Suppose $w\le 0$. Then
$$
\Pr(\ln y_1 \le w) = \Pr(y_1 \le e^w) = e^w. \tag 1
$$
That gives you the distribution of $\ln y_1$ on the interval $(-\infty,0]$. The derivative of $(1)$ with respect to $w$ is the density function on that interval, so that is $w\mapsto e^w$.
The density of the pair $(\ln y_1,\ln y_2)$ on the third quadrant $(-\infty,0]^2$ is therefore $(w_1,w_2) \mapsto e^{w_1} e^{w_2} = e^{w_1+w_2} \vphantom{\frac 1 1}$, and the probability measure in that quadrant is thus $e^{w_1+w_2}\,dw_1\,dw_2$.
Let us seek the cumulative distribution function of the difference $\ln y_1 - \ln y_2 = \ln \dfrac{y_1}{y_2}$. Since the distribution of $\ln y_1 - \ln y_2 = \ln \dfrac{y_1}{y_2}$ is the same as that of $\ln y_2 - \ln y_1 = \ln \dfrac{y_2}{y_1}$, we only need to do this in the case where $\ln y_1 - \ln y_2 = \ln \dfrac{y_1}{y_2}<0$. Suppose $u<0$ and we seek $\Pr(\ln y_1 - \ln y_2 \le u)$. We are in the region of the third quadrant where where $w_1 - w_2 \le u$.
So
- $w_2\le 0$, and
- For each fixed value of $w_2$ we have $w_1 \le w_2+u$.
Thus the probability is
$$
\int_{-\infty}^0 \left( \int_{-\infty}^{w_2+u} e^{w_1+w_2} \, dw_1 \right) \, dw_2 = \int_{-\infty}^0 e^{2w_2+u} \,dw_2 = e^u \int_{-\infty}^0 e^{2w_2}\, dw_2 = \frac 1 2 e^u.
$$
This is the cumulative distribution function on $(-\infty,0]$. Then density is its derivative, and it is its own derivative. By symmetry, therefore, the density on the whole real line is
$$
u \mapsto \left.\begin{cases} \frac 1 2 e^u & \text{if }u<0, \\[6pt] \frac 1 2 e^{-u} & \text{if }u>0, \end{cases} \right\} = \frac 1 2 e^{-|u|}.
$$