Chaotic Transition
Definition
The phenomenon where a system becomes chaotic or remains non-chaotic depending on the change of parameters is called chaotic transition.
Examples
For example, if we consider the logistic family, a system formed by shows different behaviors depending on the parameter , and it can be observed that it has a chaotic orbit when . The next question then is ‘what happens when it’s ?’
Firstly, if it’s then which means its maximum is greater than , and maps to negative. Moreover, since it’s a quadratic function, once it goes beyond a certain for to occur, it diverges at an alarming rate afterwards. Before a chaotic orbit comes, it has to be a bounded orbit, but divergence means the chaotic nature was lost as the parameter changed, which according to the definition above, can be called a chaotic transition.
Such phenomenon will happen more quickly as the value of increases. Hence, we can guess there is some relation between , which makes occur, and . It is not very difficult to verify this through simulation, just by running the code, the following plot is drawn.
In the code, it slightly increases the value of while finding that satisfies for a random initial value , and repeats this times to calculate the average of , . Looking at the actual plot, one can observe the linear relationship between and .
Such chaotic transitions are not only found in logistic map systems but are phenomena discovered in many systems.
Code
ga<-function(a,x,k=1) {
tmp <- a*x *(1 - x)
if(k==1) {return( tmp ) }
else {return(ga(a,tmp,k-1))}
}
N<-1000
y<-numeric(0)
A<-4+10^(-(80:120)/20)
for(a in A){
taubar<-0
for(i in 1:N){
tau<-0
x<-runif(1)
while(x>0){
x<-ga(a,x)
tau=tau+1
}
taubar<-taubar+tau
}
y<-c(y,taubar/N)
}
taubar<-y
a<-A
win.graph(); plot(log(a-4),log(taubar),type='l',main='a>4 일 때 로지스틱 맵의 Chaotic Transient')