We have the Maclaurin-Taylor series expansion for the exponential function
$$e^x=\sum_{k=0}^\infty \frac{x^k}{k!} = 1 + x{} + \frac{x^2}{2!}+\frac{x^3}{3!}+\frac{x^4}{4!}+\frac{x^5}{5!}+...$$
If we differentiate implicitly, then
$$\frac{d(e^x)}{dx} =\frac{d}{dx}\sum_{k=0}^\infty \frac{x^k}{k!} = \frac{d}{dx} \bigg( 1 + x{} + \frac{x^2}{2!}+\frac{x^3}{3!}+\frac{x^4}{4!}+\frac{x^5}{5!}+... \bigg)$$
And we know by the linearity of the differential operator, i.e. $(f(x)+g(x))' = f'(x)+g'(x)$, we get
$$\frac{d(e^x)}{dx} =\sum_{k=0}^\infty \frac{d}{dx} \bigg( \frac{x^k}{k!} \bigg) = \sum_{k=0}^\infty \frac{1}{k!} \frac{d}{dx} \bigg( x^k \bigg)$$
applying the constant rule for derivatives, i.e. $(cf(x))=cf'(x)$ and $(c)'=0$ ($c$ constant). Furthermore, knowing the power rule, $(x^n)' = nx^{n-1}$ and using the recursivity of the factorial, i.e. $k! = k(k-1)!$, for $k > 0$,
$$\frac{d(e^x)}{dx} = \sum_{k=0}^\infty \frac{1}{k!} kx^{k-1} = \frac{1}{0!} 0 \cdot x^{0-1} + \sum_{k=1}^\infty \frac{1}{k!} kx^{k-1}$$
So
$$\frac{d(e^x)}{dx}=\sum_{k=1}^\infty \frac{1}{k(k-1)!} kx^{k-1} = \sum_{k=1}^\infty \frac{1}{(k-1)!} x^{k-1}$$
We will now proceed a change of index $k-1=k'$,
$$\frac{d(e^x)}{dx}=\sum_{k'=0}^\infty \frac{1}{k'!} x^{k'}=\sum_{k=0}^\infty \frac{x^{k}}{k!} $$
(since the terms of the sum are infinite)
Which is exactly $e^x$. Thus,
$$\frac{d}{dx} \bigg( e^x \bigg) = e^x$$