pa_list_add:={ {"\pi", 0, -1, X, 1, -1, 0, 0, 1, 0.13957, 0.0001}, {"P", 1/2, +1, X, 1/2, X, 0, 1, 1, 0.93827, 0.0001}, {"n", 1/2, +1, X, 1/2, X, 0, 1, 0, 0.93957, 0.0001}, {"\rho[1900] ", 1, -1, X, 1, 1, 0, 0, 1, 1.91000, 0.1450}, {"\rho_3[1990] ", 3, -1, X, 1, 1, 0, 0, 1, 1.99000, 0.1800}, {"\rho[2150]", 1, -1, X, 1, 1, 0, 0, 1, 2.14900, 0.3630}, {"\rho_3[2250]", 3, -1, X, 1, 1, 0, 0, 1, 2.25000, 0.1750}, {"\rho_5[2350]", 5, -1, X, 1, 1, 0, 0, 1, 2.35000, 0.4000}, {"J/\psi", 1, -1, -1, 0, -1, 0, 0, 0, 3.09688, 0.0001}, {"N[1440]", 1/2, +1, X, 1/2, X, 0, 1, 1, 1.440, 0.350}, {"N[1520]", 3/2, -1, X, 1/2, X, 0, 1, 1, 1.520, 0.120}, {"N[1535]", 1/2, -1, X, 1/2, X, 0, 1, 1, 1.535, 0.150}, {"N[1650]", 1/2, -1, X, 1/2, X, 0, 1, 1, 1.650, 0.150}, {"N[1675]", 5/2, -1, X, 1/2, X, 0, 1, 1, 1.670, 0.140}, {"N[1680]", 5/2, +1, X, 1/2, X, 0, 1, 1, 1.680, 0.130}, {"N[1700]", 3/2, -1, X, 1/2, X, 0, 1, 1, 1.700, 0.100}, {"N[1710]", 1/2, +1, X, 1/2, X, 0, 1, 1, 1.710, 0.100}, {"N[1720]", 3/2, +1, X, 1/2, X, 0, 1, 1, 1.720, 0.150}, {"N[1900]", 3/2, +1, X, 1/2, X, 0, 1, 1, 1.900, 0.498}, {"N[1990]", 7/2, +1, X, 1/2, X, 0, 1, 1, 1.990, 0.380}, {"N[2000]", 5/2, +1, X, 1/2, X, 0, 1, 1, 2.000, 0.300}, {"N[2080]", 3/2, -1, X, 1/2, X, 0, 1, 1, 2.080, 0.270}, {"N[2090]", 1/2, -1, X, 1/2, X, 0, 1, 1, 2.090, 0.300}, {"N[2100]", 1/2, +1, X, 1/2, X, 0, 1, 1, 2.100, 0.260}, {"\Delta[1232][+1]", 3/2, +1, X, 3/2, X, 0, 1, +1, 1.232, 0.120}, {"\Delta[1232][0] ", 3/2, +1, X, 3/2, X, 0, 1, 0, 1.232, 0.120}, {"\Delta[1600][+1]", 3/2, +1, X, 3/2, X, 0, 1, +1, 1.600, 0.350}, {"\Delta[1600][0] ", 3/2, +1, X, 3/2, X, 0, 1, 0, 1.600, 0.350}, {"\Delta[1620][+1]", 1/2, -1, X, 3/2, X, 0, 1, +1, 1.620, 0.150}, {"\Delta[1620][0] ", 1/2, -1, X, 3/2, X, 0, 1, 0, 1.620, 0.150}, {"\Delta[1700][+1]", 3/2, -1, X, 3/2, X, 0, 1, +1, 1.700, 0.300}, {"\Delta[1700][0] ", 3/2, -1, X, 3/2, X, 0, 1, 0, 1.700, 0.300}, {"\Delta[1750][+1]", 1/2, +1, X, 3/2, X, 0, 1, +1, 1.750, 0.300}, {"\Delta[1750][0] ", 1/2, +1, X, 3/2, X, 0, 1, 0, 1.750, 0.300}, {"\Delta[1900][+1]", 1/2, -1, X, 3/2, X, 0, 1, +1, 1.900, 0.200}, {"\Delta[1900][0] ", 1/2, -1, X, 3/2, X, 0, 1, 0, 1.900, 0.200}, {"\Delta[1905][+1]", 5/2, +1, X, 3/2, X, 0, 1, +1, 1.905, 0.350}, {"\Delta[1905][0] ", 5/2, +1, X, 3/2, X, 0, 1, 0, 1.905, 0.350}, {"\Delta[1910][+1]", 1/2, +1, X, 3/2, X, 0, 1, +1, 1.910, 0.250}, {"\Delta[1910][0] ", 1/2, +1, X, 3/2, X, 0, 1, 0, 1.910, 0.250}, {"\Delta[1920][+1]", 3/2, +1, X, 3/2, X, 0, 1, +1, 1.920, 0.200}, {"\Delta[1920][0] ", 3/2, +1, X, 3/2, X, 0, 1, 0, 1.920, 0.200}, {"\Delta[1930][+1]", 5/2, -1, X, 3/2, X, 0, 1, +1, 1.930, 0.350}, {"\Delta[1930][0] ", 5/2, -1, X, 3/2, X, 0, 1, 0, 1.930, 0.350}, {"\Delta[1940][+1]", 3/2, -1, X, 3/2, X, 0, 1, +1, 1.940, 0.330}, {"\Delta[1940][0] ", 3/2, -1, X, 3/2, X, 0, 1, 0, 1.940, 0.330}, {"\Delta[1950][+1]", 7/2, +1, X, 3/2, X, 0, 1, +1, 1.950, 0.300}, {"\Delta[1950][0] ", 7/2, +1, X, 3/2, X, 0, 1, 0, 1.950, 0.300}, {"\Delta[2000][+1]", 5/2, +1, X, 3/2, X, 0, 1, +1, 2.000, 0.325}, {"\Delta[2000][0] ", 5/2, +1, X, 3/2, X, 0, 1, 0, 2.000, 0.325}, {"\Delta[2150][+1]", 1/2, -1, X, 3/2, X, 0, 1, +1, 2.150, 0.160}, {"\Delta[2150][0] ", 1/2, -1, X, 3/2, X, 0, 1, 0, 2.150, 0.160} }; 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;