Consider the system $$ x'=\mu x-y-x\sqrt{x^2+y^2}, \, y'=x+\mu y-y\sqrt{x^2+y^2} $$ I am working on that show that (1) as $\mu>0$, there exists a unique stable limit cycle around $(0,0)$ (2) as $\mu\le 0$, there is no limit cycle around $(0,0)$. And draw the phase portraits for these two cases. Also, draw the bifurcation diagram.
My proof: note that the only critical point is $(0,0)$ and $$Df(0,\mu) =\begin{pmatrix} \mu & -1 \\ 1 & \mu \end{pmatrix}$$
Then $(0,0)$ is stable if $\mu<0$ and $(0,0)$ is unstable if $\mu>0$.
For $\mu=0$, consider the polar coordinate: $$ r'=r(\mu-r), \theta'=1 $$
So $\mu=0$, $(0,0)$ is a stable focus.
For $\mu>0$, there is a limit cycle $(\mu \cos t, \mu \sin t)$. [** Question: But how to say that is unique?**]
Since as $\mu<0$, $(0,0)$ is unstable, then there is no limit cycle.
The phase portraits:
The bifurcation diagram: The red line is $r=\mu$.


I guess you can study everything is polar coordinate, as the system in that case is reduced to 1-d. You have
$$ \dot{r} = r(m-r) =: f_\mu(r) $$
with fixed points $r=0$ and $r= \mu$. The stability is controlled by by
$$ f'_\mu(r):=\frac{d}{dr}f_\mu(r) =\mu - 2r $$. Going by cases:
$$ f'_\mu(0) = \mu <0 $$
So there is no limit cycle, and the origin attracts all trajectories.
$$ f'_\mu(r=0) = \mu >0 $$ Meaning that $r=0$ is repelling. And
$$ f'_\mu(r=\mu) = -\mu < 0 $$ Which means that $r=\mu$ is repelling. This proves the uniqueness of the limit cycle (and actually, also its existence), as all the trajectories on the plane are attracted to it (both from the 'inside' and from the 'outside' the closed orbit). A stable periodic orbit does not necessarily have this property. Thus, proving that 0 is unstable is not enough.
It might be nice to know that $f(r) = x(\mu-x)$ is the famous logistic equation, that can be solved analytically.