Energy norm error estimates of a hybrid high-order method for the linear parabolic integro-differential equations on general meshes
Pith reviewed 2026-05-10 10:01 UTC · model grok-4.3
The pith
The equal-order hybrid high-order method combined with Crank-Nicolson time stepping delivers error estimates of order O(τ² + h^{k+1}) for linear parabolic integro-differential equations.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We design an equal-order HHO spatial discretization for the linear parabolic integro-differential equations, prove stability and convergence for the semi-discrete problem in appropriate norms, then introduce a Crank-Nicolson time discretization with trapezoidal rule for the integral term, analyze stability of the fully discrete scheme, and derive error estimates of order O(τ² + h^{k+1}) in the discrete l²(0,T; H¹(Ω)) and l^∞(0,T; H¹(Ω)) norms, with numerical tests on polygonal meshes confirming the theory.
What carries the argument
The equal-order hybrid high-order (HHO) discretization, which uses local polynomial approximations of degree k on cells and faces, combined with a Crank-Nicolson scheme for time and trapezoidal quadrature for the memory integral.
Load-bearing premise
The exact solution has enough smoothness in space and time so that the error analysis applies, and the trapezoidal rule for the memory term preserves the second-order temporal accuracy.
What would settle it
Numerical simulations on a problem with known exact solution where the observed convergence rate in H1 norm falls below O(τ² + h^{k+1}) for small τ and h would contradict the estimates.
Figures
read the original abstract
We are concerned in designing a suitable numerical scheme based on the equal-order hybrid high-order (HHO) method for the linear parabolic integro-differential equations. The spatial discretization is made using the equal-order HHO method and subsequently we perform the stability analysis of the corresponding semi-discrete scheme. The convergence results are presented in suitably defined Bochner norms for the semi-discrete problem. Then a second-order temporal discretization is implemented on the time domain using a Crank-Nicolson scheme where the memory term is approximated using a composite trapezoidal quadrature rule. The stability of the resultant complete discrete schemes are analyzed followed by derivation of the error estimates of order $\mathcal{O}(\tau^{2}+h^{k+1})$, $k\ge 0$ is the degree of local polynomial approximation, in discrete $l^{2}(0,T;H^{1}(\Omega))$ and $l^{\infty}(0,T;H^{1}(\Omega))$ like norms. Numerical illustrations are performed on some polygonal meshes validating the theoretical estimates.
Editorial analysis
A structured set of objections, weighed in public.
Circularity Check
Standard energy-method derivation with no circular reductions
full rationale
The paper's error analysis for the semi-discrete HHO scheme and fully discrete Crank-Nicolson/trapezoidal scheme follows conventional consistency-plus-stability arguments in Bochner norms. The claimed O(τ² + h^{k+1}) rates are obtained from standard approximation properties of the HHO reconstruction and the quadrature error under the stated regularity assumptions; no step equates a prediction to a fitted input, renames a known result, or reduces the central bound to a self-citation chain. Self-citations (if present) support auxiliary lemmas but are not load-bearing for the main estimates.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption The exact solution belongs to sufficiently high-order Sobolev spaces so that interpolation and quadrature errors can be bounded by the stated powers of h and τ.
Reference graph
Works this paper leans on
-
[1]
W. Allegretto, Y. Liu, and A. Zhou. A box scheme for coupled syst ems resulting from microsensor thermistor problems. Dynamics of continuous discrete and impulsive systems , 5(1-4):209–223, 1999
work page 1999
- [2]
-
[3]
M. Cicuttin, A. Ern, and T. Gudi. Hybrid high-order methods for t he elliptic obstacle problem. Journal of Scientific Computing , 83(1):8, 2020
work page 2020
-
[4]
M. Cicuttin, A. Ern, N. Pignet, et al. Hybrid high-order methods: a primer with applications to solid mechanics . Springer, 2021
work page 2021
-
[5]
D. Di Pietro and J. Droniou. A hybrid high-order method for Lera y– Lions elliptic equations on general meshes. Mathematics of Computation , 86(307):2159–2191, 2017
work page 2017
-
[6]
D. A. Di Pietro and J. Droniou. The hybrid high-order method for polytopal meshes. Number 19 in Modeling, Simulation and Application , 84, 2020
work page 2020
-
[7]
D. A. Di Pietro, A. Ern, and S. Lemaire. An arbitrary-order and compact- stencil discretization of diffusion on general meshes based on local re- construction operators. Computational Methods in Applied Mathematics , 14(4):461–472, 2014
work page 2014
- [8]
- [9]
-
[10]
E. Greenwell-Yanik and G. Fairweather. Finite element methods f or parabolic and hyperbolic partial integro-differential equations. Nonlinear Anal, 12:785–809, 1988
work page 1988
-
[11]
T. Gudi, G. Mallik, and T. Pramanick. A hybrid high-order method f or quasilinear elliptic problems of nonmonotone type. SIAM Journal on Nu- merical Analysis, 60(4):2318–2344, 2022
work page 2022
-
[12]
R. Jain, A. K. Pani, and S. Yadav. HDG method for linear parabolic integro-differential equations. Applied Mathematics and Computation , 450:127987, 2023
work page 2023
-
[13]
S. Larsson, V. Thom´ ee, and L. Wahlbin. Numerical solution of p arabolic integro-differential equations by the discontinuous Galerkin metho d. Math- ematics of computation , 67(221):45–71, 1998. 35
work page 1998
-
[14]
Y. P. Lin, V. Thom´ ee, and L. B. Wahlbin. Ritz–Volterra project ions to finite-element spaces and applications to integrodifferential and related equations. SIAM Journal on Numerical Analysis , 28(4):1047–1070, 1991
work page 1991
-
[15]
Y. Liu, Z. Fang, H. Li, S. He, and W. Gao. A new expanded mixed me thod for parabolic integro-differential equations. Applied Mathematics and Com- putation, 259:600–613, 2015
work page 2015
-
[16]
R. Miller. An integrodifferential equation for rigid heat conducto rs with memory. Journal of Mathematical Analysis and Applications , 66(2):313– 332, 1978
work page 1978
-
[17]
R. Mottier, A. Ern, and L. Guillot. Elasto-acoustic wave propag ation in geo- physical media using hybrid high-order methods on general meshes . Com- puter Methods in Applied Mechanics and Engineering , 448:118458, 2026
work page 2026
-
[18]
K. Mustapha, H. Brunner, H. Mustapha, and D. Sch¨ otzau. A n hp- version discontinuous Galerkin method for integro-differential equ ations of parabolic type. SIAM journal on Numerical Analysis , 49(4):1369–1396, 2011
work page 2011
-
[19]
A. K. Pani and G. Fairweather. An H 1-Galerkin mixed finite element method for an evolution equation with a positive-type memory term. SIAM journal on Numerical Analysis , 40(4):1475–1490, 2002
work page 2002
-
[20]
A. K. Pani and T. E. Peterson. Finite element methods with nume rical quadrature for parabolic integrodifferential equations. SIAM Journal on Numerical Analysis, 33(3):1084–1105, 1996
work page 1996
-
[21]
A. K. Pani and R. K. Sinha. On superconvergence results and n egative norm estimates for parabolic integro-differential equations. The Journal of Integral Equations and Applications , pages 65–98, 1996
work page 1996
-
[22]
A. K. Pani and S. Yadav. An hp-local discontinuous Galerkin met hod for parabolic integro-differential equations. Journal of Scientific Computing , 46(1):71–99, 2011
work page 2011
-
[23]
C. Pao. Solution of a nonlinear integrodifferential system arising in nu- clear reactor dynamics. Journal of Mathematical Analysis and Applications , 48(2):470–492, 1974
work page 1974
- [24]
-
[25]
R. K. Sinha, R. E. Ewing, and R. D. Lazarov. Mixed finite element a pprox- imations of parabolic integro-differential equations with nonsmooth initial data. SIAM journal on Numerical Analysis , 47(5):3269–3292, 2009
work page 2009
-
[26]
I. H. Sloan and V. Thom´ ee. Time discretization of an integro-diff erential equation of parabolic type. SIAM Journal on Numerical Analysis , 23(5):1052–1061, 1986
work page 1986
-
[27]
V. Thom´ ee and N. Y. Zhang. Error estimates for semidiscrete finite ele- ment methods for parabolic integro-differential equations. Mathematics of Computation, 53(187):121–139, 1989. 36
work page 1989
-
[28]
X. Wang, Q. Zhai, R. Zhang, and S. Zhang. The weak Galerkin finit e ele- ment method for solving the time-dependent integro-differential e quations. Advances in Applied Mathematics and Mechanics , 12(1):164–188, 2020
work page 2020
- [29]
-
[30]
Y. Xu, Z. Zhou, and J. Zhao. Error analysis of serendipity virtu al element methods for semilinear parabolic integro-differential equations. Journal of Scientific Computing , 100(2):55, 2024
work page 2024
-
[31]
Y. Xu, Z. Zhou, and J. Zhao. Error estimates of a class of sere ndipity virtual element methods for semilinear parabolic integro-differential equat ions on curved domains. Journal of Computational Mathematics , 44(2):479–520, 2026
work page 2026
- [32]
-
[33]
A. Zhu, T. Xu, and Q. Xu. Weak Galerkin finite element methods fo r lin- ear parabolic integro-differential equations. Numerical Methods for Partial Differential Equations , 32(5):1357–1377, 2016
work page 2016
-
[34]
P. Zhu and S. Xie. Supercloseness and postprocessing of stab ilizer-free weak Galerkin finite element approximations for parabolic problems. Computers & Mathematics with Applications , 119:79–88, 2022. 7 Appendix Lemma 7.1. For any p ∈ W 2, 1(0, T ; H 1(Ω)) , we have the following estimate. ∫ tj+1 tj (p(tj+ 1 2 ) − p(s))ds H1(Ω) ≤ τ2 4 ...
work page 2022
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