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 />
Technical details:<br />
Convenient coord<strong>in</strong>ates<br />
S 4 = S 1 × B 3<br />
where B 3 is a 3d solid ball with a boundary B 3 : ∑ 3<br />
i=1 x2 i < 1<br />
and S 1 is a circle τ<br />
The round S 4 metric is<br />
ds 2 =<br />
dx 2 i<br />
(1 + x 2 ) 2 + (1 − x2 ) 2<br />
(1 + x 2 ) 2 dτ 2<br />
B 3 -flat rescaled metric<br />
ds 2 = dx 2 i + (1 − x 2 ) 2 dτ 2<br />
The ’t <strong>Hooft</strong> loop is the S 1 fiber at x i = 0.<br />
The North pole, the first fixed po<strong>in</strong>t of Q 2 is x = (0, 0, 1)<br />
he South pole, the second fixed of Q 2 is x = (0, 0, −1)<br />
Vasily Pestun Localization <strong>for</strong> ’t <strong>Hooft</strong> operators on S 4 17/35