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Stochastic quantisation of Yang–Mills–Higgs in 3D

Ajay Chandra, Ilya Chevyrev, Martin Hairer, Hao Shen

2024Inventiones mathematicae23 citationsDOIOpen Access PDF

Abstract

Abstract We define a state space and a Markov process associated to the stochastic quantisation equation of Yang–Mills–Higgs (YMH) theories. The state space $\mathcal{S}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>S</mml:mi> </mml:math> is a nonlinear metric space of distributions, elements of which can be used as initial conditions for the (deterministic and stochastic) YMH flow with good continuity properties. Using gauge covariance of the deterministic YMH flow, we extend gauge equivalence ∼ to $\mathcal{S}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>S</mml:mi> </mml:math> and thus define a quotient space of “gauge orbits” $\mathfrak {O}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> </mml:math> . We use the theory of regularity structures to prove local in time solutions to the renormalised stochastic YMH flow. Moreover, by leveraging symmetry arguments in the small noise limit, we show that there is a unique choice of renormalisation counterterms such that these solutions are gauge covariant in law. This allows us to define a canonical Markov process on $\mathfrak {O}$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>O</mml:mi> </mml:math> (up to a potential finite time blow-up) associated to the stochastic YMH flow.

Topics & Concepts

MathematicsHiggs bosonStochastic quantizationApplied mathematicsAlgebra over a fieldPure mathematicsQuantumParticle physicsPhysicsPath integral formulationQuantum mechanicsMathematical Analysis and Transform MethodsBlack Holes and Theoretical PhysicsParticle physics theoretical and experimental studies