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Evolution and Optimum Seeking

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A Multimembered <strong>Evolution</strong> Strategy 133<br />

2.0<br />

1.0<br />

1<br />

Maximal universal rate<br />

of progress<br />

ϕ ( σ )<br />

max opt<br />

(1+1) - theory<br />

Numer of offspring<br />

5 10 15 20 25 30<br />

Figure 5.10: Maximal rate of progress for the sphere model<br />

Points on the curve ' max = ' ( = opt) can only be obtained iteratively. To<br />

express = (' max), the non-linear system of equations consisting of Equations (5.20)<br />

<strong>and</strong> (5.21) must be solved. The results as obtained with the multimembered evolution<br />

strategy are shown in Figure 5.10. A convenient formula can only be obtained by assuming<br />

' + ' + i.e., 2 ' max ' 2<br />

opt<br />

This estimate is actually not far wrong, since the second term in Equation (5.21) goes to<br />

zero. We thus nd<br />

' 1+ q 'max exp('max ) 1 + erf 1 q<br />

'max (5.22)<br />

2<br />

a relation with comparable structure to the result for the inclined plane.<br />

Finally we ask whether ' max= has a maximum, as in the inclined plane case. If the<br />

parent can survive the o spring, opt = 1 here too if not the condition<br />

p 1<br />

opt =2<br />

2 +('+ + + ) 2 exp[(' + + + ) 2 ][1 + erf( + )] ' +<br />

must be added to Equations (5.20) <strong>and</strong> (5.21). The solution, obtained iteratively, is:<br />

opt ' 4:7 (as an integer: opt =5)<br />

λ<br />

(5.23)

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