Seakweng Vong’s research while affiliated with University of Macau and other places

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Publications (115)


Error of the variational energy (top) and the variational mass (bottom) for the L1, L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} and variant L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} schemes for Example 5.2 with α=0.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha =0.5$$\end{document}, β=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =1$$\end{document} and p=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p=1$$\end{document}
Error of the variational energy (top) and the variational mass (bottom) for the L1 and variant L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} schemes for Example 5.2 with α=0.5\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\alpha =0.5$$\end{document}, β=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =1$$\end{document} and p=2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p=2$$\end{document}
Energy, mass and time steps curves of the L1 and L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} schemes for Example 5.2 with p=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p=1$$\end{document} and β=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =1$$\end{document}
Energy, mass and time steps curves of the L1 and L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} schemes for Example 5.2 with p=2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p=2$$\end{document} and β=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =1$$\end{document}
Energy, mass and time steps curves of the L2-1σ\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$_\sigma $$\end{document} schemes for Example 5.2 with p=1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$p=1$$\end{document} and β=-1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\beta =-1$$\end{document}
Compatible Conservation Laws and Discrete Counterparts for the Time-Fractional Nonlinear Schrödinger Equation
  • Article
  • Publisher preview available

April 2025

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80 Reads

Journal of Scientific Computing

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Seakweng Vong

We consider the conservation laws, regarding the energy and mass, for the time-fractional nonlinear Schrödinger (TFNLS) equation on both continuous and discrete levels. By introducing a class of fractional Leibniz formulas on the complex-field, a local energy conservation law and a local mass conservation law are established for the TFNLS equation. The two conservative laws are asymptotically compatible with the associated conservation laws of the NLS equation in the fractional order limit α1\alpha \rightarrow 1^-. On the discrete level, by establishing the discrete counterparts of fractional Leibniz formulas, we build up a unified framework for the construction and analysis of conservative variable-step methods, which is suitable for many discrete Caputo formulas, including the variable-step L1, L1-2, L2, L2-1σ_\sigma and L1+^+ formulas. These variable-step methods are showed to admit a discrete local energy conservation and a discrete local mass conservation laws without restrictions. The discrete energy and the discrete mass conservation laws are all asymptotically compatible with the corresponding conservation laws of the associated variable-step scheme, respectively, for the NLS problem. Numerical experiments are provided to verify the accuracy and efficiency of the conservative methods together with an adaptive time-stepping strategy in long time simulations. So far as we know, this is the first work on the energy and the mass variation laws as well as their asymptotic compatibility for the TFNLS equation.

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Nonsmooth Newton methods for vertical linear complementarity problems

Optimization Letters

In this paper, a new method for solving the vertical linear complementarity problems is established by the nonsmooth Newton iteration. With the row W\mathcal {W}-property of the set of the system matrices, the nonsingularity of the generalized Jacobian is proved and the nearly one-step convergence is presented. Furthermore, a hybrid nonsmooth Newton method is constructed to obtain global convergence. Finally, numerical examples are given to demonstrate the efficiency of the proposed methods.


Further analysis of weighted integral inequalities for improved exponential stability analysis of time delay neural networks systems

December 2024

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4 Reads

Yuanyuan Zhang

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Han Xue

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Kachong Lao

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Seakweng Vong

This work investigates the exponential stability of neural networks (NNs) systems with time delays. By considering orthogonal polynomials with weighted terms, a new weighted integral inequality is presented. This inequality extend several recently established results. Additionally, based on the reciprocally convex inequality, this study focuses on analyzing the exponential stability of systems with time-varying delays that include an exponential decay factor, a weighted version of the reciprocally convex inequality is first derived. Utilizing these inequalities and the suitable Lyapunov-Krasovskii functionals (LKFs) within the framework of linear matrix inequalities (LMIs), the new criteria for the exponential stability of NNs system is obtained. The effectiveness of the proposed method is demonstrated through multiple numerical examples.



A second-order fitted scheme for time fractional telegraph equations involving weak singularity

November 2024

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23 Reads

Fractional Calculus and Applied Analysis

In the present paper, to fill the gap of the effect of singularity arising from multiple fractional derivatives on numerical analysis, the regularity and high order difference scheme for time fractional telegraph equations are taken into consideration. Firstly, the analytic solution is obtained by employing Laplace transform, and its regularity is then deduced. Secondly, by the technic of decomposition, the improved regularity of solution is derived. Furthermore, to overcome the weak singularity and enhance convergence precision, a second-order fitted scheme based on L2-1σ1_\sigma approximation and order reduction method is applied to such problems, which is an improvement for the work [6]. Ultimately, examples are presented to verify the effectiveness of our theoretical results.



On the modulus-based methods without auxiliary variable for vertical linear complementarity problems

September 2024

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7 Reads

Journal of Applied Mathematics and Computing

In this paper, we conduct a further analysis of the modulus-based matrix splitting iteration method proposed in J-W He, S Vong. (Appl Math Lett 134: 108344, 2022) for vertical linear complementarity problems. Our study extends and enhances the existing theoretical theorems, which are also validated through numerical examples.


A variable‐step high‐order scheme for time‐fractional advection‐diffusion equation with mixed derivatives

Numerical Methods for Partial Differential Equations

We consider a high accuracy numerical scheme for solving the two‐dimensional time‐fractional advection‐diffusion equation including mixed derivatives, where the variable‐step Alikhanov formula and a fourth‐order compact approximation are employed to time and space derivatives, respectively. Under mild assumptions on the time step‐sizes, we obtain the unconditional stability and high‐order convergence (second‐order in time and fourth‐order in space) of the proposed scheme by energy method. The theoretical statements are justified by the numerical experiments.



A second-order weighted ADI scheme with nonuniform time grids for the two-dimensional time-fractional telegraph equation

July 2024

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18 Reads

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2 Citations

Journal of Applied Mathematics and Computing

In this paper, based on the weighted alternating direction implicit method, we investigate a second-order scheme with variable steps for the two-dimensional time-fractional telegraph equation (TFTE). Firstly, we derive a coupled system of the original equation by the symmetric fractional-order reduction (SFOR) method. Then the renowned L2-1σ1_\sigma formula on graded meshes is employed to approximate the Caputo derivative and a weighted ADI scheme for the coupled problem is constructed. In addition, with the aid of the Grönwall inequality, the unconditional stability and convergence of the weighted ADI scheme are analyzed. Finally, the numerical experiments are shown to verify the effectiveness and correctness of theoretical results.


Citations (73)


... Subsequently, by using variable-step L1 method, Refs. [11,29] obtain effective numerical schemes with satisfactory temporal convergence accuracy when the exact solution has multiple singularities in time. It is worth pointing out that the regularity results of Refs. ...

Reference:

Finite element method with Gr\"unwald-Letnikov type approximation in time for a constant time delay subdiffusion equation
Variable-step L 1 method combined with time two-grid algorithm for multi-singularity problems arising from two-dimensional nonlinear delay fractional equations
  • Citing Article
  • August 2024

Communications in Nonlinear Science and Numerical Simulation

... Yang et al. [27][28][29][30][31] introduced simple positivity preserving nonlinear finite volume scheme for subdiffusion equations on general non-conforming distorted meshes. Wang et al. [32,33] provided the compact ADI scheme for a 2D time-fractional integro-differential equation. Qiu et al. [34,35] introduced the ADI FEM for a nonlocal model. ...

A second-order weighted ADI scheme with nonuniform time grids for the two-dimensional time-fractional telegraph equation
  • Citing Article
  • July 2024

Journal of Applied Mathematics and Computing

... It is notable that the MVIP has been studied widely by many researchers due to its applications to many real problems in science and engineering such as the image restoration, signal processing, censor networks, data compression, machine learning, computer tomography, linear inverse problem, and radiation therapy [9]. ...

Modified general splitting method for the split feasibility problem

Journal of Global Optimization

... Abbaszadeh et al. [3] analyzed a nonlinear distributedorder time-fractional partial differential equation, utilizing a meshless method for the spatial direction and applying a nonuniform discrete time-fractional Caputo operator for the time variable. Finally, Ou et al. [27] investigated a two-dimensional nonlinear timefractional partial differential equation, solving it using FDM. Youssri et al. [41] proposed a semi-analytic numerical method for a one-dimensional time-fractional Tricomi-type equation. ...

A second-order fitted scheme combined with time two-grid technique for two-dimensional nonlinear time fractional telegraph equations involving initial singularity
  • Citing Article
  • April 2024

Journal of Computational and Applied Mathematics

... On the other hand, it is noted that there were some other accelerated techniques for the MMS iteration method, such as relaxation, precondition, two-sweep and so on. One can also mix a certain technique with the two-step splittings for acceleration, e.g., [3,22,30,47]. More techniques to improve the convergence of the MMS iteration method are worth studying in the future. ...

A relaxation two-step parallel modulus method without auxiliary variable for solving large sparse vertical linear complementarity problems

Numerical Algorithms

... On the other hand, it is noted that there were some other accelerated techniques for the MMS iteration method, such as relaxation, precondition, two-sweep and so on. One can also mix a certain technique with the two-step splittings for acceleration, e.g., [3,22,30,47]. More techniques to improve the convergence of the MMS iteration method are worth studying in the future. ...

A relaxed two-step modulus-based matrix synchronous multisplitting iteration method for linear complementarity problems
  • Citing Article
  • December 2023

Computational and Applied Mathematics

... Since then, modulus-based matrix splitting methods were extended to many generalizations of the LCP, such as HLCPs [18], (horizontal) nonlinear complementarity problems [19][20][21], implicit and quasi complementarity problems [22,23], and vertical linear and nonlinear complementarity problems [24,25]. Multisplittings were also used to achieve a parallel implementation of the algorithms [26][27][28][29][30][31][32]. More convoluted splitting techniques and non-splitting modulus-based methods were also introduced and studied for LCPs and their generalizations. ...

Modulus-based synchronous multisplitting iteration methods without auxiliary variable for solving vertical linear complementarity problems
  • Citing Article
  • December 2023

Applied Mathematics and Computation

... But in this article, we will employ the fitted scheme requiring less severe grading of the optimal mesh, which was first proposed for numerically solving the sub-diffusion equations in [27]. For such scheme, some related work has also been done in [28,29]. In the present paper, such scheme is aimed at reflecting the singular behaviour of the solution near the initial time: it establishes a difference approximation for time fractional telegraph equations, which is exact for the functions 1, t and t γ , i.e., it is fitted. ...

Fitted schemes for Caputo-Hadamard fractional differential equations

Numerical Algorithms

... Here, we derive the semidiscrete form of the MTCTFCRD model given by (1)(2)(3). To this end, we define a graded mesh on the time domain [0, ] with mesh size = − −1 for = 0, 1, 2, 3, … , . ...

Space–Time Methods Based on Isogeometric Analysis for Time-fractional Schrödinger Equation

Journal of Scientific Computing

... It is well known that the ADI (alternating direction implicit) technique is effective in dealing with high-dimensional problems, since it can reduce the original problems to a series of independent one-dimensional problems, significantly improving the computational efficiency with lower computational complexity and CPU time. There have been many various numerical schemes based on the ADI technique for solving high-dimensional fractional models in recent years; see [7][8][9][10][11][12], just to name a few. As far as we know, for the ADI numerical study of the model (1), there is little work available on this subject [13][14][15]. ...

A weighted ADI scheme with variable time steps for diffusion-wave equations

Calcolo