2016
DOI: 10.1016/j.jcp.2016.09.047
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Explicit high-order symplectic integrators for charged particles in general electromagnetic fields

Abstract: This article considers non-relativistic charged particle dynamics in both static and non-static electromagnetic fields, which are governed by nonseparable, possibly timedependent Hamiltonians. For the first time, explicit symplectic integrators of arbitrary high-orders are constructed for accurate and efficient simulations of such mechanical systems. Performances superior to the standard non-symplectic method of Runge-Kutta are demonstrated on two examples: the first is on the confined motion of a particle in … Show more

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Cited by 60 publications
(34 citation statements)
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“…There have been recent efforts to construct explicit symplectic integrators for this problem [9,10,12]. While such methods of arbitrary order have been shown to exist, they require many evaluations of A and A or evaluations of higher derivatives of A.…”
Section: Ehairer and C Lubichmentioning
confidence: 99%
See 1 more Smart Citation
“…There have been recent efforts to construct explicit symplectic integrators for this problem [9,10,12]. While such methods of arbitrary order have been shown to exist, they require many evaluations of A and A or evaluations of higher derivatives of A.…”
Section: Ehairer and C Lubichmentioning
confidence: 99%
“…While such methods of arbitrary order have been shown to exist, they require many evaluations of A and A or evaluations of higher derivatives of A. For example, the fourth-order method proposed in [10] requires 16 evaluations of each A and A per time step. This needs to be put in comparison with the two-stage Gauss-Runge-Kutta method, which is an implicit fourth-order symplectic method.…”
Section: Ehairer and C Lubichmentioning
confidence: 99%
“…The Boris method was presented in [2] and it was researched further in [8,13,26]. Various other kinds of methods have also been researched for charged-particle dynamics, such as volume-preserving algorithms in [17], symplectic or K-symplectic algorithms in [18,29,33,35], and symmetric multistep methods in [14]. It is worth mentioning that, more recently, a variational integrator has been studied in [15] for solving charged-particle dynamics in a strong magnetic field.…”
Section: Introductionmentioning
confidence: 99%
“…The method needs derivatives of the electric and magnetic field, though, which may be difficult to obtain. A recently introduced new class of methods are so-called explicit symplectic shadowed Runge-Kutta methods or ESSRK for short [11]. They are symplectic and therefore have bounded long-term energy error.…”
Section: Introductionmentioning
confidence: 99%