“…Fully drift-implicit Euler schemes can, however, often only be simulated approximatively as a nonlinear equation has to be solved in each time step and the resulting approximations of the fully drift-implicit Euler approximations require additional computational effort (particularly, when the state space of the considered SEE is high dimensional, see, e.g., Figure 4 in Hutzenthaler et al [20]) and have not yet been shown to converge strongly. Recently, a series of explicit and easily implementable timediscrete approximation schemes have been proposed and shown to converge strongly in the case of SEEs with superlinearly growing nonlinearities; see, e.g., Hutzenthaler et al [20], Wang & Gan [45], Hutzenthaler & Jentzen [18], Tretyakov & Zhang [44], Halidias [13], Sabanis [39,40], Halidias & Stamatiou [15], Hutzenthaler et al [22], Szpruch & Zhāng [42], Halidias [14], Liu & Mao [30], Hutzenthaler & Jentzen [17], Zhang [46], Dareiotis et al [10], Kumar & Sabanis [27], Beyn et al [1], Zong et al [47], Song et al [41], Ngo & Luong [36], Tambue & Mukam [43], Mao [34], Beyn et al [2], Kumar & Sabanis [28], and Mao [35] in the case of finite dimensional SEEs and see, e.g., Gyöngy et al [12] and Jentzen & Pušnik [25] in the case of infinte dimensional SEEs. These schemes are suitable modified versions of the explicit Euler scheme that somehow tame/truncate the superlinearly growing nonlinearities of the considered SEE and thereby prevent the considered tamed scheme from strong divergence.…”