In general, the Taylor Series is the last thing you should be looking at.
In fact, the Taylor Series was not looked at; they calculated the Laurent Series. The point is that:
$$\operatorname{e}^y = 1 + y + \frac{1}{2}y^2 + \frac{1}{3!}y^3 + \cdots $$
Replacing $y$ with $2/x$ gives:
\begin{array}{ccc}
\operatorname{e}^{2/x} &=& 1 + \frac{2}{x} + \frac{1}{2}\left(\frac{2}{x}\right)^2 + \frac{1}{3!}\left(\frac{2}{x}\right)^3 + \cdots \\ \\
&=& 1 + \frac{2}{x} + \frac{2}{x^2} + \frac{4}{3x^3} + \cdots
\end{array}
The actual function under consideration was $x\operatorname{e}^{2/x}+1$ and so we have:
\begin{array}{ccc}
x\operatorname{e}^{2/x}+1 &=& x\left(1 + \frac{2}{x} + \frac{2}{x^2} + \frac{4}{3x^3} + \cdots\right) + 1 \\ \\
&=& \left(x + 2 + \frac{2}{x} + \frac{4}{3x^2} + \cdots\right) + 1 \\ \\
&=& x + 3 + \frac{2}{x} + \frac{4}{3x^2} + \cdots
\end{array}
The point here is that as $x$ gets larger, anything with an $x$ in the denominator gets smaller: $1/x \to 0$ as $x \to \infty$. So as $x \to \infty$ we have $2/x \to 0$, $4/3x^2 \to 0$, etc. All of "the tail" gets smaller and smaller very quickly. The only terms that we are left with are the $x$ and the $3$.
There is a general definition for an asymptote. They don't even need to be lines.