“…(3) is locally asymptotically stable when τ ∈ (0, τ 0λ ), and it is unstable when τ ∈ (τ 0λ , +∞); (iii) a Hopf bifurcation occurs at τ = τ nλ for (3) so that there is a continuous family of periodic orbits of (3) in form of {(τ n (s), u n (x, t, s), T n (s)) : s ∈ (0, δ 1 )} so that u n (x, t, s) is a T n (s)−periodic solution of (3) with τ = τ n (s), and τ n (0) = τ nλ , lim s→0 + u n (x, t, s) = u λ (x) and lim s→0 + T n (s) = 2π/ω λ . Next, by applying the method of Faria [11,12], the normal form of system (3) can be computed to determine the direction of the Hopf bifurcation proved in Theorem 2.7 and the stability of the periodic orbits.…”