[guided]We now convert the Hölder control of $f$ into the exact power needed for the estimate of $g\circ f$. The defining estimate for $f$ says that, for the already chosen points $x,x'\in X$,
\begin{align*}
d_Y(f(x),f(x'))\le C_f d_X(x,x')^\alpha.
\end{align*}
The estimate for $g$ contains the quantity $d_Y(f(x),f(x'))^\beta$, so we need to raise this inequality to the power $\beta$. This is legitimate because both sides are nonnegative: $d_Y(f(x),f(x'))\ge 0$ and $d_X(x,x')^\alpha\ge 0$ by the metric axioms and by $0<\alpha\le 1$, while $C_f\ge 0$ by hypothesis. Also, since $0<\beta\le 1$, the map $\varphi:[0,\infty)\to[0,\infty)$ given by $\varphi(t)=t^\beta$ is increasing on $[0,\infty)$. Hence applying $\varphi$ to both sides preserves the inequality:
\begin{align*}
d_Y(f(x),f(x'))^\beta\le \left(C_f d_X(x,x')^\alpha\right)^\beta.
\end{align*}
Finally, because $C_f$ and $d_X(x,x')^\alpha$ are nonnegative real numbers, the exponent laws apply without sign ambiguity:
\begin{align*}
\left(C_f d_X(x,x')^\alpha\right)^\beta=C_f^\beta d_X(x,x')^{\alpha\beta}.
\end{align*}
Thus
\begin{align*}
d_Y(f(x),f(x'))^\beta\le C_f^\beta d_X(x,x')^{\alpha\beta}.
\end{align*}[/guided]