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