Experimental data on
fusion
elastic scattering
evaporation residue

Experimental data on elastic scattering

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6Li + 144Sm,   Elab=22.1 MeV

J.M. Figueira, J.O. Fernandez Niello, A. Arazi, O.A. Capurro, P. Carnelli, L. Fimiani, G.V. Marti, D. Martinez Heimann, A.E. Negri, A.J. Pacheco, J. Lubian, D.S. Monteiro, P.R.S. Gomes,
Physical Review, C81 (2010) 024613
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Comments
Beam quality: Beam currents were of the order of 20 pnA. Energy spread of the beam was around 0.5%.
Target: A 120 µg/cm2-thick 144Sm target, isotopically enriched to 88%, evaporated onto a 20 µg/cm2 carbon backing.
Data obtained: author graph (digitized with GSYS 2.4)
The 20 UD tandem accelerator at the TANDAR Laboratory. 

 
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Θcm (deg)σ/σR (ratio)error (%)+δσ-δσ
25.78 0.9883 2 0.0198 0.0198
28.39 1.008 2 0.0202 0.0202
31.44 1.008 2 0.0202 0.0202
34.04 1.008 2 0.0202 0.0202
36.87 0.9976 2 0.02 0.02
39.26 0.9975 2 0.02 0.02
41.87 0.9872 2 0.0198 0.0198
59.7 0.9861 2 0.0198 0.0198
62.3 0.986 2 0.0198 0.0198
64.91 0.9959 2 0.02 0.02
67.74 0.9957 2 0.02 0.02
69.7 0.9956 2 0.02 0.02
72.3 1.006 2 0.0202 0.0202
84.7 0.9746 2 0.0195 0.0195
87.3 0.9844 2 0.0197 0.0197
89.91 0.9943 2 0.0199 0.0199
92.09 0.9841 2 0.0197 0.0197
95.35 1.014 2 0.0203 0.0203
100.1 1.024 2 0.0205 0.0205
102.7 0.9835 2 0.0197 0.0197
104.9 0.9933 2 0.0199 0.0199
107.5 0.9732 2 0.0195 0.0195
110.1 0.9731 2 0.0195 0.0195
112.5 0.9534 2 0.0191 0.0191
114.7 0.963 2 0.0193 0.0193
117.3 0.9435 2 0.0189 0.0189
119.7 0.9338 2 0.0187 0.0187
122.5 0.9149 2 0.0183 0.0183
124.9 0.9335 2 0.0187 0.0187
127.1 0.924 2 0.0185 0.0185
129.5 0.8961 2 0.018 0.018
132.1 0.878 2 0.0176 0.0176
134.7 0.8778 2 0.0176 0.0176
136.9 0.8867 2 0.0178 0.0178
139 0.8776 2 0.0176 0.0176
141.4 0.8512 2 0.0171 0.0171
144 0.8424 2 0.0169 0.0169
146.4 0.8254 2 0.0166 0.0166
149 0.8337 2 0.0167 0.0167
151.4 0.8168 2 0.0164 0.0164
153.8 0.7842 2 0.0157 0.0157
156 0.7841 2 0.0157 0.0157
158.6 0.7605 2 0.0153 0.0153
161.2 0.7527 2 0.0151 0.0151
163.2 0.768 2 0.0154 0.0154
165.8 0.7679 2 0.0154 0.0154
167.9 0.7678 2 0.0154 0.0154
170.3 0.7522 2 0.0151 0.0151