Symplectic integrator

In mathematics, a symplectic integrator (SI) is a numerical integration scheme for a specific group of differential equations related to classical mechanics and symplectic geometry. Symplectic integrators form the subclass of geometric integrators which, by definition, are canonical transformations. They are widely used in molecular dynamics, discrete element methods, accelerator physics, and celestial mechanics.

Introduction

Symplectic integrators are designed for the numerical solution of Hamilton's equations, which read:$$dot p = -frac{partial H}{partial q} quadmbox{and}quad dot q = frac{partial H}{partial p},where $$q denotes the position coordinates, $$p the momentum coordinates, and $$H is the Hamiltonian (see Hamiltonian mechanics for more background).

The time evolution of Hamilton's equations is a symplectomorphism, meaning that it conserves the symplectic two-form $$dp wedge dq. A numerical scheme is a symplectic integrator if it also conserves this two-form.

Symplectic integrators possess as a conserved quantity a Hamiltonian which is slightly perturbed from the original one. By virtue of these advantages, the SI scheme has been widely applied to the calculations of long-term evolution of chaotic Hamiltonian systems ranging from the Kepler problem to the classical and semi-classical simulations in molecular dynamics.

Most of the usual numerical methods, like the primitive Euler scheme and the classical Runge-Kutta scheme, are not symplectic integrators.

Splitting methods for separable Hamiltonians

A widely used class of symplectic integrators is formed by the splitting methods.

Assume that the Hamiltonian is separable, meaning that it can be written in the form:$$H(p,q) = T(p) + V(q). qquadqquad (1)This happens frequently in Hamiltonian mechanics, with "T" being the kinetic energy and "V" the potential energy.

Then the equations of motion of a Hamiltonian system can be expressed as:$$dot{z}={z,H(z)} (2)where $${cdot, cdot} is a Poisson bracket, and $$z=(q,p). By using the notation $$D_H = {cdot, H}, this can be re-expressed as:$$dot{z}=D_H z.The formal solution of this set of equations is given as:$$z( au)=exp( au D_H)z(0). (3)

When the Hamiltonian has the form of eq. (1), the solution (3) is equivalent to:$$z( au) = exp [ au (D_T + D_V)] z(0). (4)The SI scheme approximates the time-evolution operator $$exp [ au (D_T + D_V)] in the formal solution (4) by a product of operators as:$$exp [ au (D_T + D_V)] = Pi_{i=1}^k exp(c_i au D_T)exp(d_i au D_V) + O( au^{n+1}), (5)where $$c_i and $$d_i are real numbers, and $$n is an integer, which is called the order of the integrator. Note that each of the operators $$exp(c_i au D_T) and $$exp(d_i au D_V) provides a symplecticmap, so their product appearing in the right hand side of (5) also constitutes a symplectic map. In concrete terms, $$exp(c_i au D_T) gives the mapping:$$egin{pmatrix}q\ pend{pmatrix}mapstoegin{pmatrix}q'\ p'end{pmatrix}=egin{pmatrix} q + au c_i frac{partial T}{partial p}(p)\ pend{pmatrix}and $$exp(d_i au D_V) gives:$$egin{pmatrix}q\ pend{pmatrix}mapstoegin{pmatrix}q'\ p'end{pmatrix}=egin{pmatrix} q \ p - au d_i frac{partial V}{partial q}(q)\end{pmatrix}.Note that both of these maps are practically computable.

The symplectic Euler method is the first-order integrator with $$k=1 and coefficients:$$c_1 = d_1 = 1. The Verlet method is the second-order integrator with $$k=2 and coefficients:$$c_1 = c_2 = frac12, qquad d_1 = 1, qquad d_2 = 0.A fourth order integrator (with $$k=4) was independently discovered by three groups [cite journal
last = Forest
first = E.
coauthors=Ruth, R.D.
title=Fourth-order symplectic integration
journal=Physica D
date=1990
volume=43
pages=105
doi=10.1016/0167-2789(90)90019-L] [cite journal
last = Yoshida
first = H.
title = Construction of higher order symplectic integrators
journal=Phys. Lett. A
date=1990
volume=150
pages=262
doi = 10.1016/0375-9601(90)90092-3] [cite journal
last=Candy
first=J.
coauthors=Rozmus, W.
title=A Symplectic Integration Algorithm for Separable Hamiltonian Functions
journal=J. Comput. Phys.
date=1991
volume=92
pages=230
doi=10.1016/0021-9991(91)90299-Z]

:$$c_1 = c_4 = frac{1}{2(2-2^{1/3})}, c_2=c_3=frac{1-2^{1/3{2(2-2^{1/3})},:$$d_1 = d_3 = frac{1}{2-2^{1/3, d_2 = -frac{2^{1/3{2-2^{1/3, d_4 = 0.To determine these coefficients, the Baker–Campbell–Hausdorff formula can be used. Yoshida, in particular, gives an elegant derivation of coefficients for higher-order integrators.

References

* cite book
last = Leimkuhler
first = Ben
coauthors = Sebastian Reich
title = Simulating Hamiltonian Dynamics
publisher = Cambridge University Press
date = 2005
id = ISBN 0-521-77290-7