Laplace transform
Function
todo
Discussion
Action on monomials
In this article we use $\beta=\frac{1}{T}$.
todo: clean this $\beta$ vs. $T$ Thing up. Maybe drop $T$ altogether.
With $u=\beta\,E=E/T\implies dE=Tdu$ and the definition of the Gamma function, we find
$\int_0^\infty \left(\frac{1}{n!}E^n\right){\mathrm e}^{-E/T}dE = T^{n+1} \frac{1}{n!} \int_0^\infty u^{(n+1)-1}{\mathrm e}^{-u}du = T^{n+1},$
so that
$L[f](\beta):=\int_0^\infty f(E){\mathrm e}^{-\beta E}dE$
is the integral transform realization of
$\dfrac{1}{n!}E^n\mapsto \frac{1}{\beta^{n+1}}$
Hence, for analytic functions
$f(E)=\sum_{n=0}^\infty \frac{1}{n!} f^{(n)}(0) E^n$,
you get
$L[f](\beta) = \sum_{n=0}^\infty f^{(n)}(0) \frac{1}{\beta^{n+1}}=\dfrac{1}{\beta}\sum_{n=0}^\infty f^{(n)}(0) \left(\frac{1}{\beta}\right)^n$
or, in Terms of $T:=\frac{1}{\beta}$
$L[f](T) = T\sum_{n=0}^\infty f^{(n)}(0)\, T^n$
Note how this means $f(E)=1$ is connected to $\dfrac{1}{\beta}=T$ and $f(E)=\exp(E)$ is connected to $-\dfrac{1}{1-\beta}=\dfrac{1}{\beta}\dfrac{1}{1-\frac{1}{\beta}}=T\dfrac{1}{1-T}$.