Experimental data on
fusion
elastic scattering
evaporation residue

Experimental data on evaporation residues

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(at least one item) 		Z1 A1   +   Z2 A2    
and/or Evaporation channel     n    p    α
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14N + 59Co

P.R.S. Gomes, T.J.P. Penna, R. L. Neto, J.C. Acquadro, C. Tenreiro, P.A.B. Freitas, E. Crema, N.C. Filho, M.M. Coimbra,
Nuclear Instruments and Methods, A280 (1989) 395-401
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Comments
Beam quality:
Target: from 100 to 800 mcg/cm 2
Detected particles: gamma-rays of EvR
Data obtained: author's table
8UD Pelletron accelerator of the Universidade de S. Paulo. The overall error is in the range from 8% at higher energies to almost 20% at very low energies. 

2pn+a2pn   1p1n   1p2n   1p3n   2p2n   1a1n   1a2n   1a1p   1a1p1n   1a1p2n   1a2p   2a1n   All channels
 
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2pn+a2pn
Elab (MeV)σ (mb)+δσ-δσ
32 7.5 0 0
34 32 0 0
36.5 80.2 0 0
40 200 0 0
45 230 0 0
48 250 0 0
51 240 0 0
56 220 0 0
1p1n
Elab (MeV)σ (mb)+δσ-δσ
32 7.3 0 0
34 17.2 0 0
36.5 82 0 0
40 115 0 0
45 56.5 0 0
48 40.3 0 0
51 32.5 0 0
56 28.5 0 0
1p2n
Elab (MeV)σ (mb)+δσ-δσ
32 2.2 0 0
34 24 0 0
36.5 62 0 0
40 106 0 0
45 190 0 0
48 220 0 0
51 200 0 0
56 170 0 0
1p3n
Elab (MeV)σ (mb)+δσ-δσ
36.5 1.2 0 0
40 3.1 0 0
45 4.2 0 0
48 6.9 0 0
51 7.3 0 0
56 15 0 0
2p2n
Elab (MeV)σ (mb)+δσ-δσ
40 1.2 0 0
45 11.2 0 0
48 33.6 0 0
51 72.9 0 0
56 129 0 0
1a1n
Elab (MeV)σ (mb)+δσ-δσ
32 4.2 0 0
34 7.5 0 0
36.5 22 0 0
40 35 0 0
45 38.9 0 0
48 35.7 0 0
51 34 0 0
56 27.4 0 0
1a2n
Elab (MeV)σ (mb)+δσ-δσ
40 3.2 0 0
45 12.5 0 0
48 21.8 0 0
51 34.1 0 0
56 46.8 0 0
1a1p
Elab (MeV)σ (mb)+δσ-δσ
32 1.8 0 0
34 5.4 0 0
36.5 14.2 0 0
40 17.6 0 0
45 21.3 0 0
48 36.1 0 0
51 34.4 0 0
56 39.5 0 0
1a1p1n
Elab (MeV)σ (mb)+δσ-δσ
34 4 0 0
36.5 16.6 0 0
40 45.3 0 0
45 82.3 0 0
48 108 0 0
51 138 0 0
56 174 0 0
1a1p2n
Elab (MeV)σ (mb)+δσ-δσ
40 18 0 0
45 37.3 0 0
48 80 0 0
51 79 0 0
56 105 0 0
1a2p
Elab (MeV)σ (mb)+δσ-δσ
32 4.5 0 0
34 9.2 0 0
36.5 12.9 0 0
40 20.8 0 0
45 27.8 0 0
48 37.7 0 0
51 51 0 0
56 96 0 0
2a1n
Elab (MeV)σ (mb)+δσ-δσ
34 4 0 0
36.5 8.7 0 0
40 12.9 0 0
45 17.7 0 0
48 31.3 0 0
51 37.9 0 0
56 51.8 0 0