Excitations in the higher lattice gauge theory model for topological phases II: the 2+1d case

Physical Review B American Physical Society 108:24 (2023) 245133

Authors:

Joe Huxford, Steven Simon

Abstract:

In this work, the second paper of this series, we study the (2+1)-dimensional version of a Hamiltonian model for topological phases based on higher-lattice gauge theory. We construct the ribbon operators that produce the pointlike excitations. These ribbon operators are used to find the braiding properties and topological charge carried by the pointlike excitations. The model also hosts looplike excitations, which are produced by membrane operators. By considering a change of basis, we show that, in certain cases, some looplike excitations represent domain walls between patches corresponding to different symmetry-related ground states, and we find this symmetry. We also map the higher-lattice gauge theory Hamiltonian to the symmetry-enriched string-net model for symmetry-enriched topological phases described by Heinrich, Burnell, Fidkowski, and Levin [Phys. Rev. B 94, 235136 (2016)], again in a subset of cases.

Energy minimization of paired composite fermion wave functions in the spherical geometry

Physical Review B American Physical Society 108:24 (2023) 245128

Authors:

Greg Henderson, Gunnar Moller, Steven Simon

Abstract:

We perform the energy minimization of the paired composite fermion (CF) wave functions, proposed by Möller and Simon (MS) [Phys. Rev. B 77, 075319 (2008)] and extended by Yutushui and Mross (YM) [Phys. Rev. B 102, 195153 (2020)], where the energy is minimized by varying the CF pairing function, in the case of an approximate model of the Coulomb interaction in the second Landau level for pairing channels ℓ = −1, 3, 1, which are expected to be in the Pfaffian, anti-Pfaffian, and particle-hole symmetric (PH) Pfaffian phases, respectively. It is found that the energy of the ℓ = −1 MS wave function can be reduced substantially below that of the Moore-Read wave function at small system sizes; however, in the ℓ = 3 case the energy cannot be reduced much below that of the YM trial wave function. Nonetheless, both our optimized and unoptimized wave functions with ℓ = −1, 3 extrapolate to roughly the same energy per particle in the thermodynamic limit. For the ℓ = 1 case, the optimization makes no qualitative difference and these PH-Pfaffian wave functions are still energetically unfavorable. The effective CF pairing is analyzed in the resulting wave functions, where the effective pairing for the ℓ = −1, 3 channels is found to be well approximated by a weak-pairing BCS ansatz and the ℓ = 1 wave functions show no sign of emergent CF pairing.

Nonequilibrium phenomena in driven and active Coulomb field theories

Physica A Statistical Mechanics and its Applications Elsevier 631 (2023) 127947

Authors:

Mahdisoltani Saeed, Golestanian Ramin

Scaling behaviour and control of nuclear wrinkling

Nature Physics Springer Nature 19:12 (2023) 1927-1935

Authors:

Jonathan A Jackson, Nicolas Romeo, Alexander Mietke, Keaton J Burns, Jan F Totz, Adam C Martin, Jörn Dunkel, Jasmin Imran Alsous

Shape-tension coupling produces nematic order in an epithelium vertex model

Physical Review Letters American Physical Society 131:22 (2023) 228301

Authors:

Jan Rozman, Julia M Yeomans, Rastko Sknepnek

Abstract:

We study the vertex model for epithelial tissue mechanics extended to include coupling between the cell shapes and tensions in cell-cell junctions. This coupling represents an active force which drives the system out of equilibrium and leads to the formation of nematic order interspersed with prominent, long-lived +1 defects. The defects in the nematic ordering are coupled to the shape of the cell tiling, affecting cell areas and coordinations. This intricate interplay between cell shape, size, and coordination provides a possible mechanism by which tissues could spontaneously develop long-range polarity through local mechanical forces without resorting to long-range chemical patterning.