Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 718.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 723.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 727.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 731.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 735.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 739.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 743.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 748.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 752.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 756.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 760.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 768.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 772.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 777.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 781.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 785.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 789.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 793.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 797.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 801.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 805.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 809.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 814.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 818.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 822.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 826.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 830.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 834.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 838.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 842.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 846.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 850.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 854.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 858.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 862.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 866.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 870.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 874.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 878.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 882.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 886.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 890.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 894.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 898.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 902.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 906.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 910.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.3 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 914.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 918.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 922.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 926.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 930.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 933.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 937.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 941.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 945.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 949.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 953.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 957.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 960.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 964.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 968.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 972.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 976.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 980.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 983.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 987.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 991.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 995.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 998.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1002.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.4 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1006.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1011.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1019.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1026.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1034.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1041.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1048.6 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1055.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1063.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1070.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1077.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1084.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1091.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1098.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1105.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1112.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1119.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1125.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1132.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.5 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1139.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1146.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1152.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1159.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1165.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1172.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1178.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1185.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1191.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1198.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1204.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1210.5 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1216.7 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1222.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1229.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.6 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1235.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1242.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1251.3 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1260.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.8 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1268.9 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1277.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1287.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.7 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1300.0 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.9 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1315.1 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.8 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1335.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.8 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1355.4 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.8 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1376.2 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 4.9 PCT.

Differential cross section for the reaction GAMMA P --> ETA P at a photon energy of 1394.8 MeV. The errors in the table are statistical only and there is an overall systematic uncertainty of 5.0 PCT.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.72 to 1.73 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.73 to 1.74 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.74 to 1.75 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.75 to 1.76 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.76 to 1.77 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.77 to 1.78 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.78 to 1.79 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.79 to 1.8 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.8 to 1.81 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.81 to 1.82 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.82 to 1.83 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.83 to 1.84 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.84 to 1.85 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.85 to 1.86 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.86 to 1.87 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.87 to 1.88 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.88 to 1.89 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.89 to 1.9 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.9 to 1.91 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.91 to 1.92 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.92 to 1.93 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.93 to 1.94 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.94 to 1.95 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.96 to 1.97 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.97 to 1.98 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.98 to 1.99 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 1.99 to 2 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2 to 2.01 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.01 to 2.02 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.02 to 2.03 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.03 to 2.04 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.04 to 2.05 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.05 to 2.06 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.06 to 2.07 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.07 to 2.08 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.08 to 2.09 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.09 to 2.1 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.1 to 2.11 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.11 to 2.12 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.12 to 2.13 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.13 to 2.14 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.14 to 2.15 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.15 to 2.16 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.16 to 2.17 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.17 to 2.18 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.18 to 2.19 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.19 to 2.2 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.2 to 2.21 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.21 to 2.22 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.22 to 2.23 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.23 to 2.24 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.24 to 2.25 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.25 to 2.26 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.26 to 2.27 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.27 to 2.28 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.28 to 2.29 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.29 to 2.3 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.3 to 2.31 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.31 to 2.32 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.32 to 2.33 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.33 to 2.34 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.34 to 2.35 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.35 to 2.36 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.36 to 2.37 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.37 to 2.38 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.38 to 2.39 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.39 to 2.4 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.4 to 2.41 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.41 to 2.42 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.42 to 2.43 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.43 to 2.44 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.44 to 2.45 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.45 to 2.46 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.46 to 2.47 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.47 to 2.48 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.48 to 2.49 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.49 to 2.5 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.5 to 2.51 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.51 to 2.52 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.52 to 2.53 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.53 to 2.54 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.54 to 2.55 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.55 to 2.56 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.56 to 2.57 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.57 to 2.58 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.58 to 2.59 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.59 to 2.6 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.6 to 2.61 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.61 to 2.62 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.62 to 2.63 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.63 to 2.64 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.64 to 2.65 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.65 to 2.66 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.66 to 2.67 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.67 to 2.68 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.68 to 2.69 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.69 to 2.7 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.7 to 2.71 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.71 to 2.72 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.72 to 2.73 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.75 to 2.76 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.76 to 2.77 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.77 to 2.78 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.78 to 2.79 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.79 to 2.8 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.8 to 2.81 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.81 to 2.82 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.82 to 2.83 GeV.

Differential cross section as a function of COS(THETA(K+,CM)) for the centre-of mass range 2.83 to 2.84 GeV.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.95 to -0.85.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.85 to -0.75.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.75 to -0.65.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.65 to -0.55.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.55 to -0.45.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.45 to -0.35.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.35 to -0.25.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.25 to -0.15.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.15 to -0.05.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.05 to 0.05.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.05 to 0.15.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.15 to 0.25.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.25 to 0.35.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.35 to 0.45.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.45 to 0.55.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.55 to 0.65.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.65 to 0.75.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.75 to 0.85.

Differential cross section as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.85 to 0.95.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.85 to -0.75.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.75 to -0.65.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.65 to -0.55.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.55 to -0.45.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.45 to -0.35.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.35 to -0.25.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.25 to -0.15.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.15 to -0.05.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from -0.05 to 0.05.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.05 to 0.15.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.15 to 0.25.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.25 to 0.35.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.35 to 0.45.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.45 to 0.55.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.55 to 0.65.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.65 to 0.75.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.75 to 0.85.

Recoil polarization as a function of the centre-of-mass energy for the angular range COS(THETA(K+,CM) from 0.85 to 0.95.

Breakdown of syst. uncertainties (fully bin-by-bin correlated) for differential cross section for $e^+e^-\rightarrow\pi^+\pi^-\gamma$, with $50^o<\theta_\gamma<130^o$

Bare cross section for $e^+e^-\rightarrow\pi^+\pi^-$

Statistical covariance matrix for bare cross section for $e^+e^-\rightarrow\pi^+\pi^-$

Inverse statistical covariance matrix for bare cross section for $e^+e^-\rightarrow\pi^+\pi$

Breakdown of syst. uncertainties (fully bin-by-bin correlated) for the cross section for $e^+e^-\rightarrow\pi^+\pi^-$

Pion form factor $|F_\pi|^2$

Statistical covariance matrix for pion form factor $|F_\pi|^2$

Inverse statistical covariance matrix $|F_\pi|^2$

Breakdown of syst. uncertainties (fully bin-by-bin correlated) for the pion form factor $|F_\pi|^2$

Vacuum polarisation correction $\delta_{VP}(s)=(\frac{\alpha_{em}(s)}{\alpha_{em}(0)})^2$, with $\sigma^{bare} = \sigma^{dressed}/\delta$ - calculated using the routine from F.Jegerlehner: https://web.archive.org/web/20170828074416/http://www-com.physik.hu-berlin.de/~fjeger/alphaQEDn.uu (2003, archived on August 28, 2017)

Final State Radiation correction $(1.+\eta_{FSR}(s))$, evaluated using the formula in Eur. Phys. J. C 24, 51-69 (2002)

The differential radiator function cross section $H(M_{\pi\pi}^2,s)\cdot \frac{\pi \alpha^2 \beta_\pi^3}{3 M_{\pi\pi}^2 s}$, inclusive in $\theta_\gamma$, in bins of 0.01 GeV$^2$ in $M_{\pi\pi}^2$. The value used for $s$ in the Monte Carlo production is $s = 999.85\; GeV^2$, corresponding to the mean value of DA$\Phi$NE energy for data collected in 2006. Obtained with the PHOKHARA5 MC generator, see Eur. Phys. J. C 27, 563 (2003) and https://looptreeduality.csic.es/phokhara/phokhara5.0.tar.gz

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of moments of $\Delta N_p$ distributions for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions from Lattice QCD Calculations.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 19.6 GeV from Transport Model Calculations.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 62.4 GeV from Transport Model Calculations.

Centrality dependence of $S\sigma$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations for net-baryon.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations for net-proton (No Decay).

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

Centrality dependence of $\kappa\sigma^2$ for $\Delta N_p$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from Transport Model Calculations.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are STAR data.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are from UrQMD net-proton.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are from AMPT default net-proton.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are from AMPT String Melting net-proton.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are from Therminator net-proton.

$\sqrt{s_{NN}}$ dependence of $\kappa\sigma^2$ for net proton distributions measured at RHIC. The results are from Hijing net-proton.

Photon beam asymmetry at incident photon energy 1.031 GeV.

Photon beam asymmetry at incident photon energy 1.064 GeV.

Photon beam asymmetry at incident photon energy 1.097 GeV.

Photon beam asymmetry at incident photon energy 1.130 GeV.

Photon beam asymmetry at incident photon energy 1.163 GeV.

Photon beam asymmetry at incident photon energy 1.196 GeV.

Photon beam asymmetry at incident photon energy 1.229 GeV.

Photon beam asymmetry at incident photon energy 1.262 GeV.

Photon beam asymmetry at incident photon energy 1.295 GeV.

Photon beam asymmetry at incident photon energy 1.328 GeV.

Photon beam asymmetry at incident photon energy 1.361 GeV.

Photon beam asymmetry at incident photon energy 1.394 GeV.

Photon beam asymmetry at incident photon energy 1.427 GeV.

Photon beam asymmetry at incident photon energy 1.460 GeV.

Photon beam asymmetry at incident photon energy 1.493 GeV.

Photon beam asymmetry at incident photon energy 1.526 GeV.

Photon beam asymmetry at incident photon energy 1.559 GeV.

Photon beam asymmetry at incident photon energy 1.592 GeV.

Photon beam asymmetry at incident photon energy 1.625 GeV.

Photon beam asymmetry at incident photon energy 1.658 GeV.

Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 at beam energy 400 MeV. Exclusive measurement where only the PI0 decay photons and recoil proton are detected.

Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.

Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.

Differential cross section as a function of the emitted photon energy for the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.

Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.

Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.

Angular distribution of the emitted photon for the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.

Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 350 MeV.

Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 400 MeV.

Angular distribution of the PI0 in the reaction GAMMA P --> P PI0 GAMMA at beam energy 450 MeV.

Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 350 MeV.

Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 400 MeV.

Cross section ratio as a function of the emitted photon energy in the reaction GAMMA P --> P PI0 GAMMA for the beam energy 450 MeV.

Weight averaged total cross sections.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of X(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of Z(C=POMERON). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the absolute difference of the pseudorapidities of the two jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of the dijet invariant mass. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level differential cross section for diffractive dijet production as a function of mass of the diffractive system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of X(GAMMA) for 3 ranges of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Bin averaged hadron level double-differential cross section for diffractive dijet production as a function of Z(POMERON) for 2 ranges of X(GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of X(C=GAMMA). The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of ET of jet 1. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the average pseudorapidity of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the absolute difference in the pseudorapidities of the 2 jets. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of the invariant mass of the dijet system. The first systematic error is the uncorrelated and the second the correlated uncertainty.

Ratios of the diffractive to the inclusive single-differential hadron level dijet cross sections as a function of W. The first systematic error is the uncorrelated and the second the correlated uncertainty.