Fission Product Yield Data for the Transmutation of Minor Actinide ...

More documents

Recommendations

Info

Annex 1 to Appendix II ADJUSTED DATA MEASURED BY VIVÈS, ZÖLLER AND ÄYSTÖ Vivès et al. (2000) [II.8] E n = 1.60 MeV Pre-neutron emission E n = 5.5 MeV Pre-neutron emission Mass A Yield (%) Uncertainty Mass A Yield (%) Uncertainty 7.5000E+01 –4.3656E–03 1.4209E–04 7.8000E+01 2.7388E–03 7.1044E–04 7.9000E+01 8.0673E–03 1.1367E–03 8.0000E+01 1.3395E–02 1.5630E–03 8.1000E+01 2.8005E–02 3.5522E–03 8.2000E+01 3.8401E–02 5.8256E–03 8.3000E+01 9.8707E–02 1.3498E–02 8.4000E+01 3.5164E–01 3.5664E–02 8.5000E+01 4.2392E–01 4.2484E–02 8.6000E+01 6.4248E–01 5.9961E–02 8.7000E+01 8.7907E–01 7.8575E–02 8.8000E+01 1.3097E+00 8.5573E–02 8.9000E+01 1.6787E+00 1.0880E–01 9.0000E+01 2.1215E+00 1.3289E–01 9.1000E+01 2.5971E+00 1.5878E–01 9.2000E+01 3.2447E+00 1.9235E–01 9.3000E+01 3.7560E+00 2.1665E–01 9.4000E+01 4.3424E+00 1.6532E–01 9.5000E+01 4.4360E+00 1.7193E–01 9.6000E+01 4.6361E+00 1.8528E–01 9.7000E+01 4.9172E+00 2.0013E–01 9.8000E+01 5.0394E+00 2.0603E–01 9.9000E+01 5.5539E+00 2.2414E–01 1.0000E+02 6.1263E+00 2.4283E–01 1.0100E+02 6.3753E+00 2.4865E–01 1.0200E+02 6.4716E+00 2.4574E–01 1.0300E+02 6.6572E+00 2.4404E–01 1.0400E+02 7.0271E+00 2.5185E–01 1.0500E+02 6.3598E+00 2.2620E–01 1.0600E+02 5.2813E+00 1.9615E–01 1.0700E+02 3.9937E+00 1.6454E–01 1.0800E+02 2.6459E+00 1.8511E–01 1.0900E+02 1.5191E+00 1.2138E–01 1.1000E+02 7.4444E–01 6.9268E–02 1.1100E+02 3.9131E–01 5.0583E–02 1.1200E+02 2.6189E–01 3.2964E–02 1.1300E+02 8.7609E–02 1.3783E–02 1.1400E+02 5.8556E–02 7.8149E–03 6.7000E+01 2.7711E–04 5.5385E–05 6.8000E+01 2.7711E–04 5.5385E–05 6.9000E+01 9.6940E–04 1.1077E–04 7.0000E+01 2.3540E–03 2.2154E–04 7.1000E+01 3.2430E–03 2.7692E–04 7.2000E+01 4.2099E–03 3.3231E–04 7.3000E+01 4.1060E–03 3.3231E–04 7.4000E+01 5.3387E–03 4.9846E–04 7.5000E+01 6.0832E–03 6.6462E–04 7.6000E+01 7.8019E–03 9.9693E–04 7.7000E+01 1.1983E–02 1.6062E–03 7.8000E+01 2.9070E–02 3.3785E–03 7.9000E+01 3.5724E–02 4.5416E–03 8.0000E+01 8.9406E–02 9.5262E–03 8.1000E+01 1.3484E–01 1.3791E–02 8.2000E+01 2.1427E–01 2.0825E–02 8.3000E+01 3.0298E–01 2.8523E–02 8.4000E+01 4.4530E–01 4.0597E–02 8.5000E+01 5.7356E–01 5.2671E–02 8.6000E+01 8.1798E–01 7.3053E–02 8.7000E+01 1.0490E+00 6.9203E–02 8.8000E+01 1.4099E+00 9.0554E–02 8.9000E+01 1.7439E+00 1.1082E–01 9.0000E+01 2.2224E+00 1.4003E–01 9.1000E+01 2.5176E+00 1.5781E–01 9.2000E+01 3.0491E+00 1.8485E–01 9.3000E+01 3.8910E+00 2.2580E–01 9.4000E+01 4.4983E+00 1.7056E–01 9.5000E+01 4.6434E+00 1.7817E–01 9.6000E+01 4.7660E+00 1.8919E–01 9.7000E+01 4.9223E+00 1.9955E–01 9.8000E+01 5.2338E+00 2.1104E–01 9.9000E+01 5.8253E+00 2.2946E–01 1.0000E+02 6.0551E+00 2.3503E–01 1.0100E+02 6.1702E+00 2.3860E–01 1.0200E+02 5.9899E+00 2.3001E–01 1.0300E+02 5.9916E+00 2.2533E–01 1.0400E+02 6.1456E+00 2.2531E–01 1.0500E+02 5.6174E+00 2.0346E–01 1.0600E+02 4.7795E+00 1.7945E–01 1.0700E+02 3.6097E+00 2.2065E–01 1.0800E+02 2.5537E+00 1.7218E–01 1.0900E+02 1.6316E+00 1.2046E–01 1.1000E+02 1.0536E+00 8.1873E–02 1.1100E+02 7.3045E–01 7.7096E–02 1.1200E+02 4.0852E–01 4.6357E–02 1.1300E+02 2.5812E–01 3.0295E–02 1.1400E+02 1.5572E–01 1.8000E–02 309
1.1500E+02 3.1986E–02 4.1206E–03 1.1600E+02 1.5134E–02 2.1313E–03 1.1700E+02 8.7290E–03 1.2788E–03 1.1800E+02 4.9015E–03 8.5253E–04 1.1900E+02 1.8036E–03 5.6835E–04 1.2000E+02 1.8036E–03 5.6835E–04 1.2100E+02 4.9015E–03 8.5253E–04 1.2200E+02 8.7290E–03 1.2788E–03 1.2300E+02 1.5134E–02 2.1313E–03 1.2400E+02 3.1986E–02 4.1206E–03 1.2500E+02 5.8556E–02 7.8149E–03 1.2600E+02 8.7609E–02 1.3783E–02 1.2700E+02 2.6189E–01 3.2964E–02 1.2800E+02 3.9131E–01 5.0583E–02 1.2900E+02 7.4444E–01 6.9268E–02 1.3000E+02 1.5191E+00 1.2138E–01 1.3100E+02 2.6459E+00 1.8511E–01 1.3200E+02 3.9937E+00 1.6454E–01 1.3300E+02 5.2813E+00 1.9615E–01 1.3400E+02 6.3598E+00 2.2620E–01 1.3500E+02 7.0271E+00 2.5185E–01 1.3600E+02 6.6572E+00 2.4404E–01 1.3700E+02 6.4716E+00 2.4574E–01 1.3800E+02 6.3753E+00 2.4865E–01 1.3900E+02 6.1263E+00 2.4283E–01 1.4000E+02 5.5539E+00 2.2414E–01 1.4100E+02 5.0394E+00 2.0603E–01 1.4200E+02 4.9172E+00 2.0013E–01 1.4300E+02 4.6361E+00 1.8528E–01 1.4400E+02 4.4360E+00 1.7193E–01 1.4500E+02 4.3424E+00 1.6532E–01 1.4600E+02 3.7560E+00 2.1665E–01 1.4700E+02 3.2447E+00 1.9235E–01 1.4800E+02 2.5971E+00 1.5878E–01 1.4900E+02 2.1215E+00 1.3289E–01 1.5000E+02 1.6787E+00 1.0880E–01 1.5100E+02 1.3097E+00 8.5573E–02 1.5200E+02 8.7907E–01 7.8575E–02 1.5300E+02 6.4248E–01 5.9961E–02 1.5400E+02 4.2392E–01 4.2484E–02 1.5500E+02 3.5164E–01 3.5664E–02 1.5600E+02 9.8707E–02 1.3498E–02 1.5700E+02 3.8401E–02 5.8256E–03 1.5800E+02 2.8005E–02 3.5522E–03 1.5900E+02 1.3395E–02 1.5630E–03 1.6000E+02 8.0673E–03 1.1367E–03 1.6100E+02 2.7388E–03 7.1044E–04 1.6400E+02 –4.3656E–03 1.4209E–04 310 E n = 1.60 MeV Pre-neutron emission E n = 5.5 MeV Pre-neutron emission Mass A Yield (%) Uncertainty Mass A Yield (%) Uncertainty 1.1500E+02 1.2397E–01 1.2794E–02 1.1600E+02 1.1322E–01 1.0523E–02 1.1700E+02 9.7121E–02 8.8062E–03 1.1800E+02 9.1891E–02 8.3631E–03 1.1900E+02 6.3970E–02 6.4246E–03 1.2000E+02 6.3970E–02 6.4246E–03 1.2100E+02 9.1891E–02 8.3631E–03 1.2200E+02 9.7121E–02 8.8062E–03 1.2300E+02 1.1322E–01 1.0523E–02 1.2400E+02 1.2397E–01 1.2794E–02 1.2500E+02 1.5572E–01 1.8000E–02 1.2600E+02 2.5812E–01 3.0295E–02 1.2700E+02 4.0852E–01 4.6357E–02 1.2800E+02 7.3045E–01 7.7096E–02 1.2900E+02 1.0536E+00 8.1873E–02 1.3000E+02 1.6316E+00 1.2046E–01 1.3100E+02 2.5537E+00 1.7218E–01 1.3200E+02 3.6097E+00 2.2065E–01 1.3300E+02 4.7795E+00 1.7945E–01 1.3400E+02 5.6174E+00 2.0346E–01 1.3500E+02 6.1456E+00 2.2531E–01 1.3600E+02 5.9916E+00 2.2533E–01 1.3700E+02 5.9899E+00 2.3001E–01 1.3800E+02 6.1702E+00 2.3860E–01 1.3900E+02 6.0551E+00 2.3503E–01 1.4000E+02 5.8253E+00 2.2946E–01 1.4100E+02 5.2338E+00 2.1104E–01 1.4200E+02 4.9223E+00 1.9955E–01 1.4300E+02 4.7660E+00 1.8919E–01 1.4400E+02 4.6434E+00 1.7817E–01 1.4500E+02 4.4983E+00 1.7056E–01 1.4600E+02 3.8910E+00 2.2580E–01 1.4700E+02 3.0491E+00 1.8485E–01 1.4800E+02 2.5176E+00 1.5781E–01 1.4900E+02 2.2224E+00 1.4003E–01 1.5000E+02 1.7439E+00 1.1082E–01 1.5100E+02 1.4099E+00 9.0554E–02 1.5200E+02 1.0490E+00 6.9203E–02 1.5300E+02 8.1798E–01 7.3053E–02 1.5400E+02 5.7356E–01 5.2671E–02 1.5500E+02 4.4530E–01 4.0597E–02 1.5600E+02 3.0298E–01 2.8523E–02 1.5700E+02 2.1427E–01 2.0825E–02 1.5800E+02 1.3484E–01 1.3791E–02 1.5900E+02 8.9406E–02 9.5262E–03 1.6000E+02 3.5724E–02 4.5416E–03 1.6100E+02 2.9070E–02 3.3785E–03 1.6200E+02 1.1983E–02 1.6062E–03 1.6300E+02 7.8019E–03 9.9693E–04 1.6400E+02 6.0832E–03 6.6462E–04 1.6500E+02 5.3387E–03 4.9846E–04 1.6600E+02 4.1060E–03 3.3231E–04 1.6700E+02 4.2099E–03 3.3231E–04 1.6800E+02 3.2430E–03 2.7692E–04 1.6900E+02 2.3540E–03 2.2154E–04 1.7000E+02 9.6940E–04 1.1077E–04 1.7100E+02 2.7711E–04 5.5385E–05 1.7200E+02 2.7711E–04 5.5385E–05
Page 1 and 2:
Fission Product Yield Data for the
Page 3 and 4:
AFGHANISTAN ALBANIA ALGERIA ANGOLA
Page 5 and 6:
COPYRIGHT NOTICE All IAEA scientifi
Page 7 and 8:
CONTRIBUTING AUTHORS Denschlag, J.-
Page 9 and 10:
3.2.1. Introduction . . . . . . . .
Page 11 and 12:
6. BENCHMARK EXERCISE . . . . . . .
Page 13 and 14:
However, this CRP entered an entire
Page 15 and 16:
‘Provisional masses’ are determ
Page 17 and 18:
Three scientists were invited to pa
Page 19 and 20:
8 (d) Prompt or delayed neutron emi
Page 21 and 22:
[2.1.40] ITKIS, M.G., OGANESSIAN, Y
Page 23 and 24:
[2.1.96] PATE, B.D., et al., Distri
Page 25 and 26:
[2.1.152] JACOBS, E., et al., Produ
Page 27 and 28:
16 2.2. MEASUREMENTS OF THE ENERGY
Page 29 and 30:
FIG. 2.2.3. 94 Sr: best experimenta
Page 31 and 32:
FIG. 2.2.15. 132 Te: best experimen
Page 33 and 34:
FIG. 2.2.27. 146 Ba: best experimen
Page 36 and 37:
3. EVALUATIONS 3.1. ACTINIDE NUCLEO
Page 38 and 39:
3.1.2. Statistical model At least t
Page 40 and 41:
J Â K=-J 2 2 2 ^ sym Krot ( U, J)
Page 42 and 43:
nuclei with N > 144. However, for h
Page 44 and 45:
neutron number. The observed fissio
Page 46 and 47:
FIG. 3.1.6. 235 U(n,f) fission cros
Page 48 and 49:
FIG. 3.1.10. 237 Np(n,f) fission cr
Page 50 and 51:
from higher fission chances [3.1.43
Page 52 and 53:
[3.1.48] DUSHIN, V.N., et al., Stat
Page 54 and 55:
where Y S is our new standard, and
Page 56 and 57:
TABLE 3.2.2. EVALUATED REFERENCE FI
Page 58 and 59:
TABLE 3.2.2. EVALUATED REFERENCE FI
Page 60 and 61:
TABLE 3.2.3. EVALUATED REFERENCE YI
Page 62 and 63:
TABLE 3.2.3. EVALUATED REFERENCE YI
Page 64 and 65:
The comparisons of our evaluated da
Page 66 and 67:
TABLE 3.2.4. COMPARISON OF RECOMMEN
Page 68 and 69:
Page 70 and 71:
Page 72 and 73:
Page 74 and 75:
Page 76 and 77:
Page 78 and 79:
Page 80 and 81:
Page 82 and 83:
Page 84 and 85:
Page 86 and 87:
Page 88 and 89:
Page 90 and 91:
Page 92 and 93:
Page 94 and 95:
TABLE 3.2.8. COMPARISON OF THE UNCE
Page 96:
REFERENCES TO SECTION 3.2 [3.2.1] I
Page 99 and 100:
where N C , N U are the modified an
Page 101 and 102:
activities were recorded with a pro
Page 103 and 104:
3.3.4. Results and discussion The r
Page 105 and 106:
FIG. 3.3.10. Li Ze et al. data: com
Page 107 and 108:
96 Annex 3.3.1 EVALUATED EXPERIMENT
Page 109 and 110:
Li Ze et al. [3.3.8] Thierens et al
Page 111 and 112:
100 Annex 3.3.3 EVALUATED DATA SET
Page 113 and 114:
The range of target nuclides availa
Page 115 and 116:
condensation of cross-sections by t
Page 117 and 118:
(h) REFERENCE (C,80KIEV,171,1980) i
Page 119 and 120:
uncertainties of the calculation. T
Page 122 and 123:
4. SYSTEMATICS AND MODELS FOR THE P
Page 124 and 125:
FIG. 4.1.2. 235 U total cross-secti
Page 126 and 127:
FIG. 4.1.9. Total and mode separate
Page 128 and 129:
4.2. SYSTEMATICS OF FISSION PRODUCT
Page 130 and 131:
A - = (PA - NT)/2 (4.2.1b) 4.2.2.3.
Page 132 and 133:
FIG. 4.2.4(a). 238 U + 5.5 MeV n, L
Page 134 and 135:
FIG. 4.2.8(a). U238 + 300 MeV p, LS
Page 136 and 137:
TABLE 4.2.1. EQUATIONS FOR SYSTEMAT
Page 138 and 139:
values (points) and the derived fun
Page 140 and 141:
distributions. Values of N(A) seldo
Page 142 and 143:
FIG. 4.2.19. Systematic Z P paramet
Page 144 and 145:
FIG. 4.2.21. Systematic Z P paramet
Page 146 and 147:
FIG. 4.2.23. Nuclear charge displac
Page 148 and 149:
FIG. 4.2.24. Number of protons emit
Page 150 and 151:
epresenting model values and thus s
Page 152 and 153:
FIG. 4.2.36. n T(A) for CF249T. FIG
Page 154 and 155:
FIG. 4.2.41. U235T, line: model; po
Page 156 and 157:
The FAST subroutine in the CYFP pro
Page 158 and 159:
[4.2.28] BELHAFAF, D., et al., Kine
Page 160 and 161:
4.3. FIVE GAUSSIAN SYSTEMATICS FOR
Page 162 and 163:
Derived from measured data Fitted r
Page 164 and 165:
FIG. 4.3.7. Mass distribution of 23
Page 166 and 167:
FFIG. 4.3.12. Mass distribution of
Page 168 and 169:
4.4. PHENOMENOLOGICAL MODEL FOR FRA
Page 170 and 171:
where = 2mE is the wavelength, E
Page 172 and 173:
FIG. 4.4.4. Fragment mass distribut
Page 174 and 175:
Page 176 and 177:
fragment mass distributions are des
Page 178 and 179:
Page 180 and 181:
FIG. 4.4.10. Fragment mass distribu
Page 182 and 183:
P LD È Ê * E - 44. 7ˆ ˘ = Í1 +
Page 184 and 185:
FIG. 4.4.13. Pre-neutron emission m
Page 186 and 187:
FIG. 4.4.15. Post-neutron emission
Page 188 and 189:
FIG. 4.4.17. Post-neutron emission
Page 190 and 191:
fragment mass and charge distributi
Page 192 and 193:
of the energy dependence of the fus
Page 194 and 195:
4.5. MODAL APPROACH TO THE DESCRIPT
Page 196 and 197:
This information was used for the p
Page 198 and 199:
two neighbouring isotopes at differ
Page 200 and 201:
FIG.4.5.2. Experimental relative ma
Page 202 and 203:
Frequently, the yields Y i (M) are
Page 204 and 205:
the nine optimum description parame
Page 206 and 207:
TABLE 4.5.6. RELATIVE CONTRIBUTIONS
Page 208 and 209:
TABLE 4.5.8. RELATIVE CONTRIBUTIONS
Page 210 and 211:
Extracted values of s 2 M,S demonst
Page 212 and 213:
FIG. 4.5.10. Fission fragment charg
Page 214 and 215:
FIG. 4.5.12. Unchanged charge densi
Page 216 and 217:
FIG. 4.5.16. Mass yield variance fo
Page 218 and 219:
FIG. 4.5.20. Experimental mass yiel
Page 220 and 221:
[4.5.24] GOVERDOVSKII, A.A., MITROF
Page 222 and 223:
TABLE 4.6.1. FISSION PRODUCT YIELD
Page 224 and 225:
TABLE 4.6.2. FIT PARAMETER VALUES O
Page 226 and 227:
FIG. 4.6.2. Charge distributions fo
Page 228 and 229:
model which is elucidated elsewhere
Page 230 and 231:
the agreement is better. The observ
Page 232 and 233:
inner barrier is much lower than th
Page 234 and 235:
e determined in a self-consistent m
Page 236 and 237:
FIG. 4.6.11. Overview of the coupli
Page 238 and 239:
cross-section also has to be incorp
Page 240 and 241:
FIG. 4.6.16. Same as Fig. 4.6.15, b
Page 242 and 243:
FIG. 4.6.20. Pre-neutron emission m
Page 244 and 245:
present have a reasonable contribut
Page 246 and 247:
TABLE 4.6.5. ACCURACIES OBTAINED FR
Page 248 and 249:
[4.6.7] BEIJERS, J.P.M., et al., Se
Page 250 and 251:
5. NEW MODELS AND SYSTEMATICS: DEFI
Page 252 and 253:
therefore his benchmark calculation
Page 254 and 255:
mass distributions and practically
Page 256 and 257:
5.2. BENCHMARK EXERCISE 5.2.1. Benc
Page 258 and 259:
thorough and detailed analysis of t
Page 260 and 261:
the fissioning nucleus and the numb
Page 262:
should be undertaken — such a stu
Page 265 and 266:
experimental method in order to der
Page 267 and 268:
256 Valley heights and peak-to-vall
Page 269 and 270: FIG. 6.2.3. Benchmark exercise, par
Page 271 and 272: 260 Wahl uncert. margins Wahl uncer
Page 275 and 276: 264 Wahl uncert. margins (adj. Wahl
Page 277 and 278: Wahl (1.6-160 MeV): Distributions a
Page 279 and 280: TABLE 6.2.2. 238 U PRE-NEUTRON EMIS
Page 281 and 282: as most features are very similar t
Page 283 and 284: FIG. 6.2.14. Benchmark exercise, pa
Page 289 and 290: 278 REFERENCES TO SECTION 6 [6.1] B
Page 291 and 292: As mentioned above, the mass distri
Page 293 and 294: I.3.2.6. Liu Conggui et al. [I.8] M
Page 295 and 296: after prompt-neutron emission, and
Page 297 and 298: 286 Zöller (1995) 89-110 MeV, post
Page 299 and 300: (1) Data were linearly interpolated
Page 301 and 302: 1. 290 Annex to Appendix I RECOMMEN
Page 303 and 304: 1.2. E n = 5.5 MeV 292 Nagy et al.
Page 305 and 306: 1.3. E n ª 8 MeV 294 Chapman (1978
Page 307 and 308: 1.5. E n = 14-15 MeV 296 Daroczy et
Page 309 and 310: 1.7. E n = 27.5 (22-33) MeV, Zölle
Page 311 and 312: 1.9. E n = 99.5 (89-110) MeV, Zöll
Page 313 and 314: 3. 302 239 Pu NEUTRON INDUCED FISSI
Page 316 and 317: Appendix II DATA ADJUSTMENT FOR MAS
Page 318 and 319: Vivès [II.8], Zöller [II.7] and
Page 322 and 323: Zöller (1995) [II.7] E n = 13 (11.
Page 324 and 325: E n = 50 (45-55) MeV Post-neutron e
Page 326 and 327: Äystö et al. (1998) [II.9] E p =
Page 328 and 329: E n = 1.60 MeV Pre-neutron emission
Page 330 and 331: E n = 27.5 (22-33) MeV Post-neutron
Page 332 and 333: E n = 99.5 (89-110) MeV Post-neutro
Page 334 and 335: Appendix III FISSION YIELD SYSTEMAT
Page 336 and 337: FIG. III.6. Dependence of chain yie
Page 338 and 339: TABLE III.2. Ln(y)-LINEAR(E) FIT CO
Page 340 and 341: FIG. III.14. Dependence of paramete
Page 342 and 343: FIG. III.26. Comparison of the mass
Page 344 and 345: FIG. III.38. Comparison of the mass
Page 346 and 347: TABLE III.3. QUADRATIC FUNCTION FIT
Page 348 and 349: Uncertainty ratio or uncertainty Ad
Page 350: CONTENTS OF THE CD-ROM The attached
Page 353: This publication reports on a coord
show all

Fission Product Yield Data for the Transmutation of Minor Actinide ...

You also want an ePaper? Increase the reach of your titles

Delete template?

Save as template?