The answer to this question Is spacetime symmetry a gauge symmetry? makes the following claim:
One may indeed view general relativity as a gauge theory whose gauge group is $GL(4,ℝ)$ and whose gauge field are the Christoffel symbols $Γ_$ viewed as a $GL(4,ℝ)$-valued field.
But does not provide a derivation of such. Can anyone provide a reference which gauges the general linear group, and derive general relativity from this approach? Or if possible even write the derivation as an answer.
All I can find in the literature are the Poincaré group $T(1,3) \times O(1,3)$ producing the Einstein-Cartan gauge theory, or the the $T(1,3) \times GL(4,ℝ)$ producing the metric-affine gauge theory, but nothing about the $GL(4,ℝ)$ group by itself?
Finally, the answer to this question To which extent is general relativity a gauge theory? appears to provide such an answer, but the author seems to backtrack in the comment section of his answer. Is the answer correct, or are there things missing to call it GR?