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

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

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

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Introduction Problem Def<strong>in</strong>itions Method Solution Result<br />

Result<br />

Includ<strong>in</strong>g the po<strong>in</strong>t <strong>in</strong>stanton contributions at the north and<br />

south poles, we f<strong>in</strong>ally get the result<br />

〈<br />

ZT (B)<br />

〉<br />

=<br />

∫<br />

da<br />

∣ Z north(ia − B ∣ ∣∣∣<br />

2<br />

2 ) · Z equator (ia)<br />

where Z north is Nekrasov’s partition function <strong>in</strong>clud<strong>in</strong>g classical,<br />

(slightly modified) one-loop and the <strong>in</strong>stanton factors.<br />

Our gauge theory result agrees with the computation <strong>in</strong> the<br />

Liouville/Toda theories by [Alday-Gaiotto-Tajikawa] conjecture<br />

per<strong>for</strong>med by [Drukker,Gomis,Okuda,Teschner’09] and [Alday,<br />

Gaiotto, Gukov, Tachikawa, Verl<strong>in</strong>de’09] and [Gomis,Floch’10] .<br />

Vasily Pestun Localization <strong>for</strong> ’t <strong>Hooft</strong> operators on S 4 32/35

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