ﻻ يوجد ملخص باللغة العربية
We investigate the behavior of higher-form symmetries at various quantum phase transitions. We consider discrete 1-form symmetries, which can be either part of the generalized concept categorical symmetry (labelled as $tilde{Z}_N^{(1)}$) introduced recently, or an explicit $Z_N^{(1)}$ 1-form symmetry. We demonstrate that for many quantum phase transitions involving a $Z_N^{(1)}$ or $tilde{Z}_N^{(1)}$ symmetry, the following expectation value $ langle left( log O_mathcal{C} right)^2 rangle$ takes the form $langle left( log O_mathcal{C} right)^2 rangle sim - frac{A}{epsilon} P+ b log P $, where $O_mathcal{C}$ is an operator defined associated with loop $mathcal{C}$ (or its interior $mathcal{A}$), which reduces to the Wilson loop operator for cases with an explicit $Z_N^{(1)}$ 1-form symmetry. $P$ is the perimeter of $mathcal{C}$, and the $b log P$ term arises from the sharp corners of the loop $mathcal{C}$, which is consistent with recent numerics on a particular example. $b$ is a universal microscopic-independent number, which in (2+1)d is related to the universal conductivity at the quantum phase transition. $b$ can be computed exactly for certain transitions using the dualities between (2+1)d conformal field theories developed in recent years. We also compute the strange correlator of $O_mathcal{C}$: $S_{mathcal{C}} = langle 0 | O_mathcal{C} | 1 rangle / langle 0 | 1 rangle$ where $|0rangle$ and $|1rangle$ are many-body states with different topological nature.
In recent years, new phases of matter that are beyond the Landau paradigm of symmetry breaking are mountaining, and to catch up with this fast development, new notions of global symmetry are introduced. Among them, the higher-form symmetry, whose sym
We study higher-form symmetries in 5d quantum field theories, whose charged operators include extended operators such as Wilson line and t Hooft operators. We outline criteria for the existence of higher-form symmetries both from a field theory point
We investigate the effects of quenched randomness on topological quantum phase transitions in strongly interacting two-dimensional systems. We focus first on transitions driven by the condensation of a subset of fractionalized quasiparticles (`anyons
We study the concept of categorical symmetry introduced recently, which in the most basic sense refers to a pair of dual symmetries, such as the Ising symmetries of the $1d$ quantum Ising model and its self-dual counterpart. In this manuscript we stu
Theories of photoinduced phase transitions have developed along with the progress in experimental studies, especially concerning their nonlinear characters and transition dynamics. At an early stage, paths from photoinduced local structural distortio