A multiscale time integrator Fourier pseudospectral (MTI-FP) method is proposed and rigorously analyzed for the nonlinear Dirac equation (NLDE), which involves a dimensionless parameter inversely proportional to the speed of light. The solution to the NLDE propagates waves with wavelength and in time and space, respectively. In the nonrelativistic regime, i.e., the rapid temporal oscillation causes significantly numerical burdens, making it quite challenging for designing and analyzing numerical methods with uniform error bounds in . The key idea for designing the MTI-FP method is based on adopting a proper multiscale decomposition of the solution to the NLDE and applying the exponential wave integrator with appropriate numerical quadratures. Two independent error estimates are established for the proposed MTI-FP method as and , where is the mesh size, is the time step and depends on the regularity of the solution. These two error bounds immediately suggest that the MTI-FP method converges uniformly and optimally in space with exponential convergence rate if the solution is smooth, and uniformly in time with linear convergence rate at for all and optimally with quadratic convergence rate at in the regimes when either in the regimes when either or . Numerical results are reported to demonstrate that our error estimates are optimal and sharp.
Mots clés : Nonlinear Dirac equation, nonrelativistic limit, uniformly accurate, multiscale time integrator, exponential wave integrator, spectral method, error bound
@article{M2AN_2018__52_2_543_0, author = {Cai, Yongyong and Wang, Yan}, title = {A uniformly accurate {(UA)} multiscale time integrator pseudospectral method for the nonlinear {Dirac} equation in the nonrelativistic limit regime}, journal = {ESAIM: Mathematical Modelling and Numerical Analysis }, pages = {543--566}, publisher = {EDP-Sciences}, volume = {52}, number = {2}, year = {2018}, doi = {10.1051/m2an/2018015}, zbl = {1404.35377}, mrnumber = {3834435}, language = {en}, url = {http://www.numdam.org/articles/10.1051/m2an/2018015/} }
TY - JOUR AU - Cai, Yongyong AU - Wang, Yan TI - A uniformly accurate (UA) multiscale time integrator pseudospectral method for the nonlinear Dirac equation in the nonrelativistic limit regime JO - ESAIM: Mathematical Modelling and Numerical Analysis PY - 2018 SP - 543 EP - 566 VL - 52 IS - 2 PB - EDP-Sciences UR - http://www.numdam.org/articles/10.1051/m2an/2018015/ DO - 10.1051/m2an/2018015 LA - en ID - M2AN_2018__52_2_543_0 ER -
%0 Journal Article %A Cai, Yongyong %A Wang, Yan %T A uniformly accurate (UA) multiscale time integrator pseudospectral method for the nonlinear Dirac equation in the nonrelativistic limit regime %J ESAIM: Mathematical Modelling and Numerical Analysis %D 2018 %P 543-566 %V 52 %N 2 %I EDP-Sciences %U http://www.numdam.org/articles/10.1051/m2an/2018015/ %R 10.1051/m2an/2018015 %G en %F M2AN_2018__52_2_543_0
Cai, Yongyong; Wang, Yan. A uniformly accurate (UA) multiscale time integrator pseudospectral method for the nonlinear Dirac equation in the nonrelativistic limit regime. ESAIM: Mathematical Modelling and Numerical Analysis , Tome 52 (2018) no. 2, pp. 543-566. doi : 10.1051/m2an/2018015. http://www.numdam.org/articles/10.1051/m2an/2018015/
[1] Linearized Crank–Nicholson scheme for nonlinear Dirac equations. J. Comput. Phys. 99 (1992) 348–350. | DOI | MR | Zbl
,[2] The numerical study of a nonlinear one-dimensional Dirac equation. Appl. Math. Comput. 13 (1983) 1–15. | DOI | MR | Zbl
, and ,[3] Absorbing boundary conditions for relativistic quantum mechanics equations. J. Comput. Phys. 277 (2014) 268–304. | DOI | MR | Zbl
, , , and ,[4] Existence of standing waves for Dirac fields with singular nonlinearities. Commun. Math. Phys. 133 (1990) 53–74. | DOI | MR | Zbl
, and ,[5] Uniform and optimal error estimates of an exponential wave integrator sine pseudospectral method for the nonlinear Schrödinger equation with wave operator. SIAM J. Numer. Anal. 52 (2014) 1103–1127. | DOI | MR | Zbl
and ,[6] An efficient and stable numerical method for the Maxwell–Dirac system. J. Comput. Phys. 199 (2004) 663–687. | DOI | MR | Zbl
and ,[7] A uniformly accurate multiscale time integrator pseudospectral method for the Klein–Gordon equation in the non-relativistic limit regime. SIAM J. Numer. Anal. 52 (2014) 2488–2511. | DOI | MR | Zbl
, and ,[8] A uniformly accurate multiscale time integrator pseudospectral method for the Dirac equation in the non-relativistic limit regime. SIAM J. Numer. Anal. 54 (2016) 1785–1812. | DOI | MR | Zbl
, , and ,[9] Error estimates of numerical methods for the nonlinear Dirac equation in the non-relativistic limit regime. Sci. China Math. 59 (2016) 1461–1494. | DOI | MR | Zbl
, , and ,[10] Numerical methods and comparison for the Dirac equation in the non-relativistic limit regime. J. Sci. Comput. 71 (2017) 1094–1134. | DOI | MR | Zbl
, , and ,[11] Solutions of nonlinear Dirac equations. J. Diff. Equ. 226 (2006) 210–249. | DOI | MR | Zbl
and ,[12] (Semi)-non-relativistic limits of the Dirac equation with external time-dependent electromagnetic field. Commun. Math. Phys. 197 (1998) 405–425. | DOI | MR | Zbl
, and ,[13] Theory and numerical approximations for a nonlinear 1 + 1 Dirac system. ESAIM: M2AN 46 (2012) 841–874. | DOI | Numdam | MR | Zbl
and ,[14] A convergent 2D finite-difference scheme for the Dirac–Poisson system and the simulation of graphene. J. Comput. Phys. 257 (2014) 318–332. | DOI | MR | Zbl
, and ,[15] Y. Cai and Y. Wang, (Semi-)Nonrelativisitic limit of the nonlinear Dirac equations. In preparation.
[16] Chiral confinement: an exact solution of the massive Thirring model. Phys. Rev. D 11 (1975) 3572–3582. | DOI
, and ,[17] Uniformly accurate numerical schemes for highly oscillatory Klein–Gordon and nonlinear Schrödinger equations. Numer. Math. 129 (2015) 211–250. | DOI | MR | Zbl
, , and ,[18] Dirac and Klein Gordon equations: convergence of solutions in the non-relativistic limit. Commun. Math. Phys. 79 (1981) 33–46. | DOI | MR | Zbl
and ,[19] An overview on linear and nonlinear Dirac equations. Discrete Contin. Dyn. Syst. 8 (2002) 381–397. | DOI | MR | Zbl
and ,[20] Asymptotic preserving schemes for the Klein–Gordon equation in the non-relativistic limit regime. Numer. Math. 126 (2014) 441–469. | DOI | MR | Zbl
and ,[21] Split-step spectral schemes for nonlinear Dirac systems. J. Comput. Phys. 83 (1989) 407–423. | DOI | MR | Zbl
and ,[22] Numerical integration of ordinary differential equations based on trigonometric polynomials. Numer. Math. 3 (1961) 381–397. | DOI | MR | Zbl
,[23] The nonlinear Dirac equation in Bose–Einstein condensates: foundation and symmetries. Physics D 238 (2009) 1413–21. | DOI | MR | Zbl
and ,[24] Geometric Numerical Integration. Springer-Verlag (2002). | DOI | MR | Zbl
, and ,[25] Single-cone real-space finite difference scheme for the time-dependent Dirac equation. J. Comput. Phys. 265 (2014) 50–70. | DOI | MR | Zbl
, and ,[26] Exponential integrators. Acta Numer. 19 (2000) 209–286. | DOI | MR | Zbl
and ,[27] A time-splitting spectral scheme for the Maxwell–Dirac system. J. Comput. Phys. 208 (2005) 761–789. | DOI | MR | Zbl
, , , and ,[28] Uniformly accurate numerical schemes for the nonlinear Dirac equation in the non-relativistic limit regime. Commun. Math. Sci. 15 (2017) 1107–1128. | DOI | MR | Zbl
, and ,[29] From nonlinear Klein–Gordon equation to a system of coupled nonlinear Schrödinger equations. Math. Ann. 324 (2002) 359–389. | DOI | MR | Zbl
and ,[30] Soliton solutions for Dirac equations with homogeneous non-linearity in (1 + 1) dimensions. J. Phys. A: Math. Gen. 18 (1985) L1061–L1066. | DOI | MR
,[31] Chiral confinement in quasirelativistic Bose–Einstein condensates. Phys. Rev. Lett. 104 (2010) 073603. | DOI
, , , and ,[32] Existence of stationary states for nonlinear Dirac equations. J. Diff. Equ. 74 (1988) 50–68. | DOI | MR | Zbl
,[33] The non-relativistic limit of the nonlinear Dirac equation. Ann. Inst. Henri Poincaré 9 (1992) 3–12. | DOI | Numdam | MR | Zbl
,[34] Nonlinear spinor fields and its role in cosmology. Int. J. Theor. Phys. 51 (2012) 1812–1837. | DOI | MR | Zbl
,[35] On the non-relativistic limits of the Klein–Gordon and Dirac equations. J. Math. Anal. Appl. 71 (1979) 36–47. | DOI | MR | Zbl
,[36] Higher-order accurate Runge–Kutta discontinuous Galerkin methods for a nonlinear Dirac model. Discrete Contin. Dyn. Syst. B 6 (2006) 623–640. | MR | Zbl
and ,[37] Spectral Methods: Algorithms, Analysis and Applications. Springer-Verlag, Berlin, Heidelberg (2011). | DOI | Zbl
, and ,[38] Classical, stable, nonlinear spinor field with positive rest energy. Phys. Rev. D 1 (1970) 2766–2769. | DOI
,[39] Localised solutions of a non-linear spinor field. J. Phys. A: Math. Gen. 10 (1977) 1361–1368. | DOI | MR
,[40] An efficient adaptive mesh redistribution method for a nonlinear Dirac equation. J. Comput.Phys. 222 (2007) 176–193. | DOI | MR | Zbl
and ,[41] Gaussian beam methods for the Dirac equation in the semi-classical regime. Commun. Math. Sci. 10 (2012) 1301–1315. | DOI | MR | Zbl
, , and ,[42] Numerical methods for nonlinear Dirac equation. J. Comput. Phys. 245 (2013) 131–149. | DOI | MR | Zbl
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