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Figure 1.

Stable stationary spot arrays in the reaction-diffusion system (1) generated by (a) Turing instability, (b) replication cascade.

Two space dimensions are considered, with system size and periodic boundary conditions. Typical formation pathways for the Turing case (c) and the replication scenario (d) are shown in the space-time diagrams for simulations in one-dimensional space with . In (a–d), the variable is displayed in color code: red, respectively white denote large values. Parameters: (a) ; (b) ; (c) , displayed time interval , (d) , displayed time interval . Other parameters as in Fig. 2. A pattern profile for both variables and will be shown in Fig. 4(b).

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Figure 1 Expand

Figure 2.

Stability area for -spot arrays as a function of for a system size with periodic boundary conditions and (details of simulation are covered in Methods).

The stability area is enclosed by the curves and , corresponding to the maximum and minimum number of stable spots for a given . is changed in steps of using the asymptotic state of the previous as initial condition (ramping). Turing patterns are marked by the curve . Vertical lines correspond to the values for the instabilities: , , , .

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Figure 2 Expand

Figure 3.

Different pattern pathways.

(a) The red and blue pathways represent a hysteresis curve for an example -spot array induced in state 1. We observe a sequence spots. The green path represents a cycle between 10 and 20 spots (more see text). (b) Space-time diagram for along the green path shown in (a). is changed about each . Simulation starts with a 10-spot solution at with , and increases until , where splitting is observed. Then is decreased until , where 10 spots disappear, and after which it is increased again until is reached.

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Figure 3 Expand

Figure 4.

Pattern profiles.

(a) The profile of in a Turing pattern as a function of for fixed . The blue curve represents the steady-state value . The vertical dashed lines and mark the Turing regime. A Turing pattern appears supercritically at (inset) and its amplitude increases as one moves away from threshold. At a certain point, the profile ceases to oscillate around , and continues to exist beyond the Turing regime without qualitative changes. (b) Multiple -spot profiles in space, for between at (blue curve) and at (red curve). The insets show the corresponding concentration profiles (black is , red is ).

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Figure 4 Expand