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13th International Conference on Membrane Computing - MTA Sztaki

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T. Hinze, B. Schell, M. Schumann, C. Bodenstein<br />

3 Explorati<strong>on</strong> of Chemical Frequency Dividers Inspired<br />

by Periodical Cicada’s Life Cycles<br />

In a first applicati<strong>on</strong> study inspired by periodical cicada’s life cycles, we dem<strong>on</strong>strate<br />

the practicability of our P meta framework Π π↑↓ =(M,P) for tracing and<br />

experimental explorati<strong>on</strong> of c<strong>on</strong>trolled module assembly towards new (i.e. more<br />

or less unexpected) behavioural patterns of the resulting entire system. First, we<br />

introduce in brief a pool of n<strong>on</strong>-probabilistic P modules sufficient to interact as a<br />

chemical frequency divider 1:17. To this end, we place a selecti<strong>on</strong> of different core<br />

oscillators interpreted to be employed for generati<strong>on</strong> of periodical trigger signals.<br />

A binary signal separator complements the pool of modules by its capability of<br />

binarisati<strong>on</strong> which c<strong>on</strong>verts gradually or smoothly altering signal courses into<br />

a toggling manner whereas signal values ≥ 1andthosecloseto1c<strong>on</strong>vergeto<br />

1 while signal values of ≈ 0.6 and smaller become forced down against 0. In<br />

additi<strong>on</strong>, we c<strong>on</strong>struct a logical unit whose functi<strong>on</strong> is a binary chemical counter<br />

modulo 17 based <strong>on</strong> a cycle of five-bit states. Please note that the logical unit<br />

remains unchanged during the whole study. After providing the pool of modules,<br />

we explore the effect of different core oscillators <strong>on</strong> the behavioural pattern of the<br />

entire frequency divider system in the presence or absence of the binary signal<br />

separator. Although leaving intact the logical unit, we observe new frequency<br />

divisi<strong>on</strong> ratios of 1:3, 1:5, and 1:6 just by the effect of module assembly.<br />

3.1 Sketching the Pool of Individual Modules<br />

Taking into account a Brusselator, a Repressilator, and a Goodwin oscillator, we<br />

allow for a pool of core oscillators assumed to be formerly emerged independently<br />

from each other and based <strong>on</strong> different molecular mechanisms. Each individual<br />

module is c<strong>on</strong>sidered to be fixed including its previously chosen setting of kinetic<br />

parameters. For all simulati<strong>on</strong> studies carried out in this secti<strong>on</strong>, we utilise a<br />

c<strong>on</strong>sistent time unit.<br />

The Brusselator Module<br />

The Brusselator derived from the Belousov-Zhabotinsky reacti<strong>on</strong> is a tool approved<br />

for the generati<strong>on</strong> of spiking oscillati<strong>on</strong>s forming a limit cycle [1, 28]. Here,<br />

the oscillatory persistence is exclusively reached by a positive feedback effect of<br />

an autocatalytic loop. The n<strong>on</strong>-probabilistic P module brusselator = (∅, {S},F)<br />

is completely based <strong>on</strong> mass-acti<strong>on</strong> kinetics captured by five ODEs in F :<br />

P ˙ = −k 1 PT; ˙Q = −k 3 Q; Ṡ = k 1 PT − k 2 ST 2 ; T ˙ = −k 1 PT + k 2 ST 2 +<br />

k 3 Q−k 4 T ; Ẇ = k 4 T . Figure 1 depicts the underlying topology of the reacti<strong>on</strong><br />

network in c<strong>on</strong>juncti<strong>on</strong> with the selected parameter setting. Reacti<strong>on</strong> velocities,<br />

particularly those of decay T −→ k4<br />

W producing waste W ,mainlydeterminethe<br />

oscillati<strong>on</strong> frequency. Our parameter setting avoids a transient phase and enables<br />

a lower frequency oscillati<strong>on</strong> with distinctive spikes.<br />

228

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