Letting $Y_i \equiv - 2 \ln R_i$ and noting that $R_i \sim \text{Rayleigh}(1)$ you have the CDF:
$$\begin{equation} \begin{aligned}
F_Y(y) \equiv \mathbb{P}(Y_i \leqslant y)
&= \mathbb{P}(-Y_i/2 \geqslant -y/2) \\[6pt]
&= \mathbb{P}(e^{-Y_i/2} \geqslant e^{-y/2}) \\[6pt]
&= \mathbb{P}(R_i \geqslant e^{- y/2}) \\[6pt]
&= \exp \Big( -\frac{e^{- y}}{2} \Big). \\[6pt]
\end{aligned} \end{equation}$$
You therefore obtain the density function:
$$\begin{equation} \begin{aligned}
f_Y(y) = \frac{d F_Y}{dy} (y)
&= \frac{1}{2} \cdot \exp \Big( -y -\frac{e^{- y}}{2} \Big) \\[6pt]
&= \text{Gumbel}(y| \mu = \ln 2, \beta = 1). \\[6pt]
\end{aligned} \end{equation}$$
The mean and variance of this distribution are $\mathbb{E}(Y_i) = \ln 2 + \gamma$ and $\mathbb{V}(Y_i) = \pi^2/6$, where $\gamma$ denotes the Euler-Mascheroni constant. Your random variable $L_n$ can be written as an affine function of the sample mean of the random variables $Y_1,...,Y_n$ as follows:
$$L_n = n \Big( \ln 2 - \frac{1}{2} \cdot \bar{Y}_n \Big).$$
It follows that this random variable has mean:
$$\begin{equation} \begin{aligned}
\mathbb{E}(L_n)
&= n \Big( \ln 2 - \frac{1}{2} \cdot \mathbb{E}(\bar{Y}_n) \Big) \\[6pt]
&= n \Big( \ln 2 - \frac{1}{2} \cdot (\ln 2 + \gamma) \Big) \\[6pt]
&= \frac{\ln 2 - \gamma}{2} \cdot n, \\[6pt]
&\approx 0.05796576 \cdot n \\[6pt]
\end{aligned} \end{equation}$$
and variance:
$$\begin{equation} \begin{aligned}
\mathbb{V}(L_n)
&= \frac{n^2}{4} \cdot \mathbb{V}(\bar{Y}_n) \quad \quad \quad \quad \quad \ \ \\[6pt]
&= \frac{n^2}{4} \cdot \frac{\pi^2}{6n} \\[6pt]
&= \frac{\pi^2}{24} \cdot n \\[6pt]
&\approx 0.4112335 \cdot n. \\[6pt]
\end{aligned} \end{equation}$$
As whuber points out in the comments, the exact distribution of $L$ is a convolution of Gumbel distributions (see e.g., Nadarajah 2006). This exact distribution is complicated, but we can apply the classical central limit theorem to obtain an approximation using the normal distribution. For large values of $n$ we have:
$$L_n \overset{\text{Approx}}{\sim}
\text{N} \Big( \text{Mean} = \frac{\ln 2 - \gamma}{2} \cdot n, \text{Var} = \frac{\pi^2}{24} \cdot n \Big).$$