A conservative semi-Lagrangian HWENO method for the Vlasov equation

In this paper, we propose a high order conservative semi-Lagrangian (SL) finite difference Hermite weighted essentially non-oscillatory (HWENO) method for the Vlasov equation based on dimensional splitting. HWENO was first proposed for solving nonlinear hyperbolic problems by evolving both function values and its first derivative values (Qiu and Shu (2004) 23). The major advantage of HWENO, compared with the original WENO, lies in its compactness in reconstruction stencils.There are several new ingredients in this paper. Firstly we propose a mass-conservative SL HWENO scheme for a 1-D equation by working with a flux-difference form, following the work of Qiu and Christlieb (2010) 25. Secondly, we propose a proper splitting for equations of partial derivatives in HWENO framework to ensure local mass conservation. The proposed fifth order SL HWENO scheme with dimensional splitting has been tested to work well in capturing filamentation structures without oscillations when the time step size is within the Eulerian CFL constraint. However, when the time stepping size becomes larger, numerical oscillations are observed for the 'mass conservative' dimensional splitting HWENO scheme, as there are extra source terms in equations of partial derivatives. In this case, we introduce WENO limiters to control oscillations. Classical numerical examples on linear passive transport problems, as well as the nonlinear Vlasov-Poisson system, have been tested to demonstrate the performance of the proposed scheme.

[1]  Blanca Ayuso de Dios,et al.  DISCONTINUOUS GALERKIN METHODS FOR THE MULTI-DIMENSIONAL VLASOV–POISSON PROBLEM , 2012 .

[2]  P. J. Morrison,et al.  A discontinuous Galerkin method for the Vlasov-Poisson system , 2010, J. Comput. Phys..

[3]  Chi-Wang Shu,et al.  Runge-Kutta Discontinuous Galerkin Method Using WENO Limiters , 2005, SIAM J. Sci. Comput..

[4]  Jun Zhu,et al.  A class of the fourth order finite volume Hermite weighted essentially non-oscillatory schemes , 2008 .

[5]  L. Gardner,et al.  A finite element code for the simulation of one-dimensional Vlasov plasmas I. Theory , 1988 .

[6]  Chi-Wang Shu,et al.  Runge–Kutta Discontinuous Galerkin Methods for Convection-Dominated Problems , 2001, J. Sci. Comput..

[7]  Chi-Wang Shu,et al.  Conservative high order semi-Lagrangian finite difference WENO methods for advection in incompressible flow , 2011, J. Comput. Phys..

[8]  S. Osher,et al.  Efficient implementation of essentially non-oscillatory shock-capturing schemes,II , 1989 .

[9]  E. G. Evstatiev,et al.  Variational formulation of particle algorithms for kinetic E&M plasma simulations , 2012, 2016 IEEE International Conference on Plasma Science (ICOPS).

[10]  G. Knorr,et al.  The integration of the vlasov equation in configuration space , 1976 .

[11]  Jianxian Qiu,et al.  Hermite WENO schemes and their application as limiters for Runge-Kutta discontinuous Galerkin method: one-dimensional case , 2004 .

[12]  Chang Yang,et al.  Conservative and non-conservative methods based on Hermite weighted essentially non-oscillatory reconstruction for Vlasov equations , 2013, J. Comput. Phys..

[13]  David C. Seal,et al.  A positivity-preserving high-order semi-Lagrangian discontinuous Galerkin scheme for the Vlasov-Poisson equations , 2010, J. Comput. Phys..

[14]  Chi-Wang Shu,et al.  Positivity preserving semi-Lagrangian discontinuous Galerkin formulation: Theoretical analysis and application to the Vlasov-Poisson system , 2011, J. Comput. Phys..

[15]  L. Gardner,et al.  A finite element code for the simulation of one-dimensional Vlasov plasmas. II.Applications , 1988 .

[16]  Takayuki Umeda,et al.  A conservative and non-oscillatory scheme for Vlasov code simulations , 2008 .

[17]  Andrew J. Christlieb,et al.  A conservative high order semi-Lagrangian WENO method for the Vlasov equation , 2010, J. Comput. Phys..

[18]  E. Sonnendrücker,et al.  The Semi-Lagrangian Method for the Numerical Resolution of the Vlasov Equation , 1999 .

[19]  T. Yabe,et al.  Cubic interpolated propagation scheme for solving the hyper-dimensional Vlasov-Poisson equation in phase space , 1999 .

[20]  Jan S. Hesthaven,et al.  High-order nodal discontinuous Galerkin particle-in-cell method on unstructured grids , 2006, J. Comput. Phys..

[21]  Piet Hut,et al.  A hierarchical O(N log N) force-calculation algorithm , 1986, Nature.

[22]  Wei Guo,et al.  Hybrid semi-Lagrangian finite element-finite difference methods for the Vlasov equation , 2013, J. Comput. Phys..

[23]  Yan Guo,et al.  Numerical study on Landau damping , 2001 .

[24]  Zhengfu Xu,et al.  High order maximum principle preserving semi-Lagrangian finite difference WENO schemes for the Vlasov equation , 2013, J. Comput. Phys..

[25]  P. Bertrand,et al.  Conservative numerical schemes for the Vlasov equation , 2001 .

[26]  T. Yabe,et al.  The constrained interpolation profile method for multiphase analysis , 2001 .

[27]  Nicolas Besse,et al.  Semi-Lagrangian schemes for the Vlasov equation on an unstructured mesh of phase space , 2003 .

[28]  Jianxian Qiu,et al.  Finite Difference Hermite WENO Schemes for Hyperbolic Conservation Laws , 2014, Journal of Scientific Computing.

[29]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[30]  Nicolas Besse Convergence of a High-Order Semi-Lagrangian Scheme with Propagation of Gradients for the One-Dimensional Vlasov-Poisson System , 2008, SIAM J. Numer. Anal..

[31]  Scott E. Parker,et al.  Multi-scale particle-in-cell plasma simulation , 1991 .

[32]  Jing-Mei Qiu,et al.  Conservative Semi-Lagrangian Finite Difference WENO Formulations with Applications to the Vlasov Equation , 2011 .

[33]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[34]  J. N. Leboeuf,et al.  Implicit particle simulation of magnetized plasmas , 1983 .

[35]  Yingda Cheng,et al.  Study of conservation and recurrence of Runge–Kutta discontinuous Galerkin schemes for Vlasov–Poisson systems , 2012, J. Sci. Comput..

[36]  Eric Sonnendrücker,et al.  Conservative semi-Lagrangian schemes for Vlasov equations , 2010, J. Comput. Phys..

[37]  José A. Carrillo,et al.  Discontinuous Galerkin methods for the one-dimensional Vlasov-Poisson system , 2011 .

[38]  R. LeVeque High-resolution conservative algorithms for advection in incompressible flow , 1996 .

[39]  E. Sonnendrücker,et al.  Comparison of Eulerian Vlasov solvers , 2003 .