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Evolution and Optimum Seeking

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A Multimembered <strong>Evolution</strong> Strategy 147<br />

Parents of<br />

generation g<br />

Descendants<br />

x x x . . .<br />

x<br />

1 2 3 n<br />

Discrete global recombination<br />

Figure 5.15: Scheme of global uniform recombination<br />

Recombination<br />

by choosing<br />

components<br />

columnwise<br />

<strong>and</strong> at r<strong>and</strong>om<br />

This is, however, the only way to arrive atquantitative statements, free from confusing<br />

side e ects.<br />

It is thus hard to explain the origin of the accelerating e ect of recombination. It<br />

may, for example, lie in the fact that instead of di erent starting points, the bisexual<br />

scheme o ers<br />

2 + (<br />

n;2 X<br />

; 1) 2i possible combinations in the case of n variables. With multirecombination, as chosen<br />

here, there are as many as n ,which is far more than could be put into e ect. A more<br />

detailed investigation may be found in Back (1994a).<br />

So far we have only considered recombination of the object variables, but the strategy<br />

variables, the step lengths, can be recombined in just the same way. Even if all the parents<br />

start with equal i = for all i = 1(1)n, <strong>and</strong> if all the step length components are varied<br />

by a common r<strong>and</strong>om factor in the production of descendants, the variances i of all the<br />

individuals for each i = 1(1)n di er from each other in the subsequent generations.<br />

Thus by recombination is it possible for the step lengths to adapt individually in<br />

this way to circumstances. A better combination a ords a higher chance of survival to<br />

its bearer. It can therefore be expected that in the course of the optimum search, the<br />

currently best combination of the f i i= 1(1)ng prevails{the one that is associated with<br />

the fastest rate of progress. In attempting to verify this in a practical test, an unpleasant<br />

phenomenon occurs. It can happen that one of the st<strong>and</strong>ard deviations i is suddenly<br />

i=1

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