We study the spectral properties of the stiffness matrices coming from the approximation of a $d$-dimensional second order elliptic differential problem by the $\mathbb Q_{\boldsymbol p}$ Lagrangian finite element method (FEM); here, ${\boldsymbol p}=(p_1,\ldots,p_d)$ and $p_j$ represents the polynomial approximation degree in the $j$th direction. After presenting a construction of these matrices, we investigate the conditioning and the spectral distribution in the Weyl sense, and we determine the so-called (spectral) symbol describing the asymptotic spectrum. We also study the properties of the symbol, which turns out to be a $d$-variate function taking values in the space of $N({\boldsymbol p})\times N({\boldsymbol p})$ Hermitian matrices, where $N({\boldsymbol p})=\prod_{j=1}^d p_j$. Unlike the stiffness matrices coming from the ${\boldsymbol p}$-degree B-spline isogeometric analysis approximation of the same differential problem, where a unique $d$-variate real-valued function describes all the spectrum, here the spectrum is described by $N({\boldsymbol p})$ different functions, i.e., the $N({\boldsymbol p})$ eigenvalues of the symbol, which are well-separated, far away, and exponentially diverging with respect to ${\boldsymbol p}$ and $d$. This very involved picture provides an explanation of: (a) the difficulties encountered in designing robust solvers, with convergence speed independent of the matrix size, of the approximation parameters ${\boldsymbol p}$, and of the dimensionality $d$; (b) the convergence deterioration of known iterative methods, already observed in practice for moderate ${\boldsymbol p}$ and $d$. (The PDF has been changed.)
Read full abstract