Abstract:Abstract. We study the non-equilibrium relaxation of an elastic line described by the Edwards-Wilkinson equation. Although this model is the simplest representation of interface dynamics, we highlight that many (not though all) important aspects of the non-equilibrium relaxation of elastic manifolds are already present in such quadratic and clean systems. We analyze in detail the aging behaviour of several two-times averaged and fluctuating observables taking into account finite-size effects and the crossover … Show more
“…Quite some attention was paid recently to the ageing processes [14] that take place during the correlated growth regime [15,16,17,18,19,20,21,22,23]. Most of the studies focused on local quantities as for example the height-height correlation function, ‡ In the following we mostly use the language of growth processes, but due to the different physical situations described by the same Langevin equations our results have a broader range of applications.…”
Section: Introductionmentioning
confidence: 99%
“…the response of the height to a local perturbation, the two-time roughness or the twotime incoherent scattering function [15,16,17,18,19,20]. In [21] we discussed the correlation function of the squared width and the response of the squared width to a global perturbation.…”
Abstract. Growth processes and interface fluctuations can be studied through the properties of global quantities. We here discuss a global quantity that not only captures better the roughness of an interface than the widely studied surface width, but that is also directly conjugate to an experimentally accessible parameter, thereby allowing us to study in a consistent way the global response of the system to a global change of external conditions. Exploiting the full analyticity of the linear Edwards-Wilkinson and Mullins-Herring equations, we study in detail various two-time functions related to that quantity. This quantity fulfills the fluctuation-dissipation theorem when considering steady-state equilibrium fluctuations.
“…Quite some attention was paid recently to the ageing processes [14] that take place during the correlated growth regime [15,16,17,18,19,20,21,22,23]. Most of the studies focused on local quantities as for example the height-height correlation function, ‡ In the following we mostly use the language of growth processes, but due to the different physical situations described by the same Langevin equations our results have a broader range of applications.…”
Section: Introductionmentioning
confidence: 99%
“…the response of the height to a local perturbation, the two-time roughness or the twotime incoherent scattering function [15,16,17,18,19,20]. In [21] we discussed the correlation function of the squared width and the response of the squared width to a global perturbation.…”
Abstract. Growth processes and interface fluctuations can be studied through the properties of global quantities. We here discuss a global quantity that not only captures better the roughness of an interface than the widely studied surface width, but that is also directly conjugate to an experimentally accessible parameter, thereby allowing us to study in a consistent way the global response of the system to a global change of external conditions. Exploiting the full analyticity of the linear Edwards-Wilkinson and Mullins-Herring equations, we study in detail various two-time functions related to that quantity. This quantity fulfills the fluctuation-dissipation theorem when considering steady-state equilibrium fluctuations.
“…This is exactly solvable and one readily obtains the exact expressions for the height response and correlators, in the frame where h(t, r) = 0 [41,42] R(t, s; r) = δ h(t, r) δj(s, 0) j=0…”
Section: Tests Of Schrödinger-invariance In the Edwards-wilkinson Modelmentioning
Dynamical scaling arises naturally in various many-body systems far from equilibrium. After a short historical overview, the elements of possible extensions of dynamical scaling to a local scale-invariance will be introduced. Schrödinger-invariance, the most simple example of local scale-invariance, will be introduced as a dynamical symmetry in the Edwards-Wilkinson universality class of interface growth. The Lie algebra construction, its representations and the Bargman superselection rules will be combined with nonequilibrium Janssen-de Dominicis field-theory to produce explicit predictions for responses and correlators, which can be compared to the results of explicit model studies.At the next level, the study of non-stationary states requires to go over, from Schrö-dinger-invariance, to ageing-invariance. The ageing algebra admits new representations, which acts as dynamical symmetries on more general equations, and imply that each non-equilibrium scaling operator is characterised by two distinct, independent scaling dimensions. Tests of ageing-invariance are described, in the Glauber-Ising and spherical models of a phase-ordering ferromagnet and the Arcetri model of interface growth.
“…In the context of interacting vortices in a disordered environment an impressive list of twotime quantities has been discussed [6,14,15,[17][18][19][20][21]. Some of these quantities contain information about local thermal fluctuations, whereas others provide insight into the time evolution of the global structure of the flux line configuration.…”
We discuss the use of Langevin molecular dynamics in the investigation of the non-equilibrium properties of disordered vortex matter. Our special focus is set on values of system parameters that are realistic for disordered high-Tc superconductors such as YBCO. Using a discretized elastic line model, we study different aspects of vortices far from thermal equilibrium. On the one hand we investigate steady-state properties of driven magnetic flux lines in a disordered environment, namely the current-voltage characteristics, the gyration radius, and the pinning time statistics. On the other hand we study the complex relaxation processes and glassy-like dynamics that emerge in type-II superconductors due to the intricate competition between the long-range vortex-vortex repulsion and flux pinning due to randomly placed point defects. To this end we consider different types of sudden perturbations: temperature, magnetic field, and external current quenches.
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