“We can also see that the weights are divided by a factor of two, which accounts for the typical 5× factor separating the lower and upper weight window bounds in OpenMC”.
I suppose that it is based on the fact of 2 * 2 is almost 5, so the WW interval [f(r) / 2, f(r) * (5 / 2)]
is almost log-symmetrical regarding to the central value of relative flux f(r) = ϕ(r) / max_r(ϕ(r)).
The major principle of both MAGIC and FW-CADIS is based on the assumption of the optimal splitting rate for transition from point r_1 to point r_2 is approximately proportional to product of the statistical weight w and ratio of their flux densities [1]: w * ϕ(r_1) / ϕ(r_2). Sometimes, it is close to the truth.
References
1 . Cooper, M. A., & Larsen, E. W. (2001). Automated Weight Windows for Global Monte Carlo Particle Transport Calculations. Nuclear Science and Engineering, 137(1), 1–13. https://doi.org/10.13182/NSE00-34