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. Author manuscript; available in PMC: 2025 Apr 28.
Published in final edited form as: Phys Rev Res. 2023 Dec 22;5(4):physrevresearch.5.043281. doi: 10.1103/PhysRevResearch.5.043281

Fig. 8.

Fig. 8

The ratio of the heterogeneous mean exit time En0 to the homogeneous mean exit time ℰn0 for randomly distributed barriers and antibarriers. We use a homogeneous propagator with a domain of size N = (51, 51) with absorbing boundary conditions, an initial condition at the center of the domain n0 = (26, 26) and a diffusion parameter of q = (0.8, 0.8). The explicit form of φ˜n0(n,z) is given by the z transform of Eq. (23) of Ref. [68]. Each curve is obtained using Eq. (10) and performing an ensemble average with 102 sample realizations of locations of barriers (λ > 0) or antibarriers (λ > 0) for each λ.