Maps $\mathrm{B} G \to \mathcal{X}$ correspond to an object of $\mathcal{X}(k)$ along with a $G$-action. Indeed, the map $* \to \mathrm{B} G \to \mathcal{X}$ selects an object $x$ and for each test scheme $T$ we get a natural map,
$$ \{ T \text{-torsors} \} \to \mathcal{X}(T) $$
so that the trivial torsor maps to $x$. This is determined by the induced $G$-action on $x$ since, after a cover, each torsor becomes trivial and the gluing maps pass to gluing data for an object of $\mathcal{X}$.
Maps $[E/G] \to \mathcal{X}$ correspond to "$G$-equivariant objects over $E$" meaning the data of $x \in \mathcal{X}(E)$ with a $G$-action in $\mathcal{X}$ which is compatible with the $G$-action on $E$ along the functor $\mathcal{X} \to \mathrm{Sch}_k$.
First, $\mathbb{G}_m$-equivariant coherent sheaves are exactly coherent sheaves with a $\mathbb{Z}$-grading. In some sense, this is an incarnation of the fact that the actions of tori split up into a weight space decomposition. In the affine case, this is very clear, we need a comultiplication map,
$$ M \to M \otimes k[t, t^{-1}] $$
which gives a decomposition of $M$ into the sum over $M_n = \{ m \mid m \mapsto m \otimes t^n\}$. The (co)associativity of the action shows that this is a $\mathbb{Z}$-grading.
Now we need to consider $\mathbb{G}_m$-equivariant sheaves over $\mathbb{A}^1$. This means a coherent sheaf $\mathcal{F}$ on $X \times \mathbb{A}^1$ flat over $\mathbb{A}^1$ with a $\mathbb{G}_m$-action over $\mathbb{A}^1$. We get an actual sheaf $\mathcal{F}|_1$ taking the fiber over $1 \in \mathbb{A}^1$ which is what "$f(1)$" should mean. Consider this situation affine-locally. We have a $A[t]$-module $M$ which is $\mathbb{Z}$-graded compatibly with the $\mathbb{Z}$-grading on $A[t]$ (although this grading on $A[t]$ is trivial in negative degrees this need not be true of $M$ e.g. $M = A[t, t^{-1}]$. We think of $f(1) = M/(t-1)$ as the underlying object which messes up the grading but preserves the decreasing filtration
$$ M_{\ge n} = \bigoplus\limits_{k \ge n} M_n $$
because the action of $(t-1)$ preserves this filtration but not preserve the ascending filtration. Therefore, we get a $\mathbb{Z}$-filtered $A$-module $M/(t-1)$.
This is analogous to the "dynamical description of Parabolic, Levi, and Cartan subgroups" where we are asking for the limit of a $\mathbb{G}_m$-parametrized sheaf "as $t \to 0$". This is the sort of condition that gives a parabolic so it may not be so surprising that it recovers filtered objects.