Experimental data on
fusion
elastic scattering
evaporation residue

Experimental data on elastic scattering

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10B + 9Be,   Ecm=9.5 MeV

K.Bodek, M.Hugi, J.Lang, R.Mueller, A.Schiltz,J.Sromicki, E.Ungricht,
Physics Letters, B92 (1980) 79
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Comments
Beam quality: no data
Target: 50 mcg/m**2 thick Be-9 target was used.
Data obtained: exported from EXFOR
The experiments were done at the Tandem Van de Graaff accelerator of the Eidgenossische Technische Hochschule, Zurich. The 5% errors were added (in accordance to the author reccomendation) when no data in EXFOR. 

 
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Θcm (deg)σ/σR (ratio)error (%)+δσ-δσ
12.8 0.99 16 0.1584 0.1584
15.4 1 11 0.11 0.11
17.2 0.91 8 0.0728 0.0728
19 0.79 8 0.0632 0.0632
21.3 0.682 5 0.0341 0.0341
23.1 0.608 5 0.0304 0.0304
25.8 0.511 5 0.0256 0.0256
27.6 0.456 5 0.0228 0.0228
29.8 0.411 5 0.0206 0.0206
32 0.435 5 0.0218 0.0218
34.2 0.44 5 0.022 0.022
36.5 0.44 5 0.022 0.022
36.9 0.401 5 0.0201 0.0201
37.8 0.362 5 0.0181 0.0181
40.6 0.304 5 0.0152 0.0152
42.4 0.25 5 0.0125 0.0125
44.2 0.211 7 0.0148 0.0148
46.9 0.197 5 0.0099 0.0099
49.1 0.186 6 0.0112 0.0112
49.1 0.211 5 0.0106 0.0106
51.3 0.216 5 0.0108 0.0108
53 0.239 5 0.012 0.012
55.3 0.223 4 0.009 0.009
58.8 0.206 5 0.0103 0.0103
61.1 0.153 7 0.0108 0.0108
63.4 0.1269 5 0.0064 0.0064
66.1 0.107 8 0.0086 0.0086
68.8 0.1055 1.6 0.0017 0.0017
71.8 0.118 8 0.0095 0.0095
74.9 0.1226 5 0.0062 0.0062
77.1 0.142 6 0.0086 0.0086
82.5 0.124 6 0.0075 0.0075
84.3 0.0909 5 0.0046 0.0046
85.6 0.1 5 0.005 0.005
89.7 0.073 5 0.0037 0.0037
95 0.0773 5 0.0039 0.0039
100.3 0.0838 5 0.0042 0.0042
105.2 0.0888 5 0.0045 0.0045
109.6 0.083 4 0.0034 0.0034
114.9 0.0888 5 0.0045 0.0045
119.3 0.1093 5 0.0055 0.0055
125.4 0.136 2.2 0.003 0.003
129.8 0.186 3 0.0056 0.0056
134.6 0.245 5 0.0123 0.0123
139.8 0.291 5 0.0146 0.0146
144.7 0.294 3 0.0089 0.0089
149.5 0.327 4 0.0131 0.0131
150.9 0.338 3 0.0102 0.0102
153.4 0.489 2.5 0.0123 0.0123
156.5 0.574 5 0.0287 0.0287
159.5 0.667 5 0.0334 0.0334
161.8 0.588 5 0.0294 0.0294
164.9 0.548 2.7 0.0148 0.0148
167.9 0.675 5 0.0338 0.0338