Chaos and Intermittency in the DNLS Equation Describing the Parallel Alfvén Wave Propagation

<table>Time evolution of the mother wave for attractor <svg height="15.5375" id="M301" style="vertical-align:-3.13504pt" version="1.1" viewbox="0 0 18.924999 15.5375" width="18.924999" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
<g transform="matrix(.017,-0,0,-.017,.062,11.4)"><path d="M716 28l-8 -28h-254l8 28q55 5 66 17.5t5 47.5l-30 145h-232l-74 -138q-21 -43 -11 -54.5t72 -17.5l-6 -28h-235l8 28q53 7 73.5 21t53.5 70l319 540l33 8q6 -43 33 -176l80 -381q10 -49 26.5 -63t72.5 -19zM495 281l-49 264h-2l-149 -264h200z" id="x1D434"></path></g>
<g transform="matrix(.012,-0,0,-.012,12.525,15.475)"><path d="M412 140l28 -9q0 -2 -35 -131h-373v23q112 112 161 170q59 70 92 127t33 115q0 63 -31 98t-86 35q-75 0 -137 -93l-22 20l57 81q55 59 135 59q69 0 118.5 -46.5t49.5 -122.5q0 -62 -29.5 -114t-102.5 -130l-141 -149h186q42 0 58.5 10.5t38.5 56.5z" id="x32"></path></g>
</svg>. (a) Periodic solution. (b) Chaos.</table>

Journal of Astrophysics

fig9

Figure 9

Figure 9: Chaos and Intermittency in the DNLS Equation Describing the Parallel Alfvén Wave Propagation 