Assume $$ h \circ E_{-2}= E_2 \circ h,$$ where $h$ is the semi cojnugacy. Applying the degree both sides you get $deg(h)=0$. Let $H$ denote the lifting of h such that $$H(0) \in [0,1), $$ then,
$$H(x+1)=H(x) $$
i.e H is periodic. Moreover, lifting both sides of the above equation, we easily obtain that
$2H(x) $ and $H(2-2x)$ are both lifing of the same map. A well known result implies that
$$2H(x)= H(2-2x) + c$$
where c is an integer.
Periodicity implies
$$2H(0)=H(2)+c= H(0)+c$$
and the only possibile solution to this is $c=0$ and $H(0)=0$.
Applying weiestrass theorem and periodicity we get that H attains a global maximum and minimum and the first is nonnegative, the second is nonpositive. Since the global extrema of $2H(x) , H(2-2x) $ must coincide, we get their extrema are zero. In details:
let $M,m$ be resp. the maximum and minimum of H. Assume $M>0$. Then, since $c=0$, for proper $y$:
$$2M=2H(y)=H(2-2y)>M, $$
contradicting the fact that M is a maximum. This implies $M=0.$
Now assume $m<0$,say $m=-q$, with $q$ strictly positive. Again, for proper $y$:
$$-2q=2H(y)=H(2-2y)<-q.$$
This implies $c=0$.
Then, H is constant, contradiction.
This is generalizable for different $k$, but not so trivially , though.