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The 2d Heisenberg model --- or 2d O(3) model --- is popular in condensed matter physics, and in particle physics as a toy model for QCD. Along with other analogies, it shares with 4d Yang-Mills theories, and with QCD, the property that the configurations are divided in topological sectors. In the lattice regularisation the topological charge $Q$ can still be defined such that $Q in mathbb{Z}$. It has generally been observed, however, that the topological susceptibility $chi_{rm t} = langle Q^2 rangle / V$ does not scale properly in the continuum limit, i.e. that the quantity $chi_{rm t} xi^2$ diverges for $xi to infty$ (where $xi$ is the correlation length in lattice units). Here we address the question whether or not this divergence persists after the application of the Gradient Flow.
The 2d O(3) model is widely used as a toy model for ferromagnetism and for Quantum Chromodynamics. With the latter it shares --- among other basic aspects --- the property that the continuum functional integral splits into topological sectors. Topolo
We study the impact of the Gradient Flow on the topology in various models of lattice field theory. The topological susceptibility $chi_{rm t}$ is measured directly, and by the slab method, which is based on the topological content of sub-volumes (sl
We consider the 2d XY Model with topological lattice actions, which are invariant against small deformations of the field configuration. These actions constrain the angle between neighbouring spins by an upper bound, or they explicitly suppress vorti
We study 2d U(1) gauge Higgs systems with a $theta$-term. For properly discretizing the topological charge as an integer we introduce a mixed group- and algebra-valued discretization (MGA scheme) for the gauge fields, such that the charge conjugation
Non-zero topological charge is prohibited in the chiral limit of gauge-fermion systems because any instanton would create a zero mode of the Dirac operator. On the lattice, however, the geometric $Q_text{geom}=langle F{tilde F}rangle /32pi^2$ definit