“…However, the presence of the cross-links or/and the nonideal structure of the APCN building blocks lead to the formation of frustrated/distorted morphologies, with much less regularity than the morphologies observed with (non-cross-linked) linear block copolymers . Thus, the APCN electron micrographs or atomic force micrographs usually exhibit morphologies with spheroidal domains, and the corresponding small-angle X-ray scattering (SAXS) or small-angle neutron scattering (SANS) profiles present a single broad peak. − ,,− However, recent synthetic developments, involving sparser and more regular cross-linking, e.g., end-linking, as well as the utilization of near-ideal building blocks (well-defined linear or star polymers), resulted in APCN nanophase-separated morphologies of high regularity, e.g., wavy lamellae, and SAXS and SANS profiles with a number of higher order peaks. , The experimental recording of these more regular morphologies in self-assembled APCNs renders their modeling/simulation more worthwhile. In particular, current state-of-the-art simulations and self-consistent field theories (SCFT) very successfully reproduce the experimentally observed morphologies of linear diblock melts and are, consequently, expected to accurately predict the morphologies formed by APCNs comprising well-defined building blocks .…”