activity
20132021
most citedTube algebras, excitations statistics and compactification in gauge models of topological phases

69 citations · 328 across the 12 of their papers we have counts for

collaborators

12 papers

hep-th2021★ 7 cited

Crossing with the circle in Dijkgraaf-Witten theory and applications to topological phases of matter

Alex Bullivant, Clement Delcamp

Given a fully extended topological quantum field theory, the 'crossing with the circle' conditions establish that the dimension, or categorification thereof, of the quantum invaria…

cond-mat.str-el2020★ 23 cited

Gapped boundaries and string-like excitations in (3+1)d gauge models of topological phases

Alex Bullivant, Clement Delcamp

We study lattice Hamiltonian realisations of (3+1)d Dijkgraaf-Witten theory with gapped boundaries. In addition to the bulk loop-like excitations, the Hamiltonian yields bulk dyoni…

cond-mat.str-el2019★ 16 cited

Excitations in strict 2-group higher gauge models of topological phases

Alex Bullivant, Clement Delcamp

We consider an exactly solvable model for topological phases in (3+1)d whose input data is a strict 2-group. This model, which has a higher gauge theory interpretation, provides a…

cond-mat.str-el2019★ 69 cited

Tube algebras, excitations statistics and compactification in gauge models of topological phases

Alex Bullivant, Clement Delcamp

We consider lattice Hamiltonian realizations of (+1)-dimensional Dijkgraaf-Witten theory. In (2+1)d, it is well-known that the Hamiltonian yields point-like excitations classifi…

math.QA2018★ 8 cited

Representations of the Necklace Braid Group: Topological and Combinatorial Approaches

Alex Bullivant, Andrew Kimball, Paul Martin +1

The necklace braid group is the motion group of the component necklace link in Euclidean . Here consists of …

math-ph2018★ 12 cited

Representations of the Loop Braid Group and Aharonov-Bohm like effects in discrete (3+1)-dimensional higher gauge theory

Alex Bullivant, João Faria Martins, Paul Martin

We show that representations of the loop braid group arise from Aharonov-Bohm like effects in finite 2-group (3+1)-dimensional topological higher gauge theory. For this we introduc…

cond-mat.str-el2017★ 35 cited

Twisted Quantum Double Model of Topological Orders with Boundaries

Alex Bullivant, Yuting Hu, Yidun Wan

We generalize the twisted quantum double model of topological orders in two dimensions to the case with boundaries by systematically constructing the boundary Hamiltonians. Given t…

math-ph2017★ 61 cited

Higher lattices, discrete two-dimensional holonomy and topological phases in (3+1) D with higher gauge symmetry

Alex Bullivant, Marcos Calcada, Zoltán Kádár +2

Higher gauge theory is a higher order version of gauge theory that makes possible the definition of 2-dimensional holonomy along surfaces embedded in a manifold where a gauge 2-con…

cond-mat.str-el2016★ 49 cited

Topological phases from higher gauge symmetry in 3+1D

Alex Bullivant, Marcos Calçada, Zoltán Kádár +2

We propose an exactly solvable Hamiltonian for topological phases in dimensions utilising ideas from higher lattice gauge theory, where the gauge symmetry is given by a finit…

cond-mat.str-el2015★ 16 cited

Entropic Topological Invariants in Three Dimensions

Alex Bullivant, Jiannis K. Pachos

We evaluate the entanglement entropy of exactly solvable Hamiltonians corresponding to general families of three-dimensional topological models. We show that the modification to th…

quant-ph2014★ 20 cited

Detection of Chern numbers and entanglement in topological two-species systems through subsystem winding numbers

James de Lisle, Suvabrata De, Emilio Alba +4

Topological invariants, such as the Chern number, characterise topological phases of matter. Here we provide a method to detect Chern numbers in systems with two distinct species o…

quant-ph2013★ 12 cited

Nonreversal and nonrepeating quantum walks

T. J. Proctor, K. E. Barr, B. Hanson +4

We introduce a variation of the discrete time quantum walk, the nonreversal quantum walk, which does not step back onto a position which it has just occupied. This allows us to sim…