“…Therefore, recall that away from the LCS point, the periods of the holomorphic (3, 0)-form Ω receive corrections from their flat values, namely [70,151] z j ′ = 1 2πi log x j + O(x i ) , (B.37) such that upon increasing x i towards one, the logarithmic approximation for z i ′ stops being valid and the polynomial corrections clearly dominate. Hence, instead of reaching a point where Im z i ′ → 0 asymptotically, what happens is that the complex structure variables generically approach some constant O(1) value (see e.g., [75,164,165]). This does not prevent, on the other hand, the R coordinate from keep flowing towards weak coupling, such that a more accurate parametrization of the asymptotic trajectory would be the following:…”