Georg-August-Universität Göttingen | Institut für Theoretische Physik
I study the physics of soft and disordered materials—glassy liquids, amorphous solids, polymers, and dense active matter—using large-scale simulations and theory, often in close collaboration with experiments. Across these areas, I am interested in how disorder, activity, and external driving shape structure, dynamics, and mechanical response in complex materials.
I examine how dense active materials—made of self-propelled particles—switch between jammed, solid-like states and flowing, fluidized states. In athermal active glasses [1–3], I probe how self-propulsion destabilizes stable amorphous solids, how thermal or processing history sets the activity threshold for fluidization, and how collective rearrangements and avalanches emerge near this transition. A key goal is to connect activity-induced fluidization with yielding in passive amorphous solids, especially through shared signatures of dynamic heterogeneity.
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With experimental and industrial partners, I link atomistic polymer structure to macroscopic mechanical response. Using non-affine lattice dynamics [1–3], we predict viscosity and viscoelastic moduli across many decades in frequency—from fast molecular vibrations to slow mechanical tests. This scale-bridging framework lets us interpret data on epoxy resins and glassy polymers directly in terms of microscopic structure and relaxation.
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Figure 3: Scale-bridging non-affine lattice dynamics (NALD) predicting storage ($G'$) and loss ($G''$) moduli across 20 frequency decades.
I study how glasses respond to temperature gradients and local heating, with implications for transport and processing. In a binary Lennard-Jones glass [1], I showed that heat and mass transport decouple near the glass transition, driving strong composition gradients (Soret effect) and nonlinear thermal responses. In ultrastable polydisperse glasses [2], I investigate how local heating nucleates a melting front, when melting proceeds via a propagating interface versus homogeneous melting, and what controls front dynamics.
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Figure 1: Thermal response and Soret coefficient $S_T$ behavior in supercooled glass-forming mixtures under thermal gradients.
I analyze how amorphous solids and complex liquids deform, flow, and fail. In size-polydisperse mixtures [1], I identified a rigid network of large particles coexisting with mobile small particles, and showed how this dynamic partitioning shapes bulk rheology. In confined Poiseuille flow [2], I clarified how stress gradients, boundaries, and thermalization alter local flow relative to bulk behavior. Recent work engineers controlled spatial inhomogeneities in glasses [3] to direct shear bands and failure pathways, linking microscopic stability contrasts to macroscopic failure.
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Figure 2: Microscopic boundary deformation, non-uniform velocity/stress profiles in Poiseuille flow, and emergent shear-banding failure pathways.
I study how dynamics slow and become heterogeneous near the glass transition, and how this depends on interactions, density, and temperature. In disparate-size mixtures [1], I showed that apparent transport of slow particles can be dominated by collective motion, and that removing center-of-mass drift reveals the true localization and glassy signatures. With collaborators [2–3], I use information-theoretic measures (negentropy) of displacement distributions to define entropic timescales of dynamic heterogeneity and to analyze “Brownian yet non-Gaussian” diffusion. In inverse-power-law glass-formers [4], I explore density–temperature scaling and crossover temperatures that unify thermodynamics and dynamics across densities.
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Figure 4: Intermittent particle transport and non-Gaussian displacement distributions $G_s(x,t)$ in supercooled liquids.