“…Define a global cross section Σ = s 1 , n 1 , s 2 , n 2 , t | t = 0 in the phase space 2 × 3 , and construct the m 0 -th iteration of Poincaré map P m 0 ∶ Σ → Σ as s 10 , n 10 , s 20 , n 20 → s 1 (m 0 T), n 1 (m 0 T), s 2 (m 0 T), n 2 (m 0 T) , where s i0 = s i (0), n i0 = n i (0) (i = 1, 2) are initial values. A fixed point of P m 0 corresponds to a periodic solution of system (11) T will be obtained as follows [32].…”