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Langevin dynamic for the 2D Yang-Mills measure
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We define a natural state space and Markov process associated to the stochastic Yang-Mills heat flow in two dimensions. To accomplish this we first introduce a space of distributional connections for which holonomies along sufficiently regular curves (Wilson loop observables) and the action of an associated group of gauge transformations are both well-defined and satisfy good continuity properties. The desired state space is obtained as the corresponding space of orbits under this group action and is shown to be a Polish space when equipped with a natural Hausdorff metric. To construct the Markov process we show that the stochastic Yang-Mills heat flow takes values in our space of connections and use the "DeTurck trick" of introducing a time dependent gauge transformation to show invariance, in law, of the solution under gauge transformations. Our main tool for solving for the Yang-Mills heat flow is the theory of regularity structures and along the way we also develop a "basis-free" framework for applying the theory of regularity structures in the context of vector-valued noise - this provides a conceptual framework for interpreting several previous constructions and we expect this framework to be of independent interest.
Forward citations
Cited by 3 Pith papers
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A PDE approach to the 2D Yang-Mills measure
The 2D Yang–Mills measure on the unit square admits a Coulomb-gauge representative in every Ω^1_β, β<1 — Gaussian-free-field regularity — with L^p moments growing like p^{(2+β)/2+δ}.
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Non-Gaussianity of invariant measures to SPDEs in Da Prato-Debussche regime
Invariant measures of parabolic SPDEs with odd polynomial nonlinearities in the Da Prato-Debussche regime are non-Gaussian, proved by stationary generator identities.
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Makeenko-Migdal equations for 2D Yang-Mills: from lattice to continuum
Suitable linear combinations of the discrete Makeenko-Migdal loop equations on (εZ)^2 converge to the continuum Makeenko-Migdal equation on the plane for U(N), SU(N), and SO(N).
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