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Down the waterfall

The splitting of the stable fixed point tex2html_wrap_inline9374 into a stable 2-cycle as tex2html_wrap_inline6624 becomes greater than 3 is called a bifurcation (a fancy Latin word for splitting). As tex2html_wrap_inline6624 increases further, more bifurcations happen. In particular, we expect another bifurcation just beyond tex2html_wrap_inline9380 . Trying tex2html_wrap_inline4862 , we obtain the web diagram in this figure. 100 iterations are plotted in this figure, and it appears the forward orbit settles into a cycle of 4 points.

   figure2776
Figure 68: The web diagram for tex2html_wrap_inline4862 : a 4-cycle appears

Therefore, apparently our stable 2-cycle has now bifurcated into a stable 4-cycle.

The algebra of these bifurcations becomes increasingly vexing. To find a 4-cycle, we must solve the equation tex2html_wrap_inline9386 . Unfortunately, this is a degree tex2html_wrap_inline9388 polynomial equation, and that's tough even on a computer. But wait! We know some of the roots come from tex2html_wrap_inline9390 . So we may restrict ourselves to the polynomial

displaymath9392

Alas, this is still a degree 16-4=12 polynomial, which is wee bit out of our range.

Moreover, the attractive 4-cycles also satisfy tex2html_wrap_inline9396 . Perhaps this can help. At the beginning and end of the range of tex2html_wrap_inline6624 's where there is an attracting 4-cycle, we must have tex2html_wrap_inline9400 . These are degree 15 equations. It is possible to combine two different polynomial equations in two variables x and tex2html_wrap_inline6624 into a single equation in one of the variables, particularly tex2html_wrap_inline6624 . Even this is not terribly pleasant to do. Fortunately, there is a dynamical approach that we know very well.



David J. Wright
Mon Aug 19 17:21:15 CDT 1996