“…Modeling thermally-activated flow and non-Schmid effects in bcc systems has been the subject of much work, starting in the 1980s and, particularly, in recent times. Different authors have considered different subsets of the t110u, t112u, and t123u families of glide planes, without (Raphanel & Van Houtte, 1985;Hölscher et al, 1991Hölscher et al, , 1994Raabe et al, 1994;Raabe, 1995a,b;Peeters et al, 2000;Stainier et al, 2002;Erieau & Rey, 2004;Ma et al, 2007;Hamelin et al, 2011;Kitayama et al, 2013) and with non-Schmid effects (Lee et al, 1999;Kuchnicki et al, 2008;Koester et al, 2012;Weinberger et al, 2012;Alankar et al, 2014;Lim et al, 2013;Narayanan et al, 2014;Patra et al, 2014;Knezevic et al, 2014;Lim et al, 2015a,b). Of particular interest are some recent simulations where the flow rule is directly formulated on the basis of screw dislocation properties in Fe (Yalcinkaya et al, 2008;Koester et al, 2012;Alankar et al, 2014;Narayanan et al, 2014;Patra et al, 2014;Lim et al, 2015b), Ta (Kuchnicki et al, 2008;Lim et al, 2013;Knezevic et al, 2014;Lim et al, 2015a), Mo (Yalcinkaya et al, 2008;Weinberger et al, 2012;Lim et al, 2013Lim et al, , 2015a, W (Lee et al, 1999;Weinberger et al, 2012;Lim et al, 2013;…”