[guided]The bias estimate comes from two ingredients: Taylor expansion and moment cancellation. The Taylor expansion turns the local smoothing error $f(x-hu)-f(x)$ into polynomial terms in $u$ plus a remainder. The order-$m$ kernel conditions then remove every polynomial term below order $m$.
Fix $x\in A$ and $u\in\operatorname{supp}K$. From the previous step, the entire line segment
\begin{align*}
\{x-thu:t\in[0,1]\}
\end{align*}
lies in $U$ for all sufficiently large $n$. Therefore the derivatives of $f$ needed for Taylor expansion are defined and bounded along this segment. We write $\mathcal L^1$ for one-dimensional Lebesgue measure on $[0,1]$, which is the measure used in the integral remainder term. Taylor expansion at $x$ to order $m-1$ in the vector $-hu$ gives
\begin{align*}
f(x-hu)
&=
\sum_{|\alpha|\le m-1}
\frac{D^\alpha f(x)}{\alpha!}(-hu)^\alpha
+
m\sum_{|\alpha|=m}
\frac{(-hu)^\alpha}{\alpha!}
\int_0^1
(1-t)^{m-1}D^\alpha f(x-thu)\,d\mathcal{L}^1(t).
\end{align*}
Here $\alpha=(\alpha_1,\dots,\alpha_d)$ is a multi-index, $\alpha!:=\alpha_1!\cdots\alpha_d!$, and $u^\alpha:=u_1^{\alpha_1}\cdots u_d^{\alpha_d}$.
Now multiply this identity by $K(u)$ and integrate over $\mathbb{R}^d$ with respect to $\mathcal{L}^d(u)$. The constant term gives
\begin{align*}
f(x)\int_{\mathbb{R}^d}K(u)\,d\mathcal{L}^d(u)=f(x),
\end{align*}
because the kernel has total mass $1$. If $1\le |\alpha|\le m-1$, the corresponding Taylor term contributes
\begin{align*}
\frac{D^\alpha f(x)(-h)^{|\alpha|}}{\alpha!}
\int_{\mathbb{R}^d}u^\alpha K(u)\,d\mathcal{L}^d(u)=0,
\end{align*}
because the integer moments of $K$ vanish through order $m-1$. Therefore the only contribution to $\mathbb{E}[\hat f_h(x)]-f(x)$ is the Taylor remainder:
\begin{align*}
b_h(x)
&=
m\sum_{|\alpha|=m}
\frac{(-h)^m}{\alpha!}
\int_{\mathbb{R}^d}
u^\alpha K(u)
\int_0^1
(1-t)^{m-1}D^\alpha f(x-thu)\,d\mathcal{L}^1(t)
\,d\mathcal{L}^d(u).
\end{align*}
To bound this uniformly in $x$, define
\begin{align*}
M_\alpha:=\sup_{y\in U}|D^\alpha f(y)|
\end{align*}
for each $\alpha$ with $|\alpha|=m$. These quantities are finite by the boundedness hypothesis on the order-$m$ derivatives. Taking absolute values yields
\begin{align*}
|b_h(x)|
&\le
m h^m
\sum_{|\alpha|=m}
\frac{M_\alpha}{\alpha!}
\int_{\mathbb{R}^d}
|u^\alpha|\,|K(u)|
\int_0^1
(1-t)^{m-1}\,d\mathcal{L}^1(t)
\,d\mathcal{L}^d(u).
\end{align*}
The one-dimensional integral is
\begin{align*}
\int_0^1(1-t)^{m-1}\,d\mathcal{L}^1(t)=\frac{1}{m},
\end{align*}
so
\begin{align*}
|b_h(x)|
&\le
h^m
\sum_{|\alpha|=m}
\frac{M_\alpha}{\alpha!}
\int_{\mathbb{R}^d}|u^\alpha|\,|K(u)|\,d\mathcal{L}^d(u).
\end{align*}
The right-hand side is independent of $x$. It is finite because $K\in L^1(\mathcal L^d)$ and $\operatorname{supp}K\subset\overline B(0,R)$ imply
\begin{align*}
\int_{\mathbb{R}^d}|u^\alpha|\,|K(u)|\,d\mathcal{L}^d(u)
\le
R^m\int_{\mathbb{R}^d}|K(u)|\,d\mathcal{L}^d(u)
<\infty
\end{align*}
for every $\alpha$ with $|\alpha|=m$. Thus, with
\begin{align*}
C_{\mathrm{bias}}
:=
\sum_{|\alpha|=m}
\frac{M_\alpha}{\alpha!}
\int_{\mathbb{R}^d}|u^\alpha|\,|K(u)|\,d\mathcal{L}^d(u),
\end{align*}
we have
\begin{align*}
\|b_h\|_{\infty,A}\le C_{\mathrm{bias}}h^m.
\end{align*}
This proves the deterministic bias estimate $\|b_h\|_{\infty,A}=O(h^m)$.[/guided]