pa_list_add:={ {"\eta", 0, -1, 1, 0, 1, 0, 0, 0, 0.54730, 0.0001}, {"K", 0, -1, X, 1/2, X, -1, 0, 1, 0.49368, 0.0001}, {"f_2[1270]", 2, 1, 1, 0, 1, 0, 0, 0, 1.27500, 0.1855}, {"f_0[1370]", 0, 1, 1, 0, 1, 0, 0, 0, 1.37000, 0.3500}, {"f_2[1430]", 2, 1, 1, 0, 1, 0, 0, 0, 1.43000, 0.0810}, {"f^{'}_2[1525]", 2, 1, 1, 0, 1, 0, 0, 0, 1.52500, 0.0760}, {"f_2[1565]", 2, 1, 1, 0, 1, 0, 0, 0, 1.54200, 1.1310}, {"f_2[1640]", 2, 1, 1, 0, 1, 0, 0, 0, 1.63800, 0.0990}, {"f_0[1710]", 0, 1, 1, 0, 1, 0, 0, 0, 1.71200, 0.1330}, {"f_2[1810]", 2, 1, 1, 0, 1, 0, 0, 0, 1.81500, 0.1970}, {"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}, {"K^{*}[1410]", 1, -1, X, 1/2, X, -1, 0, 1, 1.41400, 0.232}, {"K^{*}_2[1980]", 2, 1, X, 1/2, X, -1, 0, 1, 1.97300, 0.373}, {"\eta_{c}[2980]",0, -1, 1, 0, 1, 0, 0, 0, 2.97920, 0.013} }; 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;