Lattice simulations show that on T2 x R2 with twisted boundary conditions, the SU(2) vacuum is a Poissonian 2D gas of fractional instantons, with string tension proportional to the gas density and approaching the infinite-volume value.
Fractional topological charge in $SU(N)$ gauge theories without dynamical quarks
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abstract
In $SU(N)$ gauge theories without dynamical quarks, we discuss how configurations with fractional topological charge, $\sim 1/N$, can arise in the vacuum and dominate in the confining phase. They are not solutions of the classical equations of motion, but arise as quantum solutions of the effective Lagrangian. Their size is essentially fixed, on the order of the confinement scale. We give both a general mathematical analysis and illustrative solutions. Their presence can be measured through numerical simulations on the lattice using known methods. As they carry $\mathbb{Z}_N$ magnetic charge, the introduction of dynamical quarks significantly complicates their dynamics.
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A $T_2 \times R^2$ roadmap to Confinement in SU(2) Yang-Mills theory
Lattice simulations show that on T2 x R2 with twisted boundary conditions, the SU(2) vacuum is a Poissonian 2D gas of fractional instantons, with string tension proportional to the gas density and approaching the infinite-volume value.