pa_list_add:={
{"\eta",          0,  -1,   1,  0,    1,   0,    0,    0,  0.54730, 0.0001},
{"P",   	  1/2, +1,  X,  1/2,  X,   0,	  1,   1,  0.93827, 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},  
{"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},
{"\Delta[1600][+1]",   3/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.600,   0.350},
{"\Delta[1620][+1]",   1/2, -1,  X,  3/2,  X,   0,     1,   +1,  1.620,   0.150},
{"\Delta[1700][+1]",   3/2, -1,  X,  3/2,  X,   0,     1,   +1,  1.700,   0.300},
{"\Delta[1750][+1]",   1/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.750,   0.300},
{"\Delta[1900][+1]",   1/2, -1,  X,  3/2,  X,   0,     1,   +1,  1.900,   0.200},
{"\Delta[1905][+1]",   5/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.905,   0.350},
{"\Delta[1910][+1]",   1/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.910,   0.250},
{"\Delta[1920][+1]",   3/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.920,   0.200},
{"\Delta[1930][+1]",   5/2, -1,  X,  3/2,  X,   0,     1,   +1,  1.930,   0.350},
{"\Delta[1940][+1]",   3/2, -1,  X,  3/2,  X,   0,     1,   +1,  1.940,   0.330},
{"\Delta[1950][+1]",   7/2, +1,  X,  3/2,  X,   0,     1,   +1,  1.950,   0.300},
{"\Delta[2000][+1]",   5/2, +1,  X,  3/2,  X,   0,     1,   +1,  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;