It reminds me of the digamma function. So, I'll try a non-trivial approach to calculate the given infinite sum. I hope you'll find it interesting.
We have the series formula for the digamma function.
$$\psi(z)=-\gamma+\sum_{n=0}^\infty\frac{z-1}{(n+1)(n+z)},\qquad z\notin\mathbb{Z}_{\leq0}\tag{1}$$
Substitute $z=\frac14$:
$$\psi\left(\frac14\right)=-\gamma-\sum_{n=0}^\infty\frac{3}{(n+1)(4n+1)}\implies\color{red}{\sum_{n=0}^\infty\frac{1}{(n+1)(4n+1)}=-\frac{\gamma+\psi(1/4)}{3}}\tag{2}$$
Similarly, $z=\frac34$:
$$\color{red}{\sum_{n=0}^\infty\frac{1}{(n+1)(4n+3)}=-\gamma-\psi(3/4)} \tag{3}$$
We know the digamma of $1/4$ from the digamma additive formula or Gauss' digamma theorem.
$$\psi\left(\frac14\right)=-\gamma - 3 \ln 2 - \dfrac \pi 2\tag{4}$$
Reflection formula for the digamma function:
$$\psi(1-z)-\psi(z)=\pi\cot\pi z\implies\psi\left(\frac34\right)-\psi\left(\frac14\right)=\pi\tag{5}$$
Now,
$$\begin{aligned}\sum_{n=0}^{\infty} \frac1{(4n+1)(4n+3)(n+1)}&=\frac12\cdot\sum_{n=0}^\infty\left(\frac{1}{(n+1)(4n+1)}-\frac{1}{(n+1)(4n+3)}\right)\\&=\frac{-\gamma-\psi(1/4)+3\gamma+3\psi(3/4)}{6}\\&=\frac{2\gamma+3\pi-2\gamma-6\ln2-\pi}{6}\\\color{red}{\sum_{n=0}^{\infty} \frac1{(4n+1)(4n+3)(n+1)}}&\color{red}{=\frac\pi3-\ln2\approx0.35405}
\end{aligned}$$
$$\begin{aligned}\sum_{n=0}^{\infty} \frac1{(4n+1)(4n+3)(n+1)}&=\sum_{n=0}^\infty\left(\frac{2}{3(4n+1)}-\frac{2}{4n+3}+\frac{1}{3(n+1)}\right)\\&=\frac43\sum_{n=0}^\infty\left(\frac{1}{4n+1}-\frac{1}{4n+3}\right)-\frac23\sum_{n=0}^\infty\left(\frac{1}{2(2n)+1}+\frac{1}{2(2n+1)+1}-\frac{1}{2(n+1)}\right)\\&=\frac43\cdot\frac\pi4-\frac23\sum_{n=0}^\infty\left(\frac{1}{2n+1}-\frac{1}{2n+2}\right)-\frac23\sum_{n=0}^\infty\left(\frac{1}{2(2n)+2}+\frac{1}{2(2n+1)+2}-\frac{1}{2n+2}\right)\\&=\frac\pi3-\frac23\cdot\ln2-\frac13\sum_{n=0}^\infty\left(\frac{1}{2n+1}-\frac{1}{2n+2}\right)\\&=\frac\pi3-\frac23\cdot\ln2-\frac13\ln2\\&=\frac\pi3-\ln2
\end{aligned}$$