Superuniversality from disorder at two-dimensional topological phase transitions

(2020)

Authors:

Byungmin Kang, SA Parameswaran, Andrew C Potter, Romain Vasseur, Snir Gazit

Quantum Hall network models as Floquet topological insulators

Phys. Rev. Lett. 125 (2020) 086601-086601

Authors:

Andrew C Potter, Jt Chalker, Victor Gurarie

Abstract:

Network models for equilibrium integer quantum Hall (IQH) transitions are described by unitary scattering matrices, that can also be viewed as representing non-equilibrium Floquet systems. The resulting Floquet bands have zero Chern number, and are instead characterized by a chiral Floquet (CF) winding number. This begs the question: How can a model without Chern number describe IQH systems? We resolve this apparent paradox by showing that non-zero Chern number is recovered from the network model via the energy dependence of network model scattering parameters. This relationship shows that, despite their topologically distinct origins, IQH and CF topology-changing transitions share identical universal scaling properties.

Topological Defects on the Lattice: Dualities and Degeneracies

(2020)

Authors:

David Aasen, Paul Fendley, Roger SK Mong

Bacteria solve the problem of crowding by moving slowly

(2020)

Authors:

Oliver J Meacock, Amin Doostmohammadi, Kevin R Foster, Julia M Yeomans, William M Durham

Active inter-cellular forces in collective cell motility.

Journal of the Royal Society, Interface 17:169 (2020) 20200312-20200312

Authors:

Guanming Zhang, Romain Mueller, Amin Doostmohammadi, Julia M Yeomans

Abstract:

The collective behaviour of confluent cell sheets is strongly influenced both by polar forces, arising through cytoskeletal propulsion, and by active inter-cellular forces, which are mediated by interactions across cell-cell junctions. We use a phase-field model to explore the interplay between these two contributions and compare the dynamics of a cell sheet when the polarity of the cells aligns to (i) their main axis of elongation, (ii) their velocity and (iii) when the polarity direction executes a persistent random walk. In all three cases, we observe a sharp transition from a jammed state (where cell rearrangements are strongly suppressed) to a liquid state (where the cells can move freely relative to each other) when either the polar or the inter-cellular forces are increased. In addition, for case (ii) only, we observe an additional dynamical state, flocking (solid or liquid), where the majority of the cells move in the same direction. The flocking state is seen for strong polar forces, but is destroyed as the strength of the inter-cellular activity is increased.