“…Within the SCFT, the free energy functional of such a system is obtained as , where u 0 is the (Edwards) short-range excluded volume interaction, ϕ( r , θ) and ϕ* ( r , θ) are the dimensionless volume fractions of all and sticker monomers, respectively, ω( r , θ) is the auxiliary field that couples with the volume fraction ϕ( r , θ), ln(ζ/π R 2 ) is the translational entropy term, with ζ being the momentum part of the polymer partition function, and is the single-chain configurational partition function, which is defined by Using the saddle-point approximation, we can obtain a set of self-consistent equations for the density field and the auxiliary field. The crucial step corresponds to the numerical solution of these self-consistent equations in terms of the polymer chain propagator, q ( r , s ), i.e., the probability of finding the s th monomer of a polymer at r , which can be obtained by solving the modified diffusion equation with the initial condition q ( r , θ, s = 0) = 1, where s ∈ [0, N ] is the contour variable along the chain.…”