|
GSI
FRS
| |
C: Nuclide production cross sections (sigma) and relative fission yields (eta)
C: from the projectile fission of 238U in Be at 750 A MeV.
C: Statistical uncertainties are given. An additional systematic uncertainty
C: of 20% results from normalization of beam intensity and transmission.
C: The fission yields eta(A,Z) are normalized to 200%.
* References:
* Ch. Engelmann, F. Ameil, P. Armbruster, M. Bernas, S. Czajkowski, Ph. Dessagne,
* C. Donzaud, H. Geissel, A. Heinz, Z. Janas, C. Kozhuharov, Ch. Miehe,
* G. Munzenberg, M. Pfutzner, C. Rohl, W. Schwab, C. Stephan, K. Summerer,
* L. Tassan-Got, and B. Voss
* "Production and identification of heavy Ni isotopes: evidence for the doubly
* magic nucleus 78Ni."
* Z. Phys. A 352 (1995) 351
* M. Bernas, C. Engelmann, P. Armbruster, S. Czajkowski, F. Ameil,
* C. Bockstiegel, Ph. Dessagne, C. Donzaud, H. Geissel, A. Heinz, Z. Janas,
* C. Kozhuharov, Ch. Miehe, G. Munzenberg, M. Pfutzner, W. Schwab, C. Stephan,
* K. Summerer, L. Tassan-Got, and B. Voss
* "Discovery and cross section measurement of 58 new fission products in projectile
* fission of 238U at 750 A.MeV*
* Phys. Lett. B415 (1997) 111
S: ANALYZER(N(20))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of calcium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-20 Y,NT11 D% N
49 48 11 2.0E-2
50 14 11 3.9E-3
51 2.7 8 1.1E-3
52 0.45 10 1.9E-4
53 0.036 20 1.5E-5
54 0.005 22 2.1E-6
55 0.002 29 8.5E-7
56 0.001 40 4.2E-7
S: ANALYZER(N(21))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of scandium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-21 Y,NT11 D% N
51 160 8 6.8E-2
52 44 7 1.9E-2
53 14 5 3.9E-2
54 2.5 6 1.1E-3
55 0.4 11 1.7E-4
56 0.05 12 2.1E-5
57 0.01 13 4.2E-6
58 0.003 21 1.3E-6
S: ANALYZER(N(22))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of titanium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-22 Y,NT11 D% N
54 34 8 1.4E-2
55 7.4 5 3.1E-3
56 4.8 5 2.0E-3
57 0.72 6 3.1E-4
58 0.19 9 8.1E-5
59 0.05 22 2.1E-5
60 0.01 23 4.2E-6
61 0.0025 33 1.1E-6
S: ANALYZER(N(23))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of vanadium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-23 Y,NT11 D% N
56 68 6 2.9E-2
57 39 7 1.7E-2
58 9.2 4 3.9E-3
59 4.1 5 1.7E-3
60 0.51 8 2.2E-4
61 0.31 9 5.5E-5
62 0.021 14 8.9E-6
63 0.0064 17 2.7E-6
64 0.0003 100 1.3E-7
S: ANALYZER(N(24))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of chromium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-24 Y,NT11 D% N
59 55 8 2.3E-2
60 25 8 1.1E-2
61 5.2 6 2.2E-3
62 2.3 7 9.7E-4
63 0.34 9 1.4E-4
64 0.072 18 3.1E-5
65 0.0078 13 3.3E-6
66 0.0015 30 6.4E-7
67 0.0005 100 2.1E-7
S: ANALYZER(N(25))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of manganese
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-25 Y,NT11 D% N
61 126 10 5.3E-2
62 39 7 1.7E-2
63 24 8 1.0E-2
64 5.4 6 2.3E-3
65 1.6 9 6.8E-4
66 0.22 9 9.3E-5
67 0.04 13 1.7E-5
68 0.005 18 2.1E-6
69 0.0004 65 1.7E-7
S: ANALYZER(N(26))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of iron
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-26 Y,NT11 D% N
63 270 13 1.1E-1
64 87 5 3.7E-2
65 37 6 1.6E-2
66 15 5 6.4E-3
67 4.9 8 2.1E-3
68 0.93 7 3.9E-4
69 0.23 13 9.7E-5
70 0.028 9 1.2E-5
71 0.0047 20 2.0E-6
72 0.0003 100 1.3E-7
S: ANALYZER(N(27))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of cobald
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-27 Y,NT11 D% N
65 194 23 8.2E-2
66 150 4 6.4E-2
67 72 5 3.1E-2
68 24 8 1.0E-2
69 12 3 5.1E-3
70 3.1 4 1.3E-3
71 0.68 6 2.9E-4
72 0.10 8 4.2E-5
73 0.02 10 8.5E-6
74 0.002 29 8.5E-7
75 0.00003 50 1.3E-7
S: ANALYZER(N(28))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of nickel
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-28 Y,NT11 D% N
68 119 4 5.0E-2
69 69 3 2.9E-2
70 35 3 1.5E-2
71 15 3 6.4E-3
72 7.7 3 3.3E-3
73 2.5 4 1.1E-3
74 0.63 5 2.7E-4
75 0.086 5 3.6E-5
76 0.014 9 5.9E-6
77 0.0014 29 5.9E-7
78 0.0002 56 8.5E-8
S: ANALYZER(N(29))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of copper
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-29 Y,NT11 D% N
70 220 15 5.5E-5
71 143 12 5.5E-6
72 77 10 4.2E-7
73 43 10 9.6E-2
74 20 9 7.3E-2
75 11 9 4.0E-2
76 2.7 10 3.1E-2
77 0.86 10 1.4E-2
78 0.11 10 6.8E-3
79 0.015 9 1.9E-3
80 0.001 8 5.1E-4
S: ANALYZER(N(30))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of zink
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-30 Y,NT11 D% N
73 227 14 9.6E-2
74 172 14 7.3E-2
75 94 11 4.0E-2
76 73 14 3.1E-2
77 32 10 1.4E-2
78 16 10 6.8E-3
79 4.5 9 1.9E-3
80 1.2 8 5.1E-4
81 0.13 10 5.5E-5
82 0.013 14 5.5E-6
83 0.001 35 4.2E-7
S: ANALYZER(N(31))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of gallium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-31 Y,NT11 D% N
76 242 3 1.0E-1
77 193 2 8.2E-2
78 144 2 6.1E-2
79 106 1 4.5E-2
80 51 2 2.2E-2
81 22 2 9.3E-3
82 4.3 2 1.8E-3
83 0.81 3 3.4E-4
84 0.10 5 4.2E-5
85 0.0065 13 2.8E-6
86 0.0006 49 2.5E-7
S: ANALYZER(N(32))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of germanium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-32 Y,NT11 D% N
78 370 2 1.6E-1
79 371 2 1.6E-1
80 323 2 1.4E-1
81 291 1 1.2E-1
82 207 1 8.8E-2
83 76 1 3.2E-2
84 29 1 1.2E-2
85 4.7 2 2.0E-3
86 0.82 3 3.5E-4
87 0.067 5 2.8E-5
88 0.0067 13 2.8E-6
89 0.0006 55 2.5E-7
S: ANALYZER(N(33))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of arsen
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-33 Y,NT11 D% N
82 535 2 2.3E-1
83 503 2 2.1E-1
84 394 1 1.7E-1
85 247 1 1.0E-1
86 73 1 3.1E-2
87 19 2 8.1E-3
88 2.9 3 1.2E-3
89 0.34 3 1.4E-4
90 0.021 8 8.9E-6
91 0.0032 24 1.4E-6
92 0.0006 50 2.5E-7
S: ANALYZER(N(34))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of scandium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-34 Y,NT11 D% N
83 1360 2 5.8E-1
84 1150 1 4.9E-1
85 870 30 3.7E-1
86 910 1 3.9E-1
87 536 1 2.3E-1
88 279 1 1.2E-1
89 61 1 2.6E-2
90 14 2 5.9E-3
91 1.1 2 4.7E-4
92 0.12 4 5.1E-5
93 0.0082 12 3.5E-6
94 0.002 26 8.5E-7
S: ANALYZER(N(35))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of bromium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-35 Y,NT11 D% N
86 1360 1 5.8E-1
87 1280 1 5.4E-1
88 960 50 4.1E-1
89 1020 1 4.3E-1
90 447 1 1.9E-1
91 238 1 1.0E-1
92 34 1 1.4E-2
93 8.2 2 3.5E-3
94 0.67 3 2.8E-4
95 0.075 4 3.2E-5
96 0.0059 13 2.5E-6
97 0.0007 36 3.0E-7
S: ANALYZER(N(36))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of krypton
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-36 Y,NT11 D% N
89 2170 1 9.2E-1
90 1600 1 6.8E-1
91 1580 1 6.7E-1
92 1290 1 5.5E-1
93 467 1 2.0E-1
94 168 1 7.1E-2
95 29 1 1.2E-2
96 6.0 2 2.5E-3
97 0.50 3 2.1E-4
98 0.054 5 2.3E-5
99 0.0026 18 1.1E-6
100 0.0005 55 2.1E-7
S: ANALYZER(N(37))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of rubidium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-37 Y,NT11 D% N
91 3000 1 1.3
92 2040 10 8.6E-1
93 1300 50 5.5E-1
94 1450 1 6.1E-1
95 1040 1 4.4E-1
96 323 1 1.4E-1
97 122 1 5.2E-2
98 18 2 7.6E-3
99 3.2 3 1.4E-3
100 0.23 4 9.7E-5
101 0.025 7 1.1E-5
102 0.0009 31 3.8E-7
S: ANALYZER(N(38))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of strontium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-38 Y,NT11 D% N
94 2540 1 1.1
95 1950 1 8.3E-1
96 1180 50 5.0E-1
97 1460 1 6.2E-1
98 856 1 3.6E-1
99 223 1 9.4E-2
100 53 1 2.2E-2
101 7.9 2 3.3E-3
102 0.94 3 4.0E-4
103 0.050 6 2.1E-5
104 0.0066 13 2.8E-6
105 0.0008 60 3.4E-7
S: ANALYZER(N(39))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of yttrium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-39 Y,NT11 D% N
99 1580 1 6.7E-1
100 1250 1 5.3E-1
101 514 1 2.2E-1
102 124 1 5.3E-2
103 24 1 1.0E-2
104 2.8 3 1.2E-3
105 0.31 6 1.3E-4
106 0.016 10 6.8E-6
107 0.0028 25 1.2E-6
S: ANALYZER(N(40))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of zirconium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-40 Y,NT11 D% N
99 2560 1 1.1
100 2410 1 1.0
101 1240 50 5.3E-1
102 1390 1 5.9E-1
103 674 1 2.9E-1
104 280 1 1.2E-1
105 50 1 2.1E-2
106 9.1 2 3.9E-3
107 0.88 4 3.7E-4
108 0.10 6 4.2E-5
109 0.0054 15 2.3E-6
110 0.0004 43 1.7E-7
S: ANALYZER(N(41))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of niobium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-41 Y,NT11 D% N
105 1800 1 7.6E-1
106 383 2 1.6E-1
107 134 4 5.7E-2
108 25 6 1.1E-2
109 4.5 15 1.9E-3
110 0.48 43 2.0E-4
111 0.050 1 2.1E-5
112 0.0025 1 1.1E-6
113 0.0007 50 3.0E-7
S: ANALYZER(N(42))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of molybdenum
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-42 Y,NT11 D% N
114 0.024 36 1.0E-5
115 0 100 0 /* only for technical reasons */
S: ANALYZER(N(43))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of technecium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-43 Y,NT11 D% N
116 0.081 20 3.4E-5
117 0.0084 60 3.6E-6
S: ANALYZER(N(44))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of rubidium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-44 Y,NT11 D% N
119 0.014 45 5.9E-6
120 0 100 0 /* only for technical reasons */
S: ANALYZER(N(45))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of rhenium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-45 Y,NT11 D% N
122 0.013 45 5.5E-6
123 0 100 0 /* only for technical reasons */
S: ANALYZER(N(46))
X: Neutron number
Y: Cross section / mi^b
C: isotopes of palladium
C: A sigma / micro-barn uncertainty / % eta(A,Z) / %
A: X-46 Y,NT11 D% N
124 0.032 23 1.4E-5
125 0 100 0 /* only for technical reasons */
|
