[guided]We now prove the main case in the uniform continuity definition. Assume $C>0$, and fix an arbitrary tolerance $\varepsilon>0$. Uniform continuity requires a single number $\delta>0$ that works simultaneously for all pairs $x,y\in X$, so $\delta$ may depend on $\varepsilon$, $C$, and $\gamma$, but it must not depend on $x$ or $y$.
The Hölder estimate tells us that image distances are controlled by $C\,d_X(x,y)^\gamma$. To force this quantity to be smaller than $\varepsilon$, we choose $\delta$ so that $C\delta^\gamma=\varepsilon$. Thus define
\begin{align*}
\delta:=\left(\frac{\varepsilon}{C}\right)^{1/\gamma}.
\end{align*}
This number is positive because $\varepsilon>0$, $C>0$, and $\gamma>0$.
Now let $x,y\in X$ be any points satisfying $d_X(x,y)<\delta$. Distances in a [metric space](/page/Metric%20Space) are nonnegative, so $d_X(x,y)\in[0,\infty)$. Since $\gamma>0$, the power function $t\mapsto t^\gamma$ is increasing on $[0,\infty)$, and therefore
\begin{align*}
d_X(x,y)^\gamma<\delta^\gamma.
\end{align*}
By the definition of $\delta$,
\begin{align*}
\delta^\gamma=\frac{\varepsilon}{C}.
\end{align*}
Using the Hölder estimate for this pair $x,y$, we obtain
\begin{align*}
d_Y(f(x),f(y))\le C\,d_X(x,y)^\gamma<C\,\delta^\gamma=\varepsilon.
\end{align*}
This proves exactly what uniform continuity asks for: for the given $\varepsilon>0$, the single positive number $\delta=(\varepsilon/C)^{1/\gamma}$ works for every pair of points in $X$.[/guided]