The hp-version interior penalty discontinuous Galerkin (IPDG) method of Han and Zhang (BIT Numerical Mathematics 63, 2023) for the quad-curl equation curl4u\mathrm{curl}^4 u and the associated quad-curl eigenvalue problem comes with a priori error bounds that are optimal in the mesh size hh but provably suboptimal in the polynomial degree pp: the analysis loses 3 orders in pp on nonconforming simplicial meshes and 2 orders on conforming ones. The open problem is to complete the convergence theory of this method by determining the sharp polynomial-degree dependence of its a priori error bounds — the DG norm for the source problem, and the eigenvalue and eigenfunction errors — whether that sharp exponent is the optimal one or instead reflects a genuine residual loss. The paper itself also notes, within the same theory, that the pp-independence on general simplicial meshes of the reconstruction-based constant behind the hp discrete compactness argument is currently verified only for H(curl)H(\mathrm{curl})-conforming rectangular elements, and it indicates but does not carry out the extension of the hp-error analysis to general polygonal (2D) and polyhedral (3D) meshes; these are related context for the central pp-optimality objective rather than separate completion requirements.

Background

For a vector field uu on a simply connected polyhedral domain Ω⊂R3\Omega \subset \mathbb{R}^3, the curl operator ∇×u\nabla \times u generalizes to the fourth-order quad-curl operator curl4\mathrm{curl}^4. The quad-curl problem seeks uu with ∇×∇×∇×∇×u=f\nabla \times \nabla \times \nabla \times \nabla \times u = f together with a divergence-free constraint ∇⋅u=0\nabla \cdot u = 0 and suitable boundary conditions. It arises in the inverse electromagnetic scattering transmission eigenvalue problem and in the time discretization of resistive magnetohydrodynamics, and its eigenvalue problem curl4u=λu\mathrm{curl}^4 u = \lambda u governs so-called Maxwell transmission eigenvalues used to derive nondestructive testing criteria. Because the curl operator has a large kernel (gradient fields), the problem is not elliptic in the standard sense, and discretizations need special care: conforming methods require finite elements with continuous tangential curls across mesh faces (H(curl2)H(\mathrm{curl}^2)-conforming elements), while mixed and discontinuous formulations introduce auxiliary variables or penalty terms. Interior penalty discontinuous Galerkin (IPDG) methods use fully discontinuous piecewise-polynomial spaces and add mesh-face penalty terms, scaled by the polynomial degree pp, to weakly enforce continuity of the field and its curls. The hp version refines both the mesh size hh and the polynomial degree pp, and an analysis is called pp-optimal when the polynomial-degree exponent in the error bound matches the best-approximation exponent of the underlying space. For second-order elliptic problems, hp-optimal DG bounds are known (e.g., Stamm and Wihler, 2010), but for fourth-order operators the hp-IPDG theory itself remains suboptimal in pp (Mozolevski, Süli, and Bösing proved analogous bounds for the biharmonic equation). For the quad-curl problem, Chen, Qiu, and Xu (2021) analyzed an hh-version mixed IPDG method, and Sun (2016) gave the first mixed finite element method for the eigenvalue problem; H(curl2)H(\mathrm{curl}^2)-conforming spectral element methods (Wang, Shan, Li, and Zhang, 2021; Wang, Li, Q. Zhang, and Z. Zhang, 2025) provide high-order approximation spaces but without pp-explicit error theory. Han and Zhang (2023) proposed the first hp-version IPDG method for the quad-curl source problem (with and without the divergence-free constraint) and its eigenvalue problem, with two interior penalty parameters. They proved well-posedness via a discrete Poincaré inequality in the discrete divergence-free space, established hp-version discrete compactness (the property, central to Maxwell-type eigenvalue approximation since Kikuchi and Boffi, that bounded discrete divergence-free fields are precompact in L2L^2, ruling out spurious eigenmodes), and then invoked the Babuška–Osborn spectral approximation framework (the classical perturbation theory relating operator convergence to eigenvalue/eigenvector convergence) to obtain eigenvalue convergence. Their bounds are optimal in hh but suboptimal in pp: for the source problem, the DG-norm bound behaves like hmin⁡(p+1,s)−2p3.5−sh^{\min(p+1,s)-2} p^{3.5-s} on nonconforming meshes (meshes with hanging nodes) and hmin⁡(p+1,s)−2p3−sh^{\min(p+1,s)-2} p^{3-s} on conforming meshes for solutions in HsH^s, and the eigenvalue bounds behave like h2min⁡(s,p+1)−4p7−2sh^{2\min(s,p+1)-4} p^{7-2s} and p6−2sp^{6-2s} respectively — by the authors' accounting, a loss of 3 orders of pp on nonconforming simplicial meshes and 2 orders on conforming ones. Their numerical experiments nevertheless show exponential pp-convergence for smooth solutions, so the defect is in the theory (the algebraic pp-exponents under finite regularity), where the losses trace back to pp-dependent constants in trace inequalities, in the interpolation analysis, and in a reconstruction operator: the discrete compactness proof rests on an inequality whose hidden constant is hh-independent by results of Houston, Perugia, Schneebeli, and Schötzau (2005) for time-harmonic Maxwell IPDG, but whose pp-independence is verified by the authors only for H(curl)H(\mathrm{curl})-conforming rectangular (Nédélec-type edge) elements. p-version discrete compactness is known for conforming discrete differential forms (Boffi, Costabel, Dauge, Demkowicz, and Hiptmair, 2011), but that result has not been transferred to the DG divergence-free reconstruction setting.

Problem Statement

For the hp-version interior penalty discontinuous Galerkin method of Han and Zhang (BIT Numerical Mathematics 63, 2023) for the quad-curl source problem curl4u=f\mathrm{curl}^4 u = f (both with and without the divergence-free constraint) and the associated quad-curl eigenvalue problem, on simplicial (triangular/tetrahedral) meshes with polynomial degree pp: determine the exact sharp dependence on the polynomial degree pp of each of the three a priori error bounds — the DG-norm error of the source problem, the eigenvalue errors, and the eigenfunction errors — on nonconforming and on conforming meshes. The three quantities are separately resolvable: fixing the sharp pp-exponent of any one of them settles that quantity and leaves the other two open (the loss currently reported in the theory being 3 orders of pp on nonconforming meshes and 2 orders on conforming meshes).

The paper notes two related gaps in the same convergence theory, recorded here as context rather than as requirements on a solution: the hidden constant in the reconstruction-based inequality underlying the hp discrete compactness of the discrete divergence-free DG space is verified to be independent of hh, but its independence of pp is established only for H(curl)H(\mathrm{curl})-conforming rectangular elements (Remark 4.1); and the extension of the hp-error analysis to general polygonal (2D) and polyhedral (3D) meshes is indicated but not performed (Remarks 3.1 and 4.2), including the conditions on element edge/face counts under which the uniform convergence of the discrete solution operators can be guaranteed.

References

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