1978 Torn Unimodal Chaos

What torn unimodal chaos is ?

It is known that for producing a chaotic behavior, sensitivity to initial conditions is combined to some recurrence properties. These two specific characteristics result from two mechanisms : stretching and squeezing. This can be produced by a folding or a tearing. Typically, an attractor involving a folding is produced by the Rössler system and one involving a tearing is the Lorenz system. These two mechanisms were investigated in [1]. Torn unimodal chaos corresponds to an attractor with a tearing mechanism that is characterized by a cusp --- or a Lorenz --- map. The Lorenz system is a good example but it has a rotation symmetry. The purpose here is to have an attractor with a tearing mechanism without any symmetry.

The system

To the best of our knowledge, the first set of equations that was identified to produce a chaotic attractor bounded by a genus-1 torus and possessing a Lorenz map was proposed by Otto Rössler and Peter Ortoleva from Indiana University [2] as an isothermal abstract reaction system. The systems reads :

This abstract chemical reaction produces a torn unimodal chaotic attractor as shown in Fig. 1. Parameter values are \(a=33\), \(b=150\), \(c=1\), \(d=3.5\), \(e=4815\), \(f=410\), \(g=0.59\), \(h=4\), \(j=2.5\), \(k=2.5\), \(l=5.29\), \(m=750\), \(K_1=0.01\) and \(K_2=0.01\). A first-return map to a Poincaré section (Fig. 2) has the shape of the Lorenz map as expected. The \(l\)-value is slightly modified to obtain a Lorenz map without a gap between the two monotonic branches as originally published in Ref. 2.