pa_list_add:={ {"\eta", 0, -1, 1, 0, 1, 0, 0, 0, 0.54730, 0.0001}, {"n", 1/2, +1, X, 1/2, X, 0, 1, 0, 0.93957, 0.0001}, {"f_2[1910]", 2, 1, 1, 0, 1, 0, 0, 0, 1.91500, 0.1630}, {"f_2[1950]", 2, 1, 1, 0, 1, 0, 0, 0, 1.93400, 0.4530}, {"f_2[2010]", 2, 1, 1, 0, 1, 0, 0, 0, 2.01100, 0.2020}, {"f_0[2020]", 0, 1, 1, 0, 1, 0, 0, 0, 2.02000, 0.4100}, {"f_4[2050]", 4, 1, 1, 0, 1, 0, 0, 0, 2.02500, 0.1940}, {"f_0[2100]", 0, 1, 1, 0, 1, 0, 0, 0, 2.10000, 0.2010}, {"f_2[2150]", 2, 1, 1, 0, 1, 0, 0, 0, 2.13800, 0.1940}, {"f_0[2200]", 0, 1, 1, 0, 1, 0, 0, 0, 2.19700, 0.2010}, {"f_2[2300]", 2, 1, 1, 0, 1, 0, 0, 0, 2.29700, 0.1490}, {"f_4[2300]", 4, 1, 1, 0, 1, 0, 0, 0, 2.30000, 0.2150}, {"f_0[2330]", 0, 1, 1, 0, 1, 0, 0, 0, 2.33000, 0.2170}, {"f_2[2340]", 2, 1, 1, 0, 1, 0, 0, 0, 2.33900, 0.3190}, {"\eta_{c}[2980]",0, -1, 1, 0, 1, 0, 0, 0, 2.97920, 0.013}, {"\Delta[1600][0] ", 3/2, +1, X, 3/2, X, 0, 1, 0, 1.600, 0.350}, {"\Delta[1620][0] ", 1/2, -1, X, 3/2, X, 0, 1, 0, 1.620, 0.150}, {"\Delta[1700][0] ", 3/2, -1, X, 3/2, X, 0, 1, 0, 1.700, 0.300}, {"\Delta[1750][0] ", 1/2, +1, X, 3/2, X, 0, 1, 0, 1.750, 0.300}, {"\Delta[1900][0] ", 1/2, -1, X, 3/2, X, 0, 1, 0, 1.900, 0.200}, {"\Delta[1905][0] ", 5/2, +1, X, 3/2, X, 0, 1, 0, 1.905, 0.350}, {"\Delta[1910][0] ", 1/2, +1, X, 3/2, X, 0, 1, 0, 1.910, 0.250}, {"\Delta[1920][0] ", 3/2, +1, X, 3/2, X, 0, 1, 0, 1.920, 0.200}, {"\Delta[1930][0] ", 5/2, -1, X, 3/2, X, 0, 1, 0, 1.930, 0.350}, {"\Delta[1940][0] ", 3/2, -1, X, 3/2, X, 0, 1, 0, 1.940, 0.330}, {"\Delta[1950][0] ", 7/2, +1, X, 3/2, X, 0, 1, 0, 1.950, 0.300}, {"\Delta[2000][0] ", 5/2, +1, X, 3/2, X, 0, 1, 0, 2.000, 0.325} }; phase_method:='real_coefficient; direct_model:='ok; final_particle_list:='("P" "n" "\pi" "K" "\eta" "\pi^0" "K^0" "\gamma" "\eta^{'}[958]"); vertices_add_comment:='"In this model, We have added some effective vertices, to do some calculation related to some resonance states"; end;