Quantum walk, a kind of systems with time-periodic driving (Floquet systems), is defined by a time-evolution operator, and can possess non-trivial topological phases. Recently, the stability of topologically protected edge states in a nonlinear quantum walk has been studied, in terms of an effective time-indepedent non-Hermitian Hamiltonian, by applying a continuum limit to the nonlinear quantum walk. In this paper, we study the stability of the edge states by treating a nonunitary time-evolution operator, which is derived from the time-evolution operator of nonlinear quantum walks without the continuum limit. As a result, we find additional bifurcations at which edge states change from stable attractors to unstable repellers with increasing the strength of nonlinearity. The additional bifurcation we shall show is unique to Floquet nonlinear systems, since the origin of the bifurcations is that a stable region for eigenvalues of nonunitary time-evolution operators is bounded, while that of effective non-Hermitian Hamiltonians is unbouneded.