We say that a function $g\in C^{\infty}(\mathbb{R}^{n})$ is of Gevrey class $G^{\sigma}(\mathbb{R}^{n})$ if for each compact $K\subset\mathbb{R}^{n}$, there exist $C,R>0$ such that
$$\sup_{x\in K}\left|D^{\alpha}g(x)\right|\leq CR^{k}k^{\sigma k}, \quad \left|\alpha\right|=k$$
For $\sigma>1$, one can show that there exist compactly supported elements in $G^{\sigma}(\mathbb{R}^{n})$, which are not identically zero.
Exercise 2, Section 5 of M.E. Taylor, Partial Differential Equations I (2nd Edition) asks the reader to show that if $g\in G^{\sigma}(\mathbb{R}^{n})$, for $1<\sigma<2$, that the series
$$u(t,x):=\sum_{k=0}^{\infty}\dfrac{x^{2k}}{(2k)!}g^{(k)}(t), \qquad (t,x)\in\mathbb{R}\times\mathbb{R}$$
solves the heat equation with initial datum $u(t,0)=g(t)$. It then asks the reader to using a compactly supported Gevrey class function to find a nontrivial solution to the heat equation supported in the strip $a\leq t\leq b$. My issue is not with either of these tasks, but rather a comment made by the author concerning the growth of such a solution.
Question. At the bottom of pg. 245, the author remarks that for "fixed $t>0$, such solutions blow up too fast to belong to $\mathcal{S}'(\mathbb{R}^{n})$." How does one obtain a lower bound on the growth of $u(t,\cdot)$ to prove this?
My original idea was to suppose $u(t,\cdot)$ is a tempered distribution for some $t_{0}>0$ such that $u(t_{0},\cdot)\not\equiv 0$. If I could show that the map $t\mapsto u(t,\cdot)$ belonged to $C^{1}([t_{0},\infty),\mathcal{S}'(\mathbb{R}^{n}))$. We would then arrive at a contradiction by applying the uniqueness result for this class with initial datum $u(t_{0},\cdot)$, since $u(t,x)$ vanishes identically for all $t$ sufficiently large. An another idea is to somehow use the structure theorem for tempered distributions, but the problem here is that I do not know what $\left\{g^{(k)}(t)\right\}_{k}$ looks like for arbitrary $a\leq t\leq b$.
Motivation. I am so interested in this proving this property because it seems that examples of nonuniqueness for the heat equation Cauchy problem can exhibit different behavior for $t>0$ fixed.
EDIT: So Ian made a remark that made me think the author's claim is not true as stated. First, it's trivially not true for $t\notin [a,b]$ since $u(t,x)\equiv 0$. Second, couldn't we construct $g$ to be a nonzero constant on some small subinterval of $[a,b]$, in which case $u(t,x)$ is polynomial for some times?
EDIT2: I think the original question may have been unclear in that I do not know that for some $t>0$ fixed, $\left|u(t,x)\right|$ grows very rapidly (e.g. dominates $e^{c\left|x\right|^{2}}$ for some $c>0$) as $\left|x\right|\rightarrow\infty$; this is for what I am asking.