IOP PUBLISHING JOURNAL OF PHYSICS A: MATHEMATICAL AND THEORETICAL
J. Phys. A: Math. Theor. 41 (2008) 485101 (13pp) doi:10.1088/1751-8113/41/48/485101
On the topology of the L ¨ u attractor and related
systems
S Anastassiou
1
, T Bountis
1
and Y G Petalas
2
1
Center for Research and Applications of Nonlinear Systems (CRANS),
Department of Mathematics, University of Patras, GR-26500, Patras, Greece
2
Computational Intelligence Laboratory (CI Lab), Artificial Intelligence Research Center
(UPAIRC), Department of Mathematics, University of Patras, GR-26500, Patras, Greece
E-mail: SAnastassiou@gmail.com
Received 27 June 2008, in final form 11 September 2008
Published 22 October 2008
Online at stacks.iop.org/JPhysA/41/485101
Abstract
We use well-established methods of knot theory to study the topological
structure of the set of periodic orbits of the L¨ u attractor. We show that,
for a specific set of parameters, the L ¨ u attractor is topologically different from
the classical Lorenz attractor, whose dynamics is formed by a double cover
of the simple horseshoe. This argues against the ‘similarity’ between the L¨ u
and Lorenz attractors, claimed, for these parameter values, by some authors
on the basis of non-topological observations. However, we show that the L¨ u
system belongs to the Lorenz-like family, since by changing the values of the
parameters, the behaviour of the system follows the behaviour of all members
of this family. An attractor of the L¨ u kind with higher order symmetry is
constructed and some remarks on the Chen attractor are also presented.
PACS number: 05.45.−a
1. Introduction
L¨ u and Chen introduced in [11] a simple 3-parameter family of ordinary differential equations
(ODEs), nowadays called the L¨ u system, which exhibits chaotic behaviour. The equations of
this system are
˙ x = a(y − x)
˙ y =−xz + cy
˙ z = xy − bz
(1)
where a,b,c are real parameters. In the same paper, L¨ u and Chen integrated these ODEs
numerically, for fixed a = 36 and b = 3, varying only the third parameter. They observed that,
when 12.7 <c< 17, the attractor generated by (1) is pictorially ‘similar’ to the well-known
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