with a characteristic spectral density $\\mathcal{A}(\\omega)\\sim\\sqrt{\\omega}$. On the other hand, for frequencies above the loss rate, the system retains the universal behavior of a zero temperature, quantum spin glass. Remarkably, at the glass transition, the two subsystems of spins and photons thermalize to a joint effective temperature, even in the presence of photon loss. This thermalization is a consequence of the strong spin-photon interactions, which favor detailed balance in the system and detain photons from escaping the cavity. In the thermalized system, the features of the spin glass are mirrored onto the photon degrees of freedom, leading to an emergent photon glass phase. Exploiting the inherent photon loss of the cavity, we make predictions of possible measurements on the escaping photons, which contain detailed information of the state inside the cavity and allow for a precise, non-destructive measurement of the glass state. As a further set of non-equilibrium systems, we consider one-dimensional quantum fluids driven out of equilibrium, whose universal low energy theory is formed by the so-called Luttinger Liquid description, which, due to its large degree of universality, is of intense theoretical and experimental interest. A set of recent experiments in research groups in Vienna, Innsbruck and Munich have probed the non-equilibrium time-evolution of one-dimensional quantum fluids for different experimental realizations and are pushing into a time regime, where thermalization is expected. From a theoretical point of view, one-dimensional quantum fluids are particular interesting, as Luttinger Liquids are integrable and therefore, due to an infinite number of constants of motion, do not thermalize. The leading order correction to the quadratic theory is irrelevant in the sense of the renormalization group and does therefore not modify static correlation functions, however, it breaks integrability and will therefore, even if irrelevant, induce a completely different non-equilibrium dynamics as the quadratic Luttinger theory alone. In this thesis, we derive for the first time a kinetic equation for interacting Luttinger Liquids, which describes the time evolution of the excitation densities for arbitrary initial states. The resonant character of the interaction makes a straightforward derivation of the kinetic equation, using Fermi\'s golden rule, impossible and we have to develop non-perturbative techniques in the Keldysh framework. We derive a closed expression for the time evolution of the excitation densities in terms of self-energies and vertex corrections. Close to equilibrium, the kinetic equation describes the exponential decay of excitations, with a decay rate $\\sigma^R=\\mbox\\Sigma^R$, determined by the self-energy at equilibrium. However, for long times $\\tau$, it also reveals the presence of dynamical slow modes, which are the consequence of exactly energy conserving dynamics and lead to an algebraic decay $\\sim\\tau^$ with $\\eta_D=0.58$. The presence of these dynamical slow modes is not contained in the equilibrium Matsubara formalism, while they emerge naturally in the non-equilibrium formalism developed in this thesis. In order to initialize a one-dimensional quantum fluid out of equilibrium, we consider an interaction quench in a model of interacting, dispersive fermions in Chap.~\\ref. In this scenario, the fermionic interaction is suddenly changed at time $t=0$, such that for $t>0$ the system is not in an eigenstate and therefore undergoes a non-trivial time evolution. For the quadratic theory, the stationary state in the limit $t\\rightarrow\\infty$ is a non-thermal, or prethermal, state, described by a generalized Gibbs ensemble (GGE). The GGE takes into account for the conservation of all integrals of motion, formed by the eigenmodes of the Hamiltonian. On the other hand, in the presence of non-linearities, the final state for $t\\rightarrow\\infty$ is a thermal state with a finite temperature $T>0$. . The spatio-temporal, dynamical thermalization process can be decomposed into three regimes: A prequench regime on the largest distances, which is determined by the initial state, a prethermal plateau for intermediate distances, which is determined by the metastable fixed point of the quadratic theory and a thermal region on the shortest distances. The latter spreads sub-ballistically $\\sim t^$ in space with $0<\\alpha<1$ depending on the quench. Until complete thermalization (i.e. for times $t<\\infty$), the thermal region contains more energy than the prethermal and prequench region, which is expressed in a larger temperature $T_{t}>T_$, decreasing towards its final value $T_$. As the system has achieved local detailed balance in the thermalized region, energy transport to the non-thermal region can only be performed by the macroscopic dynamical slow modes and the decay of the temperature $T_{t}-T_\\sim t^$ again witnesses the presence of these slow modes. The very slow spreading of thermalization is consistent with recent experiments performed in Vienna, which observe a metastable, prethermal state after a quench and only observe the onset of thermalization on much larger time scales. As an immediate indication of thermalization, we determine the time evolution of the fermionic momentum distribution after a quench from non-interacting to interacting fermions. For this quench scenario, the step in the Fermi distribution at the Fermi momentum $k\\sub$ decays to zero algebraically in the absence of a non-linearity but as a stretched exponential (the exponent being proportional to the non-linearity) in the presence of a finite non-linearity. This can serve as a proof for the presence or absence of the non-linearity even on time-scales for which thermalization can not yet be observed. Finally, we consider a bosonic quantum fluid, which is driven away from equilibrium by permanent heating. The origin of the heating is atomic spontaneous emission of laser photons, which are used to create a coherent lattice potential in optical lattice experiments. This process preserves the system\'s $U(1)$-invariance, i.e. conserves the global particle number, and the corresponding long-wavelength description is a heated, interacting Luttinger Liquid, for which phonon modes are continuously populated with a momentum dependent rate $\\partial_tn_q\\sim\\gamma |q|$. In the dynamics, we identify a quasi-thermal regime for large momenta, featuring an increasing time-dependent effective temperature. In this regime, due to fast phonon-phonon scattering, detailed balance has been achieved and is expressed by a time-local, increasing temperature. The thermal region emerges locally and spreads in space sub-ballistically according to $x_t\\sim t^{4/5}$. For larger distances, the system is described by an non-equilibrium phonon distribution $n_q\\sim |q|$, which leads to a new, non-equilibrium behavior of large distance observables. For instance, the phonon decay rate scales universally as $\\gamma_q\\sim |q|^{5/3}$, with a new non-equilibrium exponent $\\eta=5/3$, which differs from equilibrium. This new, universal behavior is guaranteed by the $U(1)$ invariant dynamics of the system and is insensitive to further subleading perturbations. The non-equilibrium long-distance behavior can be determined experimentally by measuring the static and dynamic structure factor, both of which clearly indicate the exponents for phonon decay, $\\eta=5/3$ and for the spreading of thermalization $\\eta_T=4/5$. Remarkably, even in the presence of this strong external drive, the interactions and their aim to achieve detailed balance are strong enough to establish a locally emerging and spatially spreading thermal region. The physical setups in this thesis do not only reveal interesting and new dynamical features in the out-of-equilibrium time evolution of interacting systems, but they also strongly underline the high degree of universality of thermalization for the classes of models studied here. May it be a system of coupled spins and photons, where the photons are pulled away from a thermal state by Markovian photon decay caused by a leaky cavity, a one-dimensional fermionic quantum fluid, which has been initialized in an out-of-equilibrium state by a quantum quench or a one-dimensional bosonic quantum fluid, which is driven away from equilibrium by continuous, external heating, all of these systems at the end establish a local thermal equilibrium, which spreads in space and leads to global thermalization for $t\\rightarrow\\infty$. This underpins the importance of thermalizing collisions and endorses the standard approach of equilibrium statistical mechanics, describing a physical system in its steady state by a thermal Gibbs ensemble.

Die vorliegende Arbeit befasst sich mit dem Thema der Nichtgleichgewichts-Dispersionskräfte. Der Fokus liegt auf der kontroversen Casimir- bzw. Quantenreibung. Sie tritt auf, wenn sich zwei elektrisch neutrale Körper relativ zueinander bewegen. Vermittelt wird diese kontaktlose Reibungskraft über fluktuierende elektromagnetische (Quanten-) Felder und ist somit der Kategorie der fluktuationsinduzierten Phänome zuzuordnen, deren bekannte Beispiele die Van-der-Waals-Kraft und der Casimir-Effekt sind. Im Speziellen wurde die Situation eines mikroskopischen Objektes, welches sich mit einer festgelegten Geschwindigkeit und Höhe über eine makroskopische und flache Oberfläche beweget, untersucht. Um einen Zugang in das Themenfeld zu erlangen, wird eine kurze Einleitung in die Theorie der linearen Antwort und der Dynamik offener Systeme gegeben. Des Weiteren, werden unterschiedliche Modelle zur Beschreibung des mikroskopischen Objektes eingeführt und verschiedene Konfigurationen und Modelle bezüglich der makroskopischen Oberfläche berücksichtigt. Neben einem exakten, wenn auch komplexen, Integralausdruck werden diverse asymptotische Ausdrücke für verschiedene relevante Grenzfälle der kontaktlosen Reibung hergeleitet. Darüber hinaus, um die Asymptoten mit der exakten Lösung vergleichen zu können, wurde eine numerisch Auswertungsroutine des exakten Ausdrucks entwickelt und implementiert. Durch die Nutzung einer vollen Nichtgleichgewichtbeschreibung und das Einbeziehen sowohl der Rückwirkung des elektromagnetischen Feldes auf die Dynamik des mikroskopischen Objektes, als auch dessen Rotationsfreiheitsgrade, werden bestehende theoretische Beschreibungen erweitert. Abschließend wird ein Ausblick auf experimentelle Messungen der kontaktlosen Reibung gegeben. / The present thesis addresses the topic of nonequilibrium dispersion forces. The focus lies on the controversial Casimir or quantum friction, which occurs when two electrically neutral bodies move at a relative velocity with respect to each other. The noncontact friction force is mediated by the fluctuations of the (quantum) electromagnetic field and therefore belongs to the category of fluctuation-induced phenomena, whose prominent examples are the van der Waals force and the Casimir effect. Especially, the setup of a microscopic object moving at a fixed velocity and height above a flat macroscopic surface is investigated. To access this topic, a brief introduction into linear response and open system dynamics is given. Moreover, different models for the description of the microscopic object are introduced and various setups and models of the flat macroscopic surface are considered. Besides an exact but rather involved integral expression, several asymptotic expressions of the noncontact friction for different relevant limits are derived. Furthermore, in order to compare the asymptotic with the exact expression, a numerical approach for its evaluation was developed and implemented. Using a full nonequilibrium approach, which includes the backaction of the electromagnetic field onto the microscopic object’s dynamics, as well as its rotational degrees, existing theoretical descriptions are extended. Eventually, an outlook towards experimental measurements of the noncontact friction is given.

In the present work, we discuss two subjects related to the nonequilibrium dynamics of polymers or biological filaments adsorbed to two-dimensional substrates. <br><br> The first part is dedicated to thermally activated dynamics of polymers on structured substrates in the presence or absence of a driving force. The structured substrate is represented by double-well or periodic potentials. We consider both homogeneous and point driving forces. Point-like driving forces can be realized in single molecule manipulation by atomic force microscopy tips. Uniform driving forces can be generated by hydrodynamic flow or by electric fields for charged polymers. <br><br> In the second part, we consider collective filament motion in motility assays for motor proteins, where filaments glide over a motor-coated substrate. The model for the simulation of the filament dynamics contains interactive deformable filaments that move under the influence of forces from molecular motors and thermal noise. Motor tails are attached to the substrate and modeled as flexible polymers (entropic springs), motor heads perform a directed walk with a given force-velocity relation. We study the collective filament dynamics and pattern formation as a function of the motor and filament density, the force-velocity characteristics, the detachment rate of motor proteins and the filament interaction. In particular, the formation and statistics of filament patterns such as nematic ordering due to motor activity or clusters due to blocking effects are investigated. Our results are experimentally accessible and possible experimental realizations are discussed. / In der vorliegenden Arbeit behandeln wir zwei Probleme aus dem Gebiet der Nichtgleichgewichtsdynamik von Polymeren oder biologischen Filamenten, die an zweidimensionale Substrate adsorbieren. <br><br> Der erste Teil befasst sich mit der thermisch aktivierten Dynamik von Polymeren auf strukturierten Substraten in An- oder Abwesenheit einer treibenden Kraft. Das strukturierte Substrat wird durch Doppelmulden- oder periodische Potentiale dargestellt. Wir betrachten sowohl homogene treibende Kräfte als auch Punktkräfte. Punktkräfte können bei der Manipulation einzelner Moleküle mit die Spitze eines Rasterkraftmikroskops realisiert werden. Homogene Kräfte können durch einen hydrodynamischen Fluss oder ein elektrisches Feld im Falle geladener Polymere erzeugt werden. <br><br> Im zweiten Teil betrachten wir die kollektive Bewegung von Filamenten in Motility-Assays, in denen Filamente über ein mit molekularen Motoren überzogenes Substrat gleiten. Das Modell zur Simulation der Filamentdynamik beinhaltet wechselwirkende, deformierbare Filamente, die sich unter dem Einfluss von Kräften, die durch molekulare Motoren erzeugt werden, sowie thermischem Rauschen bewegen. Die Schaftdomänen der Motoren sind am Substrat angeheftet und werden als flexible Polymere (entropische Federn) modelliert. Die Kopfregionen der Motoren vollführen eine gerichtete Schrittbewegung mit einer gegebenen Kraft-Geschwindigkeitsbeziehung. Wir untersuchen die kollektive Filamentdynamik und die Ausbildung von Mustern als Funktion der Motor- und der Filamentdichte, der Kraft-Geschwindigkeitscharakteristik, der Ablöserate der Motorproteine und der Filamentwechselwirkung. Insbesondere wird die Bildung und die Statistik der Filamentmuster, wie etwa die nematische Anordnung aufgrund der Motoraktivität oder die Clusterbildung aufgrund von Blockadeeffekten, untersucht. Unsere Ergebnisse sind experimentell zugänglich und mögliche experimentelle Realisierungen werden diskutiert.

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In this thesis extensions to the formalism of endoreversible thermodynamics for multi-extensity fluxes and chemical reactions are introduced. These extensions make it possible to model a great variety of systems which could not be investigated with standard endoreversible thermodynamics. Multi-extensity fluxes are important when studying processes with matter fluxes or processes in which volume and entropy are exchanged between subsystems. For including reversible as well as irreversible chemical reaction processes a new type of subsystems is introduced - the so called reactor. It is similar to endoreversible engines, because the fluxes connected to it are balanced. The difference appears in the balance equations for particle numbers, which contain production or destruction terms, and in the possible entropy production in the reactor. Both extensions are then applied to an endoreversible fuel cell model. The chemical reactions in the anode and cathode of the fuel cell are included with the newly introduced subsystem -- the reactor. For the transport of the reactants and products as well as the proton transport through the electrolyte membrane, the multi-extensity fluxes are used. This fuel cell model is then used to calculate power output, efficiency and cell voltage of a fuel cell with irreversibilities in the proton and electron transport. It directly connects the pressure and temperature dependencies of the cell voltage with the dissipation due to membrane resistance. Additionally, beside the listed performance measures it is possible to quantify and localize the entropy production and dissipated heat with only this one model. / In dieser Arbeit erweitere ich den Formalismus der endoreversiblen Thermodynamik, um Flüsse mit mehr als einer extensiven Größe sowie chemische Reaktionsprozesse modellieren zu können. Mit Hilfe dieser Erweiterungen eröffnen sich zahlreiche neue Anwendungsmöglichkeiten für endoreversible Modelle. Flüsse mit mehreren extensiven Größen sind für die Betrachtung von Masseströmen ebenso nötig wie für Prozesse, bei denen sowohl Volumen als auch Entropie zwischen zwei Teilsystem ausgetauscht werden. Für sowohl reversibel wie auch irreversibel geführte chemische Reaktionsprozesse wird ein neues Teilsystem - der "Reaktor" - vorgestellt, welches sich ähnlich wie endoreversible Maschinen durch Bilanzgleichungen auszeichnet. Der Unterschied zu den Maschinen besteht in den Produktions- bzw. Vernichtungstermen in den Teilchenzahlbilanzen sowie der möglichen Entropieproduktion innerhalb des Reaktors. Beide Erweiterungen finden dann in einem endoreversiblen Modell einer Brennstoffzelle Anwendung. Dabei werden Flüsse mehrerer gekoppelter Extensitäten für den Zustrom von Wasserstoff und Sauerstoff sowie für den Protonentransport durch die Elektrolytmembran benötigt. Chemische Reaktionen treten in der Anode und Kathode der Brennstoffzelle auf. Diese werden mit dem neu eingeführten Teilsystem, dem Reaktor, eingebunden. Mit Hilfe des Modells werden dann Wirkungsgrad, Zellspannung und Leistung einer Brennstoffzelle unter Berücksichtigung der Partialdrücke der Substanzen, der Temperatur sowie der Dissipation beim Protonentransport berechnet. Dabei zeigt sich, dass experimentelle Daten für die Zellspannung sowohl qualitativ als auch näherungsweise quantitativ durch das Modell abgebildet werden können. Der Vorteil des endoreversiblen Modells liegt dabei in der Möglichkeit, mit nur einem Modell neben den genannten Kenngrößen auch die abgegebene Wärme sowie die Entropieproduktion zu quantifizieren und den einzelnen Teilprozessen zuzuordnen.

In der vorliegenden Arbeit wird die Dynamik geordneter modulierter Phasen außerhalb des thermischen Gleichgewichts untersucht. Der Schwerpunkt liegt auf einem zweidimensionalen, streifenbildenden System, genannt Modell B mit Coulomb-Wechselwirkung, welches aus einem geordneten Anfangszustand unter dem Einfluß eines Rauschterms relaxiert. Aus den mittels numerischer Simulationen gewonnenen Daten wird die lokale Orientierung der Streifen extrahiert und deren raum-zeitliche Korrelationsfunktionen berechnet. Wir beobachten eine langsame Dynamik und Alterungseffekte in der Zwei-Zeit-Autokorrelationsfunktion, welche einer Skalenform folgt, die aus kritischen Systemen bekannt ist. Dies geht einher mit dem Wachstum einer räumlichen Korrelationslänge senkrecht zu den Streifen. Zu sehr späten Zeiten klingt die zugehörige räumliche Korrelationsfunktion mit einem Potenzgesetz ab. Weiterhin wird der Einfluß der Systemgröße und verschiedener Seitenverhältnisse auf die Dynamik des Orientierungsfeldes studiert, wobei ein Wachstumsprozeß parallel zur Ausrichtung der Streifen identifiziert wird. Es zeigt sich, daß dieser Prozeß für die Nichtgleichgewichtsdynamik entscheidend ist. Zwei weitere Modelle für modulierte Phasen werden in ähnlicher Weise untersucht. Die Swift-Hohenberg-Gleichung in der Variante mit erhaltenem sowie nicht erhaltenem Ordnungsparameter zeigt ebenfalls Alterungseffekte in der Dynamik der Streifenorientierung. In einem System, welches zweidimensionale hexagonale Muster bildet, werden Alterungseffekte in der Autokorrelationsfunktion der Verschiebung beobachtet. Jedoch sättigt die zugehörige räumliche Korrelationslänge bei einem endlichen Wert, was auf eine Unterbrechung der Alterung hindeutet.

In this thesis extensions to the formalism of endoreversible thermodynamics for multi-extensity fluxes and chemical reactions are introduced. These extensions make it possible to model a great variety of systems which could not be investigated with standard endoreversible thermodynamics. Multi-extensity fluxes are important when studying processes with matter fluxes or processes in which volume and entropy are exchanged between subsystems. For including reversible as well as irreversible chemical reaction processes a new type of subsystems is introduced - the so called reactor. It is similar to endoreversible engines, because the fluxes connected to it are balanced. The difference appears in the balance equations for particle numbers, which contain production or destruction terms, and in the possible entropy production in the reactor. Both extensions are then applied to an endoreversible fuel cell model. The chemical reactions in the anode and cathode of the fuel cell are included with the newly introduced subsystem -- the reactor. For the transport of the reactants and products as well as the proton transport through the electrolyte membrane, the multi-extensity fluxes are used. This fuel cell model is then used to calculate power output, efficiency and cell voltage of a fuel cell with irreversibilities in the proton and electron transport. It directly connects the pressure and temperature dependencies of the cell voltage with the dissipation due to membrane resistance. Additionally, beside the listed performance measures it is possible to quantify and localize the entropy production and dissipated heat with only this one model. / In dieser Arbeit erweitere ich den Formalismus der endoreversiblen Thermodynamik, um Flüsse mit mehr als einer extensiven Größe sowie chemische Reaktionsprozesse modellieren zu können. Mit Hilfe dieser Erweiterungen eröffnen sich zahlreiche neue Anwendungsmöglichkeiten für endoreversible Modelle. Flüsse mit mehreren extensiven Größen sind für die Betrachtung von Masseströmen ebenso nötig wie für Prozesse, bei denen sowohl Volumen als auch Entropie zwischen zwei Teilsystem ausgetauscht werden. Für sowohl reversibel wie auch irreversibel geführte chemische Reaktionsprozesse wird ein neues Teilsystem - der "Reaktor" - vorgestellt, welches sich ähnlich wie endoreversible Maschinen durch Bilanzgleichungen auszeichnet. Der Unterschied zu den Maschinen besteht in den Produktions- bzw. Vernichtungstermen in den Teilchenzahlbilanzen sowie der möglichen Entropieproduktion innerhalb des Reaktors. Beide Erweiterungen finden dann in einem endoreversiblen Modell einer Brennstoffzelle Anwendung. Dabei werden Flüsse mehrerer gekoppelter Extensitäten für den Zustrom von Wasserstoff und Sauerstoff sowie für den Protonentransport durch die Elektrolytmembran benötigt. Chemische Reaktionen treten in der Anode und Kathode der Brennstoffzelle auf. Diese werden mit dem neu eingeführten Teilsystem, dem Reaktor, eingebunden. Mit Hilfe des Modells werden dann Wirkungsgrad, Zellspannung und Leistung einer Brennstoffzelle unter Berücksichtigung der Partialdrücke der Substanzen, der Temperatur sowie der Dissipation beim Protonentransport berechnet. Dabei zeigt sich, dass experimentelle Daten für die Zellspannung sowohl qualitativ als auch näherungsweise quantitativ durch das Modell abgebildet werden können. Der Vorteil des endoreversiblen Modells liegt dabei in der Möglichkeit, mit nur einem Modell neben den genannten Kenngrößen auch die abgegebene Wärme sowie die Entropieproduktion zu quantifizieren und den einzelnen Teilprozessen zuzuordnen.