“…Each dye molecule described as TLS is characterized by its center of mass position (x i , y i , z i ), where the index i runs over all N such molecules, and by the orientation given by the unit vector n i along d. As emphasized in Ref. [1], it is important that this transition (S 0 → S 1 characterized by real matrix element d) is non-degenerate which leads to lowering the symmetry from O(4) to O(2)×Z 2 , and, thus, allows the condensation to occur in 2D geometry in the algebraic sense. At time scales longer than few ns the vector field n i becomes classical order parameter.…”