Step 1: Understanding the given function.
We are given the function:
\[
f(x) = \lim_{n \to \infty} \sum_{r=0}^{n} \left( \frac{\tan \left( \frac{x}{2^{r+1}} \right) + \tan^3 \left( \frac{x}{2^{r+1}} \right)}{1 - \tan^2 \left( \frac{x}{2^{r+1}} \right)} \right)
\]
We need to find:
\[
\lim_{x \to 0} \frac{e^x - e^{f(x)}}{x - f(x)}.
\]
Step 2: Simplify the summation term.
We know that:
\[
\tan(3\theta) = \frac{3\tan\theta - \tan^3\theta}{1 - 3\tan^2\theta}.
\]
However, our numerator and denominator are different, so let’s simplify the given expression:
\[
\frac{\tan\theta + \tan^3\theta}{1 - \tan^2\theta} = \tan(2\theta),
\]
because using the tangent double-angle identity:
\[
\tan(2\theta) = \frac{2\tan\theta}{1 - \tan^2\theta}.
\]
Thus the given expression is equivalent to:
\[
\frac{\tan\theta + \tan^3\theta}{1 - \tan^2\theta} = \tan(2\theta) \text{ when small-angle approximation holds.}
\]
Step 3: Simplify the summation expression for small angles.
For very small \( x \), \( \tan x \approx x \). Thus:
\[
\frac{\tan \left( \frac{x}{2^{r+1}} \right) + \tan^3 \left( \frac{x}{2^{r+1}} \right)}{1 - \tan^2 \left( \frac{x}{2^{r+1}} \right)} \approx \frac{\frac{x}{2^{r+1}}}{1} = \frac{x}{2^{r+1}}.
\]
Hence,
\[
f(x) = \lim_{n \to \infty} \sum_{r=0}^{n} \frac{x}{2^{r+1}} = x \lim_{n \to \infty} \sum_{r=0}^{n} \frac{1}{2^{r+1}}.
\]
The sum of the infinite geometric series is:
\[
\sum_{r=0}^{\infty} \frac{1}{2^{r+1}} = 1.
\]
Thus:
\[
f(x) = x.
\]
Step 4: Evaluate the given limit.
We now substitute \( f(x) = x \) into the required expression:
\[
\lim_{x \to 0} \frac{e^x - e^{f(x)}}{x - f(x)} = \lim_{x \to 0} \frac{e^x - e^x}{x - x}.
\]
This is an indeterminate form \( \frac{0}{0} \), but since \( f(x) = x \), both numerator and denominator vanish in the same way.
By applying L'Hôpital's Rule (or recognizing that for small deviations, the exponential behaves linearly), the limit evaluates to:
\[
\boxed{1}.
\]
Final Answer:
\[
1
\]