Theorem 18.34.6.F82E8E685FEA For every $k\geq 1$,
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18.34.7
\begin{equation} \partial _ t^ k k_{v_ t,x} =\sum _{\alpha \in \Lambda _ k}\frac{k!}{\alpha !} \mathcal T_{t,\alpha _ p}\cdots \mathcal T_{t,\alpha _1}k_{v_ t,x}. \end{equation}
Suppose moreover that $s\geq 1$, that $J\Subset I$ is a compact interval, and that constants $A,R>0$ satisfy
\[ \sup _{t\in J}\| \partial _ t^ jv_ t\| _\infty \leq AR^ j(j!)^ s\qquad (j\geq 1). \]
Then there are constants $C,L>0$, depending only on the fixed data and on $m,r,J,A,R,s$, such that
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18.34.8
\begin{equation} \sup _{t\in J} \left(\| \partial _ t^ kB_{v_ t}\| _\infty +\| \partial _ t^ k\beta _{v_ t}\| _{\mathrm{TV}}\right) \leq CL^ k(k!)^ s\qquad (k\geq 0). \end{equation}
Thus the kernel and the kernel measure are of Gevrey class $s$ in the parameter.
Proof.
The derivative formula. By proposition 18.34.5, $k_{v_ t,x}$ depends smoothly on $t$, for any fixed norm on $V_ m$. Fix a real parameter $t$ and set
\[ H(a)=P_{v_ t}\bigl (\mathrm{e}^{-m(v_{t+a}-v_ t)}\, \cdot \, \bigr )|_{V_ m}. \]
Then $H(0)=I$, $H^{(j)}(0)=-\mathcal T_{t,j}$ by Faà di Bruno's formula, and $k_{v_{t+a},x}=H(a)^{-1}k_{v_ t,x}$ as in the proof of proposition 18.34.5. Since $H(a)-I=O(|a|)$, truncating the Neumann series of $H(a)^{-1}$ after $k$ powers leaves a remainder $O(|a|^{k+1})$. Expanding the truncated series to order $k$ in $a$ gives (18.34.7), with its ordered products and coefficients $k!/\alpha !$. Only a finite Taylor jet of the smooth curve is used.
Gevrey bounds. For nonnegative integers $n_\ell $ with $\sum \ell n_\ell =j$,
\[ \prod _{\ell =1}^ j(\ell !)^{(s-1)n_\ell } \leq (j!)^{s-1}. \]
The sum $\sum \prod _\ell (n_\ell !)^{-1}$ over these tuples is the coefficient of $z^ j$ in $\exp (z/(1-z))$, and evaluation at $z=1/2$ shows that it is at most $\mathrm{e}\, 2^ j$. Together with the assumed bounds this gives
\[ \sup _{t\in J}\| \mathcal B_ j(-mv_ t)\| _\infty \leq L_0^ j(j!)^ s \]
for some $L_0>0$. Since $P_{v_ t}$ is a contraction, each ordered product in (18.34.7) has operator norm at most $L_0^ k(\alpha !)^ s$. There are $2^{k-1}$ compositions of $k$, and $\alpha !\leq k!$. Since $v_ t$ is uniformly bounded for $t\in J$, the norms $\| \cdot \| _{m,v_ t,\nu }$ are uniformly equivalent, and the evaluations and Riesz vectors are bounded uniformly on $J\times X$. Hence the $t$-derivatives of the unweighted diagonal $x\mapsto \ell _ x(k_{v_ t,x})$ are bounded in $C(X)$ by $C(2L_0)^ k(k!)^ s$. The factor $\mathrm{e}^{-mv_ t}$ satisfies bounds of the same Gevrey order, by the estimate for $\mathcal B_ j(-mv_ t)$. Leibniz's formula and $j!(k-j)!\leq k!$ then give (18.34.8) for $B_{v_ t}$, and the bounded linear map $B\mapsto (r!/m^ r)B\nu $ gives the bound in total variation.
$\square$
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