2(1670).
The following four plots are what the weights would look like for the
four waves for a narrow bin near the peak of the a2(1320).
(Note: There is no resonance shape imposed in the fit).
In order to generate the above weights, we have used the following camp
file, where for the above plots we have only turned on the corresponding
production strengths, V_(JPC)(M epsilon). Something rather interesting is
how the
(770)
appears washed out in the 1+- data set. It is also striking
how the
distribution
can help select out different naturalities of the final state particle,
particularly for the
+
distributions versus
GJ.
The Dalitz plots for these four are shown below.
1++
2++
1-+
2-+
Given below is the simple camp file that produces the distributions.
rmat gen1_bin1.denmat;
damp 2++1+.ramps;
damp 1-+1+nsym.amps;
complex Rpos;
complex V_2++1+ ;
event_loop:
V_2++1+ = (1,1);
Rpos = V_1-+1+ * 1-+1+nsym.amps + V_1++1+ * 1++1+.ramps +
Rneg = V_1-+1- * 1-+1-nsym.amps + V_1++1- * 1++1-.ramps +
wt = ( absSq( Rpos ) * gen1_bin1.denmat[0 , 0] +
damp 2++1-.ramps;
damp 1++1+.ramps;
damp 1++1-.ramps;
damp 2-+1+.ramps;
damp 2-+1-.ramps;
damp 1-+1+.ramps;
damp 1-+1-.ramps;
damp 1-+1-nsym.amps;
complex Rneg;
complex V_2++1- ;
complex V_1++1+ ;
complex V_1++1- ;
complex V_2-+1+ ;
complex V_2-+1- ;
complex V_1-+1+ ;
complex V_1-+1- ;
V_2++1- = (1,1);
V_1++1+ = (2,2);
V_1++1- = (2,2);
V_2-+1+ = (0,0);
V_2-+1- = (0,0);
V_1-+1+ = (0,0);
V_1-+1- = (0,0);
V_2-+1+ * 2-+1+.ramps + V_2++1+ * 2++1+.ramps ;
V_2-+1- * 2-+1-.ramps + V_2++1- * 2++1-.ramps ;
absSq( Rneg ) * gen1_bin1.denmat[1 , 1] );