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13th International Conference on Membrane Computing - MTA Sztaki

13th International Conference on Membrane Computing - MTA Sztaki

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

We parameterise the Repressilator in a way to exhibit a medium frequency limit<br />

cycle oscillati<strong>on</strong> emphasising a comparatively small amplitude in c<strong>on</strong>cert with<br />

small signal values not exceeding a threshold of approximately 0.6, see Figure<br />

2. This threshold is meant to coincide with the ambiguous “forbidden range” in<br />

terms of a clear distincti<strong>on</strong> between 0 and 1 of binarily interpreted signals.<br />

The Goodwin Module<br />

The Goodwin oscillator follows the scheme of a three-staged cyclic gene regulatory<br />

network c<strong>on</strong>sisting of two subsequent activating transiti<strong>on</strong>s al<strong>on</strong>g with<br />

a single inhibiti<strong>on</strong> completing the loop by a negative feedback [12]. According<br />

to the internal balance of reacti<strong>on</strong> velocities, the resulting oscillatory waveform<br />

might vary from an almost sinusoidal behaviour towards an asymmetric λ-like<br />

shape. Here, a fast growing edge is combined with a slightly sigmoidal diminishment<br />

of the signal. This makes the Goodwin oscillator a promising candidate<br />

for naturally plated limit cycle oscillati<strong>on</strong>s. The n<strong>on</strong>-probabilistic P module<br />

goodwin = (∅, {X},F) c<strong>on</strong>taining three ODEs<br />

Ẋ =<br />

H<br />

1+Z 9 − k 4X Ẏ = k 1 X − k 5 Y Ż = k 2 Y − k 6 Z<br />

defines the Goodwin oscillator in its original form [12]. The degradati<strong>on</strong> velocities<br />

most significantly determine its oscillatory frequency. Our c<strong>on</strong>figurati<strong>on</strong><br />

shown in Figure 3 is focused <strong>on</strong> a lower frequency oscillati<strong>on</strong> of a high amplitude<br />

spanned by signal values altering between approx. 0.6 and2.5. In c<strong>on</strong>trast<br />

to the Repressilator’s parameterisati<strong>on</strong>, we intend to face the binarily operating<br />

signal postprocessing units with intense signals revealing high values for a<br />

comparatively l<strong>on</strong>ger amount of time.<br />

Fig. 3. Goodwin oscillator reacti<strong>on</strong> network (left) in its original form. We assume the<br />

c<strong>on</strong>centrati<strong>on</strong> course of species X over time (right) to act as module output. Higherorder<br />

Hill kinetic’s parameter setting H =1.5,k i =0.05 for i ∈{1,...,6} chosen<br />

to maintain slightly plated oscillati<strong>on</strong>s whose amplitude enables signal values between<br />

approx. 0.6 and 2.5; initial c<strong>on</strong>centrati<strong>on</strong>s: X(0) = 1.0,Y(0) = 1.6,Z(0) = 1.7<br />

230

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