Perron's inversion formula states that if $F(x) = \sum_{n \leq x} f(n)$ and $F(s) = \sum_{n = 1}^{\infty} f(n) n^{-s}$, then
\[F(x) = \frac{1}{2\pi i} \int_{\sigma - i\infty}^{\sigma + i\infty} F(s) x^s \, \frac{ds}{s}\]
for $\sigma$ sufficiently large and $x > 1$ not an integer. We take $f(n) = \sum_{N(\mathfrak{a}) = n} \mu^2(\mathfrak{a}) N(\mathfrak{a})^{-\alpha}$. Then via multiplicativity,
\[F(s) = \prod_{\mathfrak{p}} \sum_{k = 0}^{\infty} \frac{\mu^2(\mathfrak{p}^k)}{N(\mathfrak{p}^k)^{\alpha}} \frac{1}{k N(\mathfrak{p}^k)^s} = \prod_{\mathfrak{p}} \left(1 + \frac{1}{N(\mathfrak{p})^{\alpha + s}}\right) = \prod_{\mathfrak{p}} \frac{1 - N(\mathfrak{p})^{-2(\alpha + s)}}{1 - N(\mathfrak{p})^{-(\alpha + s)}} = \frac{\zeta_K(\alpha + s)}{\zeta_K(2(\alpha + s))},\]
where $\zeta_K(s)$ denotes the Dedekind zeta function of the number field $K$. So
\[\sum_{N(\mathfrak{a}) \leq x} \frac{\mu^2(\mathfrak{a})}{N(\mathfrak{a})^{\alpha}} = \frac{1}{2\pi i} \int_{\sigma - i\infty}^{\sigma + i\infty} \frac{\zeta_K(\alpha + s)}{\zeta_K(2(\alpha + s))} x^s \, \frac{ds}{s}\]
for $\sigma > \max\{1 - \alpha,0\}$. The integrand has a pole at $s = 1 - \alpha$, at $s = 0$, and at $s = \frac{\rho}{2} - \alpha$ for any zero $\rho$ of $\zeta_K(s)$. By Cauchy's residue theorem, we may move the line of integration to the left, picking up residues along the way. These give the main terms for the left-hand side.
Suppose first that $\alpha \neq 1$. Then the residue of the integrand as $s = 1 - \alpha$ is
\[\lim_{s \to 1} (s - 1) \zeta_K(s) \times \frac{x^{1 - \alpha}}{(1 - \alpha) \zeta_K(2)}.\]
When $K = \mathbb{Q}$, the limit is $1$ and $\zeta(2) = \pi^2/6$. In general, the limit is given by the analytic class number formula, and $\zeta_K(2)$ may not have such a nice closed form.
Now suppose that $\alpha = 1$. Then the integrand has a double pole at $s = 0$, so this residue is a little more complicated to calculate. We write the integrand in the form
\[\frac{\zeta_K(s + 1)}{\zeta_K(2s + 2)} \frac{e^{s \log x}}{s}\]
and expand this as a Laurent series around $s = 0$. The main term (after writing $e^{s \log x} = 1 + s \log x + O_x(s^2)$) turns out to be
\[\lim_{s \to 1} (s - 1) \zeta_K(s) \times \frac{\log x}{\zeta_K(2)}.\]
There is also a constant term that is much more complicated (at least when $K$ is not $\mathbb{Q}$).