Exact Results for 't Hooft Loops in Gauge Theories ... - Solvay Institutes

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Introduction Problem Definitions Method Solution Result We often take V = (Ψ, QΨ), where Ψ are the fermions of the theory. The path integral with action S t = S 0 + tQV and V = (Ψ, QΨ) localizes to configurations QΨ = 0 Vasily Pestun Localization for ’t Hooft operators on S 4 12/35
Introduction Problem Definitions Method Solution Result ∫ Z = X Localization summary e −S = ∑ ∫ e −S| Yα Z1−loop [N Yα ] α Y α⊂X where: Q is a fermionic symmetry Q 2 = R is a bosonic symmetry QS = 0 X = {Φ} is a space of fields Y α = {Φ|QΨ = 0} are components of the localization locus N Yα - normal bundle to Y α ⊂ X. Vasily Pestun Localization for ’t Hooft operators on S 4 13/35
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Exact Results for 't Hooft Loops in Gauge Theories ... - Solvay Institutes

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