[step:Sum over index tuples and take the $2m$-th root to bound $\|S_J\|$]
Combining Steps 2 and 3,
\begin{align*}
\|(S_J^* S_J)^m\|_{\mathcal{L}(H)} \le \gamma(0) \sum_{j_1, k_1, \dots, j_m, k_m \in J} \gamma(j_1 - k_1)\,\gamma(k_1 - j_2)\,\gamma(j_2 - k_2) \cdots \gamma(j_m - k_m).
\end{align*}
We bound the right-hand sum by carefully tracking which index ranges over $J$ versus $\mathbb{Z}$. Substitute the difference variables $d_1 := j_1 - k_1$, $d_2 := k_1 - j_2$, $d_3 := j_2 - k_2$, $\dots$, $d_{2m-1} := j_m - k_m$, keeping $j_1$ as the free index that anchors the chain. The map
\begin{align*}
(j_1, k_1, j_2, k_2, \dots, j_m, k_m) \mapsto (j_1, d_1, d_2, \dots, d_{2m-1})
\end{align*}
is a bijection of $\mathbb{Z}^{2m}$ onto itself, and the integrand becomes $\gamma(d_1)\,\gamma(d_2)\cdots\gamma(d_{2m-1})$, independent of $j_1$.
In the original sum, $j_1$ ranges over $J$ (so the sum over $j_1$ contributes a factor $|J|$), and each of $k_1, j_2, k_2, \dots, k_m$ ranges over $J$, which translates into constraints on $d_1, d_2, \dots, d_{2m-1}$. Dropping these constraints by non-negativity (each $\gamma \ge 0$, so removing constraints can only increase the sum) and replacing the $d_i$-ranges by all of $\mathbb{Z}$:
\begin{align*}
\sum_{j_1, k_1, \dots, j_m, k_m \in J} \gamma(j_1 - k_1)\cdots\gamma(j_m - k_m) &\le \sum_{j_1 \in J}\sum_{d_1, \dots, d_{2m-1} \in \mathbb{Z}} \gamma(d_1)\,\gamma(d_2)\cdots\gamma(d_{2m-1}) \\
&= |J| \cdot \left(\sum_{d \in \mathbb{Z}} \gamma(d)\right)^{2m-1} = |J| \cdot A^{2m-1},
\end{align*}
where $|J|$ is the cardinality of $J$ and $A = \sum_{d \in \mathbb{Z}} \gamma(d)$ by hypothesis. Thus
\begin{align*}
\|(S_J^* S_J)^m\|_{\mathcal{L}(H)} \le \gamma(0) \cdot |J| \cdot A^{2m-1}.
\end{align*}
On the other hand, $S_J^* S_J$ is a positive self-adjoint bounded operator, so its operator norm equals its spectral radius and
\begin{align*}
\|S_J\|_{\mathcal{L}(H)}^{2m} = \|S_J^* S_J\|_{\mathcal{L}(H)}^m = \|(S_J^* S_J)^m\|_{\mathcal{L}(H)}.
\end{align*}
Combining,
\begin{align*}
\|S_J\|_{\mathcal{L}(H)}^{2m} \le \gamma(0) \cdot |J| \cdot A^{2m-1},
\end{align*}
hence
\begin{align*}
\|S_J\|_{\mathcal{L}(H)} \le A \cdot \big(\gamma(0) \cdot |J| / A\big)^{1/(2m)}.
\end{align*}
The factor $(\gamma(0)\,|J|/A)^{1/(2m)} \to 1$ as $m \to \infty$, so letting $m \to \infty$ gives
\begin{align*}
\|S_J\|_{\mathcal{L}(H)} \le A.
\end{align*}
This bound holds for every finite $J \subset \mathbb{Z}$, with constant $A$ independent of $J$.
[/step]