Notice $$T_n = \left(\frac{n!}{\prod_{\ell=1}^n 2\ell+1}\right)^2 =
\left(\frac{(1)_n}{(\frac32)_n}\right)^2 4^{-n}$$
where $\displaystyle\;(\alpha)_n = \prod_{\ell=0}^{n-1}(\alpha+\ell)\;$ is the rising factorials.
Since $0 < (1)_n < (\frac32)_n$, we have $|T_n| < 4^{-n}$ and the series converges absolutely.
Aside from a constant, the sum at hand has the form of a
generalized hypergeometric function.
$$
\sum_{n=1}^\infty T_n = \sum_{n=1}^\infty \frac{(1)_n(1)_n(1)_n}{n!(\frac32)_n(\frac32)_n} 4^{-n} = {}_3F_2\left( 1, 1, 1 ; \frac32, \frac32; \frac14 \right) - 1$$
Throwing following command HypergeometricPFQ[{1,1,1},{3/2,3/2},1/4] - 1 to wolfram alpha, we can evaluate the series with high precision
$$\sum_{n=1}^\infty T_n \approx 0.132968794417890464087477244396881449530734610666632988747\ldots$$
Unluckily, there doesn't seem to be other simpler closed form for this number.