In the "$\log$" expression, expand $\sin$ around $x_0=\frac{\pi}{6}$ using Taylor series, up to the second term, get
$$
\sin x \approx \frac{1}{2} + \frac{\sqrt{3}}{2}\left(x-\frac{\pi}{6}\right)
$$
so the expression $\log(1-2 \sin x)$ becomes $\log\left(\frac{\sqrt{3}}{2} \left(\frac{\pi}{6} - x\right)\right) = \log \frac{\sqrt{3}}{2} + \log \left(\frac{\pi}{6} - x\right)$. Now set $t=\frac{\pi}{6} - x$, rewrite $-\tan (-t_ = -\frac{\sin t}{\cos t}$ and expand $\sin t \sim t $ for $t \to 0^+$. This additional condition of convergence from the right allows rewriting the limit as
$$
\lim_{t \to 0^{+}} t \log t
$$
Now you can rewrite $t \log t = \frac{\log t }{\frac{1}{t}}$, and note that $\frac{1}{t} \to \infty$ and $\log t \to -\infty$. Set $\log t =v, \frac{1}{t} = e^{-v}$ for $v \to \infty$ and obviously
$$
\lim_{v \to \infty}\frac{v }{e^v} = 0
$$
All other terms converge to constants and are easy to compute. Keep in mind also that the original expression is $\varphi = e^{\log \varphi}$, so don't forget to take the exponent.
Result: no L'Hopital Rule used, only Taylor Series Expansion!