# Differential operators with arbitrary functions?

By Taylor expansion, one has $$f(x+t) = \sum_{k=0}^∞ \frac{D^k}{k!}f(x)([x+t]-x)^k = \sum_{k=0}^∞ \frac{(Dt)^k}{k!}f(x)$$ and hence one could say $e^{Dt}$ is translation by $t$. But this isn't a "differential operator", not by Wikipedia's definition. My questions: in what sense is this a truly convergent "differential operator"? I have seen similar ones e.g. replace $D$ with the Laplacian; what does this mean, and why do we care about them?

• Lagrange wrote $g(s+t)=\exp(t\frac{d}{dt})g(s)$ in his Nouvelle espece de calcul, 1772. This is a formal way to denote what in the modern science is related to the field of $C_0$ semigroups. Here is a nice book.
– A.Γ.
Oct 25, 2015 at 22:40
• @A.G. Thanks :) If you expand a little on that I would be more than happy to accept that as an answer. Oct 26, 2015 at 8:58

1. Starting with the familiar $$e^t=\sum_{n=0}^\infty\frac{t^n}{n!}.$$ We know that $e^{t+s}=e^te^s$.
2. For a matrix $A\in M_{n\times n}$ $$e^{At}=\sum_{n=0}^\infty\frac{A^nt^n}{n!}.$$ What we know is the same $e^{A(t+s)}=e^{At}e^{As}$ and that it is the fundamental solution to $\dot x=Ax$. If we denote the fundamental solution by $T(t)=e^{At}$, the former property can be written as $$T(t+s)=T(t)T(s),\qquad T(0)=I.$$ Thus, the mapping $T(t)=e^{At}$ defines a $C_0$ semigroup. Here, you can interpret $T(t)$ as the shift along the trajectories of $\dot x=Ax$.
3. For an abstract one-parametric $C_0$ semigroup on a Banach space $X$ we define the generator $A$ as (in the derivative manner) $$Ax=\lim_{t\to 0^+}\frac{1}{t}(T(t)-I)x,\qquad\forall x\in X.$$ If a $C_0$ semigroup is uniformly continuous, which means that $t\mapsto T(t)$ is continuos wrt the uniform operator topology, then there exists a bounded operator $A$ such that $T(t)=e^{At}$. It means that
4. Consider a left translation semigroup $$T(t)f(s)=f(s+t).$$ It can be shown to be not uniformly continuous, unfortunately, but it is still quite nice in the sense that it is strongly continuous semigroup (i.e. wrt the strong operator topology) on $L^p$, $1\le p<\infty$. For strongly continuous semigroup it is still possible to define the generator $A$, however it is no longer bounded, but a closed operator. For the left shift semigroup the generator is the differential operator $$Af(s)=f'(s)$$ defined on the Sobolev space (the space with the graph metric) $W^{1,p}$. So $A=D$, and it is tempting to write $T(t)=e^{Dt}$, but it is no longer possible, since the semigroup is not uniformly bounded. However, there are certain similarities with $e^{Dt}$ as we have seen above.