A Boundary conditions on the Euclidean Schwarzschild black hole

Afonso Campos
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This question is based on page 71 of Thomas Hartman's notes on Quantum Gravity and Black Holes (http://www.hartmanhep.net/topics2015/gravity-lectures.pdf).

The Euclidean Schwarzschild black hole

$$ds^{2} = \left(1-\frac{2M}{r}\right)d\tau^{2} + \frac{dr^{2}}{1-\frac{2M}{r}} + r^{2}d\Omega_{2}^{2}$$

is obtained from the Lorentzian Schwarzschild black hole via Wick rotation ##t \to -i\tau##.

Why does the fact that the coordinates must be regular at the origin imply that the angular coordinate must be identified as

$$\phi \sim \phi + 8\pi M?$$
 
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Afonso Campos said:
Why does the fact that the coordinates must be regular at the origin imply that the angular coordinate must be identified

It isn't the angular coordinate ##\phi## that's identified, it's the "angular" coordinate ##\tau##--the one that is derived via ##t \rightarrow - i \tau##. The "origin" is ##r = 2M##, and the solution has no interior, so the only range covered is ##r \ge 2M##.
 
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PeterDonis said:
It isn't the angular coordinate ##\phi## that's identified, it's the "angular" coordinate ##\tau##--the one that is derived via ##t \rightarrow - i \tau##. The "origin" is ##r = 2M##, and the solution has no interior, so the only range covered is ##r \ge 2M##.

How can we see explicitly that the range ##r < 2M## in the Lorentzian Schwarzschild black hole is not covered by the ##\tau## coordinate in the Euclidean Schwarzschild black hole?
 
Afonso Campos said:
How can we see explicitly that the range ##r < 2M## in the Lorentzian Schwarzschild black hole is not covered by the ττ\tau coordinate in the Euclidean Schwarzschild black hole?

The question doesn't make sense. To see whether the range ##r < 2M## is covered or not, you look at the behavior of the ##r## coordinate, not any other coordinate.
 
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