Fig. 7 of J. Diklić, S. Szilner , L. Corradi, T. Mijatović, G. Pollarolo, P. Čolović et al., Transfer reactions in 206Pb+ 118 Sn: from quasielastic to deep-inelastic processes, Phys. Rev. C 107, 014619 (2023) filled circles, which correspond to the integration of the full Q-values Z A theta_cm dsigma/domega_cm err ******************************************* 48 114 118.5 3.8 0.1 48 114 116.6 5.0 0.2 48 114 114.6 6.6 0.2 48 114 112.6 6.5 0.2 48 114 110.6 6.3 0.2 48 114 108.7 5.1 0.2 48 114 106.7 3.9 0.1 48 114 104.7 2.4 0.1 48 115 118.3 3.1 0.1 48 115 116.3 4.2 0.1 48 115 114.3 5.4 0.2 48 115 112.3 5.3 0.2 48 115 110.3 5.3 0.2 48 115 108.3 4.6 0.2 48 115 106.3 3.3 0.1 48 115 104.3 2.3 0.1 48 116 118.1 2.1 0.1 48 116 116.1 3.1 0.1 48 116 114.1 3.3 0.1 48 116 112.1 3.5 0.1 48 116 110.1 3.5 0.1 48 116 108.1 3.1 0.1 48 116 106.1 2.4 0.1 48 116 104.1 1.7 0.1 48 117 117.76 1.14 0.07 48 117 115.75 1.48 0.08 48 117 113.74 1.69 0.09 48 117 111.73 1.72 0.09 48 117 109.71 1.69 0.09 48 117 107.70 1.69 0.09 48 117 105.69 1.08 0.07 48 117 103.68 0.88 0.07 48 118 117.58 0.40 0.04 48 118 115.56 0.59 0.05 48 118 113.54 0.72 0.06 48 118 111.52 0.67 0.06 48 118 109.51 0.75 0.06 48 118 107.49 0.70 0.06 48 118 105.47 0.56 0.05 48 118 103.45 0.41 0.05 49 115 118.40 8.0 0.2 49 115 116.40 10.3 0.2 49 115 114.40 11.0 0.2 49 115 112.40 11.5 0.2 49 115 110.45 11.5 0.2 49 115 108.50 10.0 0.2 49 115 106.50 7.7 0.2 49 115 104.50 6.4 0.2 49 116 118.10 8.7 0.2 49 116 116.10 11.4 0.2 49 116 114.10 13.2 0.3 49 116 112.20 14.2 0.3 49 116 110.20 15.3 0.3 49 116 108.20 12.6 0.3 49 116 106.20 10.1 0.2 49 116 104.20 7.9 0.2 49 117 118.00 8.0 0.2 49 117 116.00 11.5 0.2 49 117 114.00 15.0 0.3 49 117 112.00 15.6 0.3 49 117 110.00 17.1 0.3 49 117 108.00 15.4 0.3 49 117 106.00 11.8 0.2 49 117 104.00 10.1 0.2 49 118 117.70 5.5 0.2 49 118 115.70 8.9 0.2 49 118 113.65 11.0 0.2 49 118 111.60 11.2 0.2 49 118 109.60 11.9 0.2 49 118 107.60 10.8 0.2 49 118 105.60 7.1 0.2 49 118 103.60 5.7 0.2 49 119 117.50 2.3 0.1 49 119 115.50 3.4 0.1 49 119 113.50 4.1 0.1 49 119 111.40 4.0 0.1 49 119 109.40 4.3 0.1 49 119 107.40 3.8 0.1 49 119 105.40 2.4 0.1 49 119 103.35 1.9 0.1 50 116 118.20 15.1 0.3 50 116 116.20 16.3 0.3 50 116 114.20 17.0 0.3 50 116 112.20 16.7 0.3 50 116 110.20 17.9 0.3 50 116 108.20 16.9 0.3 50 116 106.20 13.9 0.3 50 116 104.20 12.6 0.3 50 117 118.10 48.1 0.5 50 117 116.10 54.9 0.5 50 117 114.10 48.6 0.5 50 117 112.10 45.9 0.5 50 117 110.15 51.6 0.5 50 117 108.15 52.3 0.5 50 117 106.20 46.9 0.5 50 117 104.20 46.4 0.5 50 119 117.70 29.7 0.4 50 119 115.70 41.8 0.5 50 119 113.70 57.5 0.5 50 119 111.70 69.4 0.6 50 119 109.65 84.0 0.6 50 119 107.60 84.0 0.7 50 119 105.60 80.3 0.6 50 119 103.60 71.4 0.6 50 120 117.60 15.1 0.3 50 120 115.55 17.7 0.3 50 120 113.50 21.7 0.3 50 120 111.50 24.6 0.3 50 120 109.50 29.7 0.4 50 120 107.50 27.8 0.4 50 120 105.45 24.4 0.4 50 120 103.40 19.9 0.3 51 117 118.00 5.7 0.2 51 117 116.00 7.7 0.2 51 117 114.00 7.8 0.2 51 117 112.00 6.9 0.2 51 117 110.00 5.9 0.2 51 117 108.00 6.0 0.2 51 117 106.00 6.4 0.2 51 117 104.00 4.8 0.2 51 119 117.70 7.3 0.2 51 119 115.65 10.5 0.2 51 119 113.60 12.4 0.2 51 119 111.60 12.0 0.2 51 119 109.60 13.1 0.3 51 119 107.60 9.9 0.2 51 119 105.60 9.2 0.2 51 119 103.60 7.0 0.2 51 120 117.50 6.1 0.2 51 120 115.50 8.4 0.2 51 120 113.50 9.7 0.2 51 120 111.50 9.5 0.2 51 120 109.45 9.9 0.2 51 120 107.40 7.5 0.2 51 120 105.40 5.9 0.2 51 120 103.40 4.2 0.1 51 121 117.30 4.7 0.1 51 121 115.20 5.6 0.2 51 121 113.20 6.8 0.2 51 121 111.20 6.3 0.2 51 121 109.10 6.5 0.2 51 121 107.10 5.0 0.2 51 121 105.10 4.6 0.2 51 121 103.00 3.1 0.1 empty circles (the quasi-elastic part with the integration in the range from the Qgs to -35 MeV). The elastic+inelastic channel (Z=50, A=118) is given as a ratio over the Rutherford cross section Z A theta_cm dsigma/domega_cm err *************************************** 50 116 138.10 0.04 0.03 50 116 136.10 0.07 0.04 50 116 134.11 0.14 0.05 50 116 132.11 0.29 0.07 50 116 130.12 0.46 0.09 50 116 128.12 0.37 0.08 50 116 126.10 0.52 0.10 50 116 124.10 0.83 0.13 50 116 118.20 5.23 0.15 50 116 116.20 8.29 0.20 50 116 114.20 9.32 0.22 50 116 112.20 10.00 0.22 50 116 110.80 11.58 0.24 50 116 108.20 11.44 0.24 50 116 106.20 10.31 0.23 50 116 104.30 10.66 0.23 50 117 136.09 0.09 0.04 50 117 134.09 0.16 0.05 50 117 132.09 0.40 0.09 50 117 130.10 0.70 0.11 50 117 128.10 0.89 0.13 50 117 126.10 1.20 0.15 50 117 124.10 1.42 0.16 50 117 118.10 10.36 0.22 50 117 116.10 18.19 0.30 50 117 114.10 22.67 0.33 50 117 112.10 24.96 0.35 50 117 110.15 30.64 0.39 50 117 108.15 34.45 0.42 50 117 106.20 33.42 0.41 50 117 104.20 35.71 0.43 50 118 136.00 0.0007 0.0003 50 118 134.00 0.0041 0.0007 50 118 132.00 0.0100 0.0010 50 118 130.00 0.0090 0.0010 50 118 128.00 0.0150 0.0010 50 118 126.00 0.0150 0.0010 50 118 124.00 0.0216 0.0015 50 118 118.00 0.0870 0.0010 50 118 116.00 0.1350 0.0020 50 118 114.00 0.2200 0.0020 50 118 112.00 0.3000 0.0025 50 118 110.00 0.3730 0.0030 50 118 108.00 0.4360 0.0030 50 118 106.00 0.5100 0.0030 50 118 104.00 0.5510 0.0030 50 119 135.80 0.20 0.06 50 119 133.80 0.73 0.11 50 119 131.80 1.44 0.16 50 119 129.80 1.78 0.18 50 119 127.80 1.79 0.18 50 119 125.80 2.73 0.22 50 119 123.70 4.00 0.27 50 119 117.70 13.44 0.25 50 119 115.70 20.24 0.31 50 119 113.70 29.71 0.38 50 119 111.70 40.53 0.45 50 119 109.70 53.01 0.52 50 119 107.60 58.15 0.54 50 119 105.60 61.84 0.56 50 119 103.60 59.35 0.56 50 120 135.71 0.09 0.04 50 120 133.70 0.21 0.06 50 120 131.70 0.52 0.10 50 120 129.70 1.05 0.14 50 120 127.65 1.13 0.14 50 120 125.60 1.29 0.15 50 120 123.60 1.71 0.18 50 120 117.60 6.65 0.18 50 120 115.55 9.41 0.21 50 120 113.50 12.78 0.25 50 120 111.50 16.45 0.29 50 120 109.50 21.92 0.33 50 120 107.50 21.37 0.34 50 120 105.50 20.20 0.32 50 120 103.40 17.43 0.30