Electric-field-induced shape transition of nematic tactoids

Physical Review E American Physical Society 96 (2017) 022706

Authors:

Luuk Metselaar, I Dozov, K Antonova, E Belamie, P Davidson, Julia M Yeomans, Amin Doostmohammadi

Abstract:

The occurrence of new textures of liquid crystals is an important factor in tuning their optical and photonics properties. Here, we show, both experimentally and by numerical computation, that under an electric field chitin tactoids (i.e. nematic droplets) can stretch to aspect ratios of more than 15, leading to a transition from a spindle-like to a cigar-like shape. We argue that the large extensions occur because the elastic contribution to the free energy is dominated by the anchoring. We demonstrate that the elongation involves hydrodynamic flow and is reversible, the tactoids return to their original shapes upon removing the field.

Exact solution for the quench dynamics of a nested integrable system

Journal of Statistical Mechanics Theory and Experiment IOP Publishing 2017:8 (2017) 083103

Authors:

Márton Mestyán, Bruno Bertini, Lorenzo Piroli, Pasquale Calabrese

High‐throughput cell mechanical phenotyping for label‐free titration assays of cytoskeletal modifications

Cytoskeleton Wiley 74:8 (2017) 283-296

Authors:

Stefan Golfier, Philipp Rosendahl, Alexander Mietke, Maik Herbig, Jochen Guck, Oliver Otto

Quantum entanglement growth under random unitary dynamics

Physical Review X American Physical Society 7:3 (2017) 031016

Authors:

Adam Nahum, J Ruhman, S Vijay, J Haah

Abstract:

Characterizing how entanglement grows with time in a many-body system, for example, after a quantum quench, is a key problem in nonequilibrium quantum physics. We study this problem for the case of random unitary dynamics, representing either Hamiltonian evolution with time-dependent noise or evolution by a random quantum circuit. Our results reveal a universal structure behind noisy entanglement growth, and also provide simple new heuristics for the “entanglement tsunami” in Hamiltonian systems without noise. In 1D, we show that noise causes the entanglement entropy across a cut to grow according to the celebrated Kardar-Parisi-Zhang (KPZ) equation. The mean entanglement grows linearly in time, while fluctuations grow like ðtimeÞ 1 = 3 and are spatially correlated over a distance ∝ ðtimeÞ 2 = 3 . We derive KPZ universal behavior in three complementary ways, by mapping random entanglement growth to (i) a stochastic model of a growing surface, (ii) a “minimal cut” picture, reminiscent of the Ryu-Takayanagi formula in holography, and (iii) a hydrodynamic problem involving the dynamical spreading of operators. We demonstrate KPZ universality in 1D numerically using simulations of random unitary circuits. Importantly, the leading-order time dependence of the entropy is deterministic even in the presence of noise, allowing us to propose a simple coarse grained minimal cut picture for the entanglement growth of generic Hamiltonians, even without noise, in arbitrary dimensionality. We clarify the meaning of the “velocity” of entanglement growth in the 1D entanglement tsunami. We show that in higher dimensions, noisy entanglement evolution maps to the well-studied problem of pinning of a membrane or domain wall by disorder.

Spinon decay in the spin-1/2 Heisenberg chain with weak next nearest neighbour exchange

Journal of Physics A: Mathematical and Theoretical IOP Publishing 50:33 (2017) 334002

Authors:

Stefan Groha, Fabian Essler

Abstract:

Integrable models support elementary excitations with infinite lifetimes. In the spin-1/2 Heisenberg chain these are known as spinons. We consider the stability of spinons when a weak integrability breaking perturbation is added to the Heisenberg chain in a magnetic field. We focus on the case where the perturbation is a next nearest neighbour exchange interaction. We calculate the spinon decay rate in leading order in perturbation theory using methods of integrability and identify the dominant decay channels. The decay rate is found to be small, which indicates that spinons remain well-defined excitations even though integrability is broken.