Figure 4 | Scientific Reports

Figure 4

From: A phase-field model by an Ising machine and its application to the phase-separation structure of a diblock polymer

Figure 4

Temporal change until equilibrium is reached by the quantum annealing simulator in the case of \(f=0.3\) (a) without Ohta-Kawasaki energy and (b) with Ohta-Kawasaki energy. As for the results obtained by the conventional phase-field analysis, the stronger the Ohta-Kawasaki energy becomes, the finer the microstructure at the equilibrium state. Without Ohta-Kawasaki energy, all the microstructures equilibrate as two large phases.

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