JENDL-5 (Neutron sublibrary (activation cs)) Ce-144 0 0 0 0 5.814400+4 1.426774+2 0 0 6 15849 1451 1 0.000000+0 1.000000+0 0 0 0 65849 1451 2 1.000000+0 2.000000+7 0 0 10 55849 1451 3 2.936000+2 0.000000+0 4 0 269 265849 1451 4 58-Ce-144 JAEA EVAL-FEB22 S.Kunieda, A.Ichihara, K.Shibata+5849 1451 5 DIST-DEC21 20100225 5849 1451 6 ----JENDL-5 MATERIAL 5849 5849 1451 7 -----INCIDENT NEUTRON DATA 5849 1451 8 ------ENDF-6 FORMAT 5849 1451 9 5849 1451 10 History 5849 1451 11 10-02 Re-evaluation was performed for JENDL-4 5849 1451 12 (compiled by S. Kunieda). 5849 1451 13 21-11 revised by O.Iwamoto 5849 1451 14 (MF8/MT4,16,17,22,28,32,102-107) added 5849 1451 15 5849 1451 16 MF= 1 General information 5849 1451 17 5849 1451 18 MT=451 Descriptive data and directory 5849 1451 19 5849 1451 20 5849 1451 21 MF= 2 Resonance parameters 5849 1451 22 5849 1451 23 MT=151 Resolved and unresolved resonance parameters 5849 1451 24 5849 1451 25 - No resolved resonance parameters are given. 5849 1451 26 No measurement has been done for resonance parameters of 5849 1451 27 Ce-144. Cross sections in a low energy region were assumed 5849 1451 28 that the capture was in a 1/v shape with a value of 1.0+-0.15849 1451 29 b/1/ at 0.0253 eV, and the elastic scattering was a 5849 1451 30 constant of 2.78 b calculated from a scattering radius of 5849 1451 31 4.7 fm. 5849 1451 32 5849 1451 33 - Unresolved resonance region: 50 eV - 200 keV 5849 1451 34 The parameters were obtained by fitting to the total and 5849 1451 35 capture cross sections calculated by the POD code /2/. 5849 1451 36 The ASREP code /3/ was employed in this evaluation. 5849 1451 37 The unresolved parameters should be used only for 5849 1451 38 self-shielding calculation. 5849 1451 39 5849 1451 40 Thermal cross sections & resonance integrals at 300 K 5849 1451 41 ---------------------------------------------------------- 5849 1451 42 0.0253 eV res. integ. (*) 5849 1451 43 (barns) (barns) 5849 1451 44 ---------------------------------------------------------- 5849 1451 45 Total 3.79387E+00 5849 1451 46 Elastic 2.79150E+00 5849 1451 47 n,gamma 1.00043E+00 7.63278E+00 5849 1451 48 ---------------------------------------------------------- 5849 1451 49 (*) Integrated from 0.5 eV to 10 MeV. 5849 1451 50 5849 1451 51 5849 1451 52 MF= 3 Neutron cross sections 5849 1451 53 5849 1451 54 MT= 1 Total cross section 5849 1451 55 Sum of partial cross sections. 5849 1451 56 5849 1451 57 MT= 2 Elastic scattering cross section 5849 1451 58 The OPTMAN /4/ & POD calculations /2/. 5849 1451 59 5849 1451 60 MT= 3 Non-elastic cross section 5849 1451 61 Sum of partial non-elastic cross sections. 5849 1451 62 5849 1451 63 MT= 4,51-91 (n,n') cross section 5849 1451 64 The OPTMAN /4/ & POD calculations /2/. 5849 1451 65 5849 1451 66 MT= 16 (n,2n) cross section 5849 1451 67 MT= 17 (n,3n) cross section 5849 1451 68 MT= 22 (n,na) cross section 5849 1451 69 MT= 28 (n,np) cross section 5849 1451 70 MT= 32 (n,nd) cross section 5849 1451 71 MT=102 Capture cross section 5849 1451 72 MT=103 (n,p) cross section 5849 1451 73 MT=104 (n,d) cross section 5849 1451 74 MT=105 (n,t) cross section 5849 1451 75 MT=106 (n,He3) cross section 5849 1451 76 MT=107 (n,a) cross section 5849 1451 77 Calculated by the POD code /2/. 5849 1451 78 5849 1451 79 MT=203 (n,xp) cross section 5849 1451 80 Sum of (n,np) and (n,p) 5849 1451 81 5849 1451 82 MT=204 (n,xd) cross section 5849 1451 83 Sum of (n,nd) and (n,d) 5849 1451 84 5849 1451 85 MT=205 (n,xt) cross section 5849 1451 86 MT=206 (n,xHe3) cross section 5849 1451 87 Calculated by the POD code /2/. 5849 1451 88 5849 1451 89 MT=207 (n,xa) cross section 5849 1451 90 Sum of (n,na) and (n,a) 5849 1451 91 5849 1451 92 5849 1451 93 MF= 4 Angular distributions of emitted neutrons 5849 1451 94 5849 1451 95 MT= 2 Elastic scattering 5849 1451 96 The OPTMAN /4/ & POD calculations /2/. 5849 1451 97 5849 1451 98 5849 1451 99 MF= 6 Energy-angle distributions of emitted particles 5849 1451 100 5849 1451 101 MT= 16 (n,2n) reaction 5849 1451 102 MT= 17 (n,3n) reaction 5849 1451 103 MT= 22 (n,na) reaction 5849 1451 104 MT= 28 (n,np) reaction 5849 1451 105 MT= 32 (n,nd) reaction 5849 1451 106 Neutron spectra calculated by the POD code /2/. 5849 1451 107 5849 1451 108 MT= 51-90 (n,n') reaction 5849 1451 109 Neutron angular distributions calculated by 5849 1451 110 OPTMAN /4/ & POD /2/. 5849 1451 111 5849 1451 112 MT= 91 (n,n') reaction 5849 1451 113 Neutron spectra calculated by the POD code /2/. 5849 1451 114 5849 1451 115 MT= 203 (n,xp) reaction 5849 1451 116 MT= 204 (n,xd) reaction 5849 1451 117 MT= 205 (n,xt) reaction 5849 1451 118 MT= 206 (n,xHe3) reaction 5849 1451 119 MT= 207 (n,xa) reaction 5849 1451 120 Light-ion spectra calculated by the POD code /6/. 5849 1451 121 5849 1451 122 5849 1451 123 MF=12 Gamma-ray multiplicities 5849 1451 124 5849 1451 125 MT= 3 Non-elastic gamma emission 5849 1451 126 Calculated by the POD code /2/. 5849 1451 127 5849 1451 128 5849 1451 129 MF=14 Gamma-ray angular distributions 5849 1451 130 5849 1451 131 MT= 3 Non-elastic gamma emission 5849 1451 132 Assumed to be isotropic. 5849 1451 133 5849 1451 134 5849 1451 135 MF=15 Gamma-ray spectra 5849 1451 136 5849 1451 137 MT= 3 Non-elastic gamma emission 5849 1451 138 Calculated by the POD code /2/. 5849 1451 139 5849 1451 140 5849 1451 141 5849 1451 142 5849 1451 143 *************************************************************** 5849 1451 144 * Nuclear Model Calculations with POD Code /2/ * 5849 1451 145 *************************************************************** 5849 1451 146 1. Theoretical models 5849 1451 147 The POD code is based on the spherical optical model, the 5849 1451 148 distorted-wave Born approximaiton (DWBA), one-component exciton 5849 1451 149 preequilibrium model, and the Hauser-Feshbach-Moldauer statis- 5849 1451 150 tical model. With the preequilibrium model, semi-empirical 5849 1451 151 pickup and knockout process can be taken into account for 5849 1451 152 composite-particle emission. The gamma-ray emission from the 5849 1451 153 compound nucleus can be calculated within the framework of the 5849 1451 154 exciton model. The code is capable of reading in particle 5849 1451 155 transmission coefficients calculated by separate spherical or 5849 1451 156 coupled-channel optical model code. In this evaluation, the OPTMAN5849 1451 157 code /4/ was employed for neutrons, while the ECIS code 5849 1451 158 /5/ was adopted for charged particles. 5849 1451 159 5849 1451 160 2. Optical model & parameters 5849 1451 161 Neutrons: 5849 1451 162 Model: Coupled-channel model based on the rigid-rotor model 5849 1451 163 OMP : Based on the Coupled-channel optical potential /6/ 5849 1451 164 The original Parameters were slightly modified as 5849 1451 165 listed below to reproduce experimental total cross 5849 1451 166 sections measured by Camarda et al /7/. 5849 1451 167 ------------------------------------------------------------ 5849 1451 168 - Real-volume term 5849 1451 169 VR0= -3.85E+1 MeV VR1= 2.70E-2 MeV VR2= 1.20E-4 MeV 5849 1451 170 VR3= 3.50E-7 MeV VRLA= 9.49E+1 MeV ALAVR= 4.22E-3 5849 1451 171 r= 1.21E+0 a= 6.30E-1 5849 1451 172 - Imaginary-surface term 5849 1451 173 WDBW= 1.30E+1 MeV WDWID= 1.40E+1 MeV ALAWD= 1.40E-2 5849 1451 174 r= 1.21E+0 a= 6.75E-1 5849 1451 175 - Imaginary-volume term 5849 1451 176 WCBW= 1.70E+1 MeV WCWID= 1.05E+2 MeV 5849 1451 177 r= 1.21E+0 a= 6.75E-1 5849 1451 178 - Spin-orbit term 5849 1451 179 VS= 6.35E+0 MeV ALASO= 5.00E-3 5849 1451 180 WSBW= -3.10E+0 MeV WSWID= 1.60E+2 MeV 5849 1451 181 r= 1.06E+0 a= 5.90E-1 5849 1451 182 - Isospin coefficients 5849 1451 183 CISO= 2.43E+1 WCISO= 1.80E+1 CCOUL= 9.00E-1 5849 1451 184 - Deformation parameter 5849 1451 185 Beta2= -1.66E-1 5849 1451 186 ------------------------------------------------------------ 5849 1451 187 Protons: 5849 1451 188 Model: Spherical 5849 1451 189 OMP : Koning and Delaroche /8/ 5849 1451 190 Deuterons: 5849 1451 191 Model: Spherical 5849 1451 192 OMP : Bojowald et al. /9/ 5849 1451 193 Tritons: 5849 1451 194 Mode: Spherical 5849 1451 195 OMP : Becchetti and Greenlees /10/ 5849 1451 196 He-3: 5849 1451 197 Model: Spherical 5849 1451 198 OMP : Becchetti and Greenlees /10/ 5849 1451 199 Alphas: 5849 1451 200 Model: Spherical 5849 1451 201 OMP : A simplified folding model potential /11/ 5849 1451 202 (The nucleon OMP was taken form Ref./6/.) 5849 1451 203 5849 1451 204 3. Level scheme of Ce-144 5849 1451 205 ------------------------------------ 5849 1451 206 No. Ex(MeV) J PI CC 5849 1451 207 ------------------------------------ 5849 1451 208 0 0.00000 0 + * 5849 1451 209 1 0.39744 2 + * 5849 1451 210 2 0.93865 4 + * 5849 1451 211 3 1.24221 3 - 5849 1451 212 4 1.34610 1 - 5849 1451 213 5 1.48900 2 + 5849 1451 214 6 1.52367 5 - 5849 1451 215 7 1.67367 4 + 5849 1451 216 8 1.69153 3 + 5849 1451 217 9 1.81900 2 + 5849 1451 218 10 1.82901 4 + 5849 1451 219 11 1.86450 1 + 5849 1451 220 12 1.89092 3 - 5849 1451 221 13 1.99155 3 - 5849 1451 222 14 2.02110 3 + 5849 1451 223 ------------------------------------ 5849 1451 224 Levels above 2.03110 MeV are assumed to be continuous. 5849 1451 225 5849 1451 226 5849 1451 227 4. Level density parameters 5849 1451 228 Energy-dependent parameters of Mengoni-Nakajima /12/ were used 5849 1451 229 ---------------------------------------------------------- 5849 1451 230 Nuclei a* Pair Esh T E0 Ematch Elv_max 5849 1451 231 1/MeV MeV MeV MeV MeV MeV MeV 5849 1451 232 ---------------------------------------------------------- 5849 1451 233 Ce-145 18.218 0.997 1.745 0.530 -0.507 5.270 0.447 5849 1451 234 Ce-144 17.489 2.000 1.018 0.565 0.516 6.430 2.021 5849 1451 235 Ce-143 18.015 1.003 0.415 0.562 -0.412 5.329 1.173 5849 1451 236 Ce-142 17.282 2.014 -0.311 0.610 0.530 6.671 2.365 5849 1451 237 La-144 17.385 0.000 1.211 0.544 -1.291 4.082 0.182 5849 1451 238 La-143 16.664 1.003 0.848 0.656 -1.207 6.787 0.466 5849 1451 239 La-142 17.180 0.000 -0.112 0.617 -1.592 4.824 0.361 5849 1451 240 Ba-142 17.282 2.014 0.008 0.629 0.211 7.159 1.640 5849 1451 241 Ba-141 17.811 1.011 -0.683 0.588 -0.270 5.296 1.117 5849 1451 242 Ba-140 17.074 2.028 -1.371 0.607 1.003 6.085 2.704 5849 1451 243 ---------------------------------------------------------- 5849 1451 244 5849 1451 245 5. Gamma-ray strength functions 5849 1451 246 M1, E2: Standard Lorentzian (SLO) 5849 1451 247 E1 : Generalized Lorentzian (GLO) /13/ 5849 1451 248 5849 1451 249 6. Preequilibrium process 5849 1451 250 Preequilibrium is on for n, p, d, t, He-3, and alpha. 5849 1451 251 Preequilibrium capture is on. 5849 1451 252 5849 1451 253 5849 1451 254 References 5849 1451 255 1) P.M.Lantz: Nucl. Sci. Eng., 13, 289 (1962). 5849 1451 256 2) A.Ichihara et al., JAEA-Data/Code 2007-012 (2007). 5849 1451 257 3) Y.Kikuchi et al., JAERI-Data/Code 99-025 (1999) 5849 1451 258 [in Japanese]. 5849 1451 259 4) E.Soukhovitski et al., JAERI-Data/Code 2005-002 (2005). 5849 1451 260 5) J.Raynal, CEA Saclay report, CEA-N-2772 (1994). 5849 1451 261 6) S.Kunieda et al., J. Nucl. Sci. Technol. 44, 838 (2007). 5849 1451 262 7) Camarda et al., Phys. Rev. C 29, 2106 (1984). 5849 1451 263 8) A.J.Koning, J.P.Delaroche, Nucl. Phys. A713, 231 (2003). 5849 1451 264 9) Bojowald et al., Phys. Rev. C 38, 1153 (1988). 5849 1451 265 10) F.D.Becchetti,Jr., G.W.Greenlees, "Polarization 5849 1451 266 Phenomena in Nuclear Reactions," p.682, The University 5849 1451 267 of Wisconsin Press (1971). 5849 1451 268 11) D.G.Madland, NEANDC-245 (1988), p. 103. 5849 1451 269 12) A.Mengoni, Y.Nakajima, J. Nucl. Sci. Technol. 31, 151 5849 1451 270 (1994). 5849 1451 271 13) M.Brink, Ph.D thesis, Oxford University, 1955. 5849 1451 272 5849 1451 273 1 451 299 15849 1451 274 2 151 4 15849 1451 275 3 4 25 15849 1451 276 3 16 9 15849 1451 277 3 17 6 15849 1451 278 3 22 9 15849 1451 279 3 28 7 15849 1451 280 3 32 5 15849 1451 281 3 102 178 15849 1451 282 3 103 9 15849 1451 283 3 104 7 15849 1451 284 3 105 7 15849 1451 285 3 106 5 15849 1451 286 3 107 13 15849 1451 287 8 4 2 15849 1451 288 8 16 2 15849 1451 289 8 17 2 15849 1451 290 8 22 2 15849 1451 291 8 28 2 15849 1451 292 8 32 2 15849 1451 293 8 102 2 15849 1451 294 8 103 2 15849 1451 295 8 104 2 15849 1451 296 8 105 2 15849 1451 297 8 106 2 15849 1451 298 8 107 2 15849 1451 299 5849 1 099999 5849 0 0 0 5.814400+4 1.426774+2 0 0 1 05849 2151 1 5.814400+4 1.000000+0 0 0 1 05849 2151 2 5.000000+1 2.000000+5 0 0 0 05849 2151 3 0.000000+0 4.000000-1 0 0 0 05849 2151 4 5849 2 099999 5849 0 0 0 5.814400+4 1.426774+2 0 0 0 05849 3 4 1 0.000000+0-3.974410+5 0 0 1 655849 3 4 2 65 2 5849 3 4 3 4.002266+5 0.000000+0 4.500000+5 4.635000-1 5.000000+5 6.287000-15849 3 4 4 5.500000+5 7.648000-1 6.000000+5 8.856000-1 6.500000+5 9.984000-15849 3 4 5 7.000000+5 1.107000+0 7.500000+5 1.210000+0 8.000000+5 1.308000+05849 3 4 6 8.500000+5 1.401000+0 9.000000+5 1.486000+0 9.452288+5 1.551129+05849 3 4 7 9.500000+5 1.568000+0 1.000000+6 1.644110+0 1.200000+6 1.879980+05849 3 4 8 1.250916+6 1.880240+0 1.355535+6 1.961614+0 1.400000+6 2.106600+05849 3 4 9 1.499436+6 2.104661+0 1.534349+6 2.161229+0 1.600000+6 2.270983+05849 3 4 10 1.685400+6 2.249457+0 1.703386+6 2.249192+0 1.800000+6 2.323190+05849 3 4 11 1.831749+6 2.293748+0 1.841829+6 2.290768+0 1.877568+6 2.286487+05849 3 4 12 1.904173+6 2.298492+0 2.000000+6 2.373350+0 2.005508+6 2.375468+05849 3 4 13 2.035266+6 2.393307+0 2.045336+6 2.402711+0 2.200000+6 2.548469+05849 3 4 14 2.400000+6 2.540052+0 2.600000+6 2.548154+0 2.800000+6 2.564646+05849 3 4 15 3.000000+6 2.581330+0 3.250000+6 2.595870+0 3.500000+6 2.595250+05849 3 4 16 3.750000+6 2.582395+0 4.000000+6 2.558395+0 4.250000+6 2.526792+05849 3 4 17 4.500000+6 2.488730+0 4.750000+6 2.447707+0 5.000000+6 2.406607+05849 3 4 18 5.500000+6 2.336941+0 6.000000+6 2.293371+0 6.500000+6 2.277343+05849 3 4 19 7.000000+6 2.277118+0 7.500000+6 1.948843+0 8.000000+6 1.379260+05849 3 4 20 8.500000+6 1.029687+0 9.000000+6 7.864052-1 9.500000+6 6.448209-15849 3 4 21 1.000000+7 5.589390-1 1.100000+7 4.504258-1 1.200000+7 3.652253-15849 3 4 22 1.300000+7 3.302560-1 1.400000+7 3.052659-1 1.500000+7 2.864974-15849 3 4 23 1.600000+7 2.698223-1 1.700000+7 2.560290-1 1.800000+7 2.439460-15849 3 4 24 1.900000+7 2.329378-1 2.000000+7 2.223969-1 5849 3 4 25 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3 16 1 -6.896306+6-6.896306+6 0 0 1 185849 3 16 2 18 2 5849 3 16 3 6.944641+6 0.000000+0 7.000000+6 0.000000+0 7.500000+6 3.344000-15849 3 16 4 8.000000+6 9.090000-1 8.500000+6 1.259000+0 9.000000+6 1.497000+05849 3 16 5 9.500000+6 1.630000+0 1.000000+7 1.704000+0 1.100000+7 1.790000+05849 3 16 6 1.200000+7 1.857000+0 1.300000+7 1.869000+0 1.400000+7 1.753000+05849 3 16 7 1.500000+7 1.454000+0 1.600000+7 1.120000+0 1.700000+7 8.473000-15849 3 16 8 1.800000+7 6.301000-1 1.900000+7 4.807000-1 2.000000+7 3.820000-15849 3 16 9 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3 17 1 -1.204114+7-1.204114+7 0 0 1 95849 3 17 2 9 2 5849 3 17 3 1.212554+7 0.000000+0 1.300000+7 1.196000-2 1.400000+7 1.460000-15849 3 17 4 1.500000+7 4.572000-1 1.600000+7 7.981000-1 1.700000+7 1.070000+05849 3 17 5 1.800000+7 1.278000+0 1.900000+7 1.411000+0 2.000000+7 1.488000+05849 3 17 6 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3 22 1 4.094632+5 4.094632+5 0 0 1 165849 3 22 2 16 2 5849 3 22 3 1.000000-5 0.000000+0 2.530000-2 0.000000+0 8.500000+6 0.000000+05849 3 22 4 9.000000+6 3.690000-7 9.500000+6 1.687000-6 1.000000+7 4.427000-65849 3 22 5 1.100000+7 1.772000-5 1.200000+7 5.389000-5 1.300000+7 1.486000-45849 3 22 6 1.400000+7 3.815000-4 1.500000+7 8.858000-4 1.600000+7 1.801000-35849 3 22 7 1.700000+7 3.189000-3 1.800000+7 5.004000-3 1.900000+7 7.103000-35849 3 22 8 2.000000+7 9.340000-3 5849 3 22 9 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3 28 1 -9.538886+6-9.538886+6 0 0 1 105849 3 28 2 10 2 5849 3 28 3 9.605743+6 0.000000+0 1.200000+7 0.000000+0 1.300000+7 1.225000-75849 3 28 4 1.400000+7 5.140000-6 1.500000+7 5.598000-5 1.600000+7 3.126000-45849 3 28 5 1.700000+7 1.146000-3 1.800000+7 3.113000-3 1.900000+7 6.685000-35849 3 28 6 2.000000+7 1.205000-2 5849 3 28 7 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3 32 1 -1.353794+7-1.353794+7 0 0 1 55849 3 32 2 5 2 5849 3 32 3 1.363282+7 0.000000+0 1.700000+7 0.000000+0 1.800000+7 7.280000-75849 3 32 4 1.900000+7 1.732000-5 2.000000+7 1.555000-4 5849 3 32 5 5849 3 099999 5.814400+4 1.426774+2 0 0 0 05849 3102 1 4.731167+6 4.731167+6 0 0 1 5245849 3102 2 524 2 5849 3102 3 1.000000-5 5.029943+1 1.103037-5 4.789255+1 1.216691-5 4.560085+15849 3102 4 1.342055-5 4.341881+1 1.480336-5 4.134118+1 1.632865-5 3.936297+15849 3102 5 1.801111-5 3.747942+1 1.986691-5 3.568600+1 2.191394-5 3.397839+15849 3102 6 2.417189-5 3.235249+1 2.666248-5 3.080440+1 2.940971-5 2.933038+15849 3102 7 3.243999-5 2.792690+1 3.578251-5 2.659057+1 3.946943-5 2.531819+15849 3102 8 4.353624-5 2.410669+1 4.802208-5 2.295316+1 5.297013-5 2.185484+15849 3102 9 5.842801-5 2.080906+1 6.444825-5 1.981333+1 7.108881-5 1.886525+15849 3102 10 7.841358-5 1.796253+1 8.649308-5 1.710300+1 9.540506-5 1.628461+15849 3102 11 1.052353-4 1.550538+1 1.160784-4 1.476343+1 1.280388-4 1.405699+15849 3102 12 1.412315-4 1.338435+1 1.557836-4 1.274390+1 1.718351-4 1.213409+15849 3102 13 1.895404-4 1.155346+1 2.090701-4 1.100062+1 2.306120-4 1.047423+15849 3102 14 2.543736-4 9.973031+0 2.805835-4 9.495813+0 3.094939-4 9.041430+05849 3102 15 3.413832-4 8.608790+0 3.765583-4 8.196852+0 4.153577-4 7.804625+05849 3102 16 4.581549-4 7.431167+0 5.053618-4 7.075580+0 5.574328-4 6.737007+05849 3102 17 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