dx/dt = -y -z
dy/dt = x + ay
dz/dt = b + z(x - c)
where a=b=1/5, c=5.7
The
Attractor for t=500.
(here t=20000.)
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The Poincare section is chosen to be in the positive part of the plane
(Y,Z).
Prime periodic orbits of length N correspond to N different fixpoints
in the N-return maps. These fixed points are defined by the intersection
of the curves with the diagonal (Y(t+N)=Y(t)). On the figures the fixed
points that correspond to the same periodic orbit are labeled with the
same capitol letter. Also indicated in the N-return maps are the
regions with an appropriate symbolic dynamics. The precise location of
the periodic orbits and the stability eigenvalues were obtained by using
a Newton-routine.
Period of the orbit:T=5.88108845586 ;
Poincare section point: X=0; Y=6.09176831742; Z=1.29973195919;
eigenvalues of the Jacobian: 1.000000003, -2.403953527, -0.1836169064e-10
liapunov exponent: 0.149141556;
Period of the orbit:T=11.7586260717;
One of the Poincare section points (in the 1,0 itinerary):
X=0; Y=6.91498284608; Z=0.0757168639342;
eigenvalues of the Jacobian: 1.000000000, -3.512006980,
0.8290005176e-12
liapunov exponent: 0.10683116;
periodic orbit (C) with symbolic dynamics: 1,0,0.
Period of the orbit:T=17.5157912663;
One of the Poincare section points (in the 1,0,0 itinerary):
X= 0; Y=7.54996784577; Z=0.140432840371;
eigenvalues of the Jacobian: 1.000000019, -2.341918959, 0.8112502046e-11
liapunov exponent: 0.048583055;
Period of the orbit:T=17.5958658156;
One of the Poincare section points (in the 1,0,1 itinerary):
X=0; Y=7.29442965395; Z=0.556169637263;
eigenvalues of the Jacobian: 1.000000001, 5.344908108, 0.1349406670e-10
liapunov exponent: 0.09525785;
Period of the orbit:T= 23.508557584;
One of the Poincare section points (in the 1,0,1,1 segment):
X=0; Y=7.08997393429; Z= 0 .675113965985;
eigenvalues of the Jacobian: 1.000000001, -16.69674069, -.7258300597e-10
liapunov exponent: 0.119752712;