On Two-Ridge Structure in Two-Particle Azimuthal Correlations in Proton-Lead Collisions at Large Hadron Collider Energy

Table 1

Values of parameters and 𝜒²/dof corresponding to the curves in Figures 1–3.

Figures	Type	𝑎𝑥	𝑏𝑥	𝑐1(𝑐2)	𝑏0	𝜒^2/dof
Figure 1(a)	0–20%, ℎ−𝜋	1.045±0.002	−0.020±0.002	1.197±0.012	—	0.872
Figure 1(b)	(0–20%)–(60–100%), ℎ−𝜋	1.040±0.002	−0.005±0.001	0.915±0.010	—	1.129
Figure 1(c)	(0–20%)–(60–100%), ℎ−𝑝	1.030±0.002	−0.003±0.001	0.208±0.002	—	1.105
Figure 2(a)	0.3<𝑝^𝑎𝑇<0.5 GeV/c, 𝐶	1.040±0.002	−0.024±0.002	16.498±0.172	−2.528±0.026	1.051
Figure 2(b)	0.5<𝑝^𝑎𝑇<1 GeV/c, 𝐶	1.040±0.002	−0.020±0.002	25.146±0.310	−3.840±0.040	0.595
Figure 2(c)	1<𝑝^𝑎𝑇<2 GeV/c, 𝐶	1.040±0.002	−0.019±0.002	40.516±0.422	−6.200±0.065	0.470
Figure 2(d)	2<𝑝^𝑎𝑇<3 GeV/c, 𝐶	1.040±0.002	−0.020±0.002	60.233±0.650	−9.230±0.096	0.282
Figure 2(e)	3<𝑝^𝑎𝑇<4 GeV/c, 𝐶	1.040±0.002	−0.025±0.003	66.202±0.680	−10.100±0.105	0.356
Figure 2(f)	4<𝑝^𝑎𝑇<5 GeV/c, 𝐶	1.040±0.002	−0.029±0.003	69.403±0.710	−10.600±0.110	0.819
Figure 2(a)	0.3<𝑝^𝑎𝑇<0.5 GeV/c, 𝑃	1.010±0.001	−0.045±0.005	7.540±0.080	−1.145±0.012	0.755
Figure 2(b)	0.5<𝑝^𝑎𝑇<1 GeV/c, 𝑃	1.010±0.001	−0.035±0.004	14.363±0.145	−2.215±0.024	1.322
Figure 2(c)	1<𝑝^𝑎𝑇<2 GeV/c, 𝑃	1.012±0.001	−0.030±0.003	27.830±0.303	−4.315±0.045	1.101
Figure 2(d)	2<𝑝^𝑎𝑇<3 GeV/c, 𝑃	1.013±0.001	−0.030±0.003	45.741±0.470	−7.100±0.072	0.575
Figure 2(e)	3<𝑝^𝑎𝑇<4 GeV/c, 𝑃	1.013±0.001	−0.030±0.003	60.354±0.630	−9.360±0.095	1.634
Figure 2(f)	4<𝑝^𝑎𝑇<5 GeV/c, 𝑃	1.013±0.001	−0.025±0.003	86.098±0.900	−13.390±0.135	1.903
Figure 3(a)	0.3<𝑝^𝑎𝑇<0.5 GeV/c, 𝐶−𝑃	1.040±0.002	−0.006±0.001	12.533±0.122	−1.950±0.020	1.808
Figure 3(b)	0.5<𝑝^𝑎𝑇<1 GeV/c, 𝐶−𝑃	1.040±0.002	0.000±0.000	21.923±0.220	−3.400±0.037	0.938
Figure 3(c)	1<𝑝^𝑎𝑇<2 GeV/c, 𝐶−𝑃	1.040±0.002	0.000±0.000	32.036±0.332	−4.950±0.051	0.912
Figure 3(d)	2<𝑝^𝑎𝑇<3 GeV/c, 𝐶−𝑃	1.040±0.002	0.002±0.001	42.163±0.405	−6.520±0.066	0.353
Figure 3(e)	3<𝑝^𝑎𝑇<4 GeV/c, 𝐶−𝑃	1.040±0.002	0.004±0.001	50.203±0.527	−7.790±0.080	1.074
Figure 3(f)	4<𝑝^𝑎𝑇<5 GeV/c, 𝐶−𝑃	1.040±0.002	0.002±0.001	40.485±0.500	−6.280±0.065	1.278