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13th International Conference on Membrane Computing - MTA Sztaki

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Maintenance of chr<strong>on</strong>obiological informati<strong>on</strong> by P system mediated assembly<br />

of c<strong>on</strong>trol units for oscillatory waveforms and frequency<br />

seems that the resulting toggling process runs slightly more fragile than in the<br />

Repressilator study. This becomes visible by a pr<strong>on</strong>ounced signal tuning, which<br />

exhibits damped high frequential micro oscillati<strong>on</strong>s in c<strong>on</strong>juncti<strong>on</strong> with output<br />

switch. Even several modificati<strong>on</strong>s of the experimental setup c<strong>on</strong>firm this behaviour,<br />

for instance a more distinctive transient oscillati<strong>on</strong> of the Goodwin<br />

module (shown in Figure 9) as well as doubling the rate c<strong>on</strong>stants from k =0.05<br />

to k =0.1 within the Goodwin module. Again, the core oscillator c<strong>on</strong>tinuably<br />

disturbes the computati<strong>on</strong> of the bits b ′ 1 up to b ′ 5.<br />

repressilator[1]<br />

brusselator[1]<br />

separator[1]<br />

B 2<br />

T<br />

4<br />

C<br />

goodwin[1]<br />

C<br />

mod17[1]<br />

B T 1<br />

T<br />

B 2<br />

T<br />

B 3<br />

T<br />

B 4<br />

T<br />

B 5<br />

0 0 1 1 0<br />

0<br />

1<br />

1<br />

1<br />

1<br />

0<br />

1<br />

0<br />

1<br />

0<br />

c<strong>on</strong>centrati<strong>on</strong> (a.u.)<br />

3.5<br />

3<br />

2.5<br />

2<br />

1.5<br />

1<br />

0.5<br />

0<br />

0 200 400 600 800 1000 1200<br />

time (a.u.)<br />

Fig. 9. Dynamical behaviour of the frequency divider 1:3 obtained by replacing the<br />

Brusselator with the Goodwin module in absence of the binary signal separator (left:<br />

cycle of state transiti<strong>on</strong>s, right: counts together with divider output). Instead of B1 T ,<br />

we depict B2<br />

T as divider output due to its more precisely toggling nature.<br />

3.6 Discussi<strong>on</strong><br />

The experimental results indicate that an originally designed frequency divider<br />

1:17 might change its behaviour revealing divisi<strong>on</strong> ratios of 1:3, 1:5, and 1:6<br />

just by slight rewiring of few interacting modules. By using a binary counter<br />

approach modulo 17, we intenti<strong>on</strong>ally employed a pure synthetic reacti<strong>on</strong> system<br />

derived from standard c<strong>on</strong>cepts in engineering. Although, those systems tend to<br />

be quite resistent against evoluti<strong>on</strong>ary optimisati<strong>on</strong>, there is some evidence for<br />

achievement of new or extended functi<strong>on</strong>alities. A detailed plausibilisati<strong>on</strong> of the<br />

observed behavioural pattern directly arises from the entirety of c<strong>on</strong>centrati<strong>on</strong><br />

courses involved in carrying out the state transiti<strong>on</strong>s. In order to emphasise<br />

this line of evidence, we c<strong>on</strong>ducted an additi<strong>on</strong>al simulati<strong>on</strong> study by c<strong>on</strong>sistent<br />

variati<strong>on</strong> of the rate c<strong>on</strong>stants within the logical unit. Slowing down its reacti<strong>on</strong>s<br />

by setting k =0.1 instead of k = 1 leads to complete loss of frequency divisi<strong>on</strong> by<br />

forwarding the core oscillator’s period instead. Here, the entire system exhibits<br />

a fragile “cycle” at the edge of chaotic behaviour after a l<strong>on</strong>ger transient phase,<br />

237

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