“…In spite of being a non-specific model of polymer dynamics, the BFM was successfully used to study a large variety of physical effects in two- and three dimensions like, e.g., static [ 18 , 19 , 20 , 21 , 22 , 23 , 24 , 25 , 26 , 27 , 28 , 29 ] and dynamic [ 18 , 30 , 31 , 32 , 33 ] properties of linear chains, polymer rings [ 27 , 34 ], polymer blends and interfaces [ 35 , 36 ], gels and networks [ 37 ], glass transition [ 38 , 39 , 40 ], polymer blends [ 41 ], (co)polymers at surfaces [ 42 ], polymer brushes in good solvents [ 43 , 44 , 45 , 46 , 47 , 48 , 49 ], polymer thin films [ 50 , 51 , 52 ], equilibrium polymers [ 29 , 53 , 54 ], general self-assembly [ 55 , 56 , 57 ], networks and gel point [ 58 , 59 , 60 , 61 ], olympic gels [ …”