For $s \in (0,1)$, we consider the spectral fractional Laplacian \begin{align} (-\Delta)^{-s}u = \sum_{k=1}^{\infty}\lambda_k^{-s}(\phi_k,u)_{L^2}\phi_k \end{align} where \begin{align*} \begin{cases} -\Delta\phi_k = \lambda_k\phi_k &\mbox{in }\Omega,\\ \partial_\nu \phi_k = 0 &\mbox{on }\partial\Omega,\qquad k\geq 1. \end{cases} \end{align*} Then, for $\alpha \in (0,1)$, we define the space \begin{align*} H^\alpha(\Omega) = \{ u\in L^2(\Omega):~ \nabla (-\Delta)^{(\alpha-1)/2}u\in L^2(\Omega) \}, \end{align*} and the space \begin{align*} \tilde H^\alpha(\Omega) = \{ u\in L^2(\Omega)~:~ \sum_{j=1}^\infty \lambda_j^\alpha|(\phi_j,u)_{L^2(\Omega)}|^2<\infty\} \end{align*}
Questions:
Are these two spaces equivalent?
Do Sobolev embeddings, Poincaré inequalities, etc hold in them? If yes, where can I find a reference?
UPDATE. After the discussion in the comments, let me reformulate the question in a way that avoids (hopefully) some issues:
Let $(\phi_k)\subset L^2(\Omega)$ be a complete orthonormal system for $\mathcal L^2(\Omega)= \{ u\in L^2(\Omega):\int_\Omega u d x =0 \}$ composed of eigenfunctions of $-\Delta$ with homogeneous Neumann boundary conditions with eigenvalues $(\lambda_k)\subset (0,\infty)$.
Q1: Is \begin{align} (-\Delta)^{-s}u = \sum_{k=1}^{\infty}\lambda_k^{-s}(\phi_k,u)_{L^2}\phi_k \end{align} well-defined?
Q2: Define \begin{align*} \mathcal H^\alpha(\Omega) = \{ u\in \mathcal L^2(\Omega):~ \nabla (-\Delta)^{(\alpha-1)/2}u\in L^2(\Omega) \}, \end{align*} and the space \begin{align*} \tilde{\mathcal H}^\alpha(\Omega) = \{ u\in \mathcal L^2(\Omega)~:~ \sum_{j=1}^\infty \lambda_j^\alpha|(\phi_j,u)_{L^2(\Omega)}|^2<\infty\} \end{align*} Are these spaces well-defined and are they equivalent?