You have arrived at the limit $\displaystyle \lim_{x\to0}\ln\left(\frac{e}{(1+x)^\frac1x}\right)^\frac1x$ via the correct procedure. Note that it is of the indeterminate form $\vec1^{\vec\infty}$. You made a mistake in taking the limit of the base first ignoring the power which is not correct as both the base and the power are varying w.r.t $x$ simultaneously, i.e., as $x$ approaches $0$, the base gets closer and closer to $1$ but never equal to $1$ and the power gets arbitrarily large.
You can also see that if the same process is followed, any limit of this form would always be equal to $1$, which is a clear indication of this reasoning being faulty. For example:
$$\lim_{x\to0}\left(1+x\right)^\frac1x\ne\lim_{x\to0}1^\frac1x=1$$
The general procedure for solving limits of the form $\vec1^{\vec\infty}$ is
$$\lim_{x\to a}(f(x))^{g(x)}=e^{\displaystyle\lim_{x\to a}g(x)\ln f(x)}=e^{\displaystyle\lim_{x\to a}g(x)\left(f(x)-1-\frac{(f(x)-1)^2}2+\frac{(f(x)-1)^3}3\cdots\right)}$$
Usually, only the term involving $f(x)-1$ is required to solve the limit as the other terms evaluate to zero, but one should always check this.
Hence, the correct way to evaluate your limit would be
$$\require{cancel}\begin{align}\lim_{x\to0}\ln\left(\frac{e}{(1+x)^\frac1x}\right)^\frac1x&=\lim_{x\to0}\ln\left(\frac{(1+x)^\frac1x}e\right)^\frac{-1}x\\&=\lim_{x\to0}\ln\left(\frac{\cancel{e}\left(1-\frac{x}2+\frac{11x^2}{24}\cdots\right)}{\cancel{e}}\right)^\frac{-1}x\\&=-\lim_{x\to0}\frac{\left(-\frac{x}2+\frac{11x^2}{24}\cdots\right)-\overbrace{\frac{\left(-\frac{x}2+\frac{11x^2}{24}\cdots\right)^2}2\cdots}^{\text{lowest common power of }x\text{ is }2}+\overbrace{\frac{\left(-\frac{x}2+\frac{11x^2}{24}\cdots\right)^3}3\cdots}^{\text{lowest common power of }x\text{ is }3}}x\\&=\boxed{\frac12}\end{align}$$
The Taylor expansion of $(1+x)^\frac1x$ can be obtained by rewriting it as $e^{\frac{\ln(1+x)}x}$ and using the Taylor expansions of $\ln(1+x)$ and $e^x$.