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Evolution and Optimum Seeking

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148 <strong>Evolution</strong> Strategies for Numerical Optimization<br />

(e.g., by a r<strong>and</strong>om value very far from the expectation value) so much reduced in size that<br />

the associated variable xi can now hardly be changed. The total change in the vector x is<br />

then roughly speaking within an (n ; 1)-dimensional subspace of IR n .Contrary to what<br />

one might hope, that such a descendant would have less chance of surviving than others,<br />

it turns out that the survival of such a descendant is actually favored. The reason is that<br />

the rate of progress with an optimal step length is proportional to 1=n. If the number<br />

of variables n decreases, the rate of convergence, together with the optimal step length,<br />

increases. The optimum search therefore only proceeds in a subspace of IR n . Not until<br />

the only improvement in the objective function entails changing the variable that has<br />

hitherto been omitted from the variation will the mutation-selection mechanism operate<br />

to increase its associated variance <strong>and</strong> so restore it to the range for which noticeable<br />

changes are possible.<br />

The minimum search proceeds by jumps in the value of the objective function <strong>and</strong><br />

with rates of progress that vary alternately above <strong>and</strong> below whatwould otherwise be<br />

smooth convergence. Such unstable behavior is most pronounced when , the number<br />

of parents, is small. With su ciently large the reserve of step length combinations<br />

in the gene pool is always big enough to avoid overadaptation, or to compensate for it<br />

quickly. From an experimental study (Schwefel, 1987) the conclusion could be drawn<br />

that punctuated equilibrium evolution (Gould <strong>and</strong> Eldredge, 1977, 1993) can be avoided<br />

by using a su ciently large population ( >1) <strong>and</strong> a su ciently low selection pressure<br />

( = ' 7). A further improvement can be made by using as the starting point inthe<br />

variation of the step lengths the currentaverage of two parents' variances, rather than the<br />

value from only one or the other parent. This measure too has its biological justi cation<br />

it represents an imitation of what is called intermediary recombination (instead of discrete<br />

recombination).<br />

In this context chromosome mutations should be very e ective, those in which for<br />

example, the positions of two individual step lengths are exchanged. As well as the haploid<br />

scheme of inheritance on which the presentwork is based, some forms of life also exhibit the<br />

diploid scheme. In this case each individual stores two sets of variable values. Whilst the<br />

formation of the phenotype only makes use of one allele, the production of o spring brings<br />

both alleles into the gene pool. If both alleles are the same one speaks of homozygosity,<br />

otherwise of heterozygosity. Heterozygote alleles enlarge the set of variants in the gene<br />

pool <strong>and</strong> thus the range of possible combinations. With regard to the stability of the<br />

evolutionary process this also appears to be advantageous. The true gain made by diploidy<br />

only becomes apparent, however, when the additional evolutionary factors of recessiveness<br />

<strong>and</strong> dominance are included. For multiple criteria optimization, the usefulness of this<br />

concept has been demonstrated by Kursawe (1991, 1992). Many possible extensions of<br />

the multimembered scheme have yet to be put into practice. To nd their theoretical<br />

e ect on the rate of progress, one would rst have to construct a theory of the ( , )<br />

strategy for > 1. If one goes beyond the = 1 scheme followed here, signi cant<br />

di erences between approximate theory <strong>and</strong> simulation results arise for >1 because of<br />

the greater asymmetry of the probability distribution w(s 0 ).

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