81-Tl-201 JAEA EVAL-Sep21 N.Iwamoto DIST-DEC21 20210920 ----JENDL-5 MATERIAL 8119 -----INCIDENT NEUTRON DATA ------ENDF-6 FORMAT History 21-09 Evaluated with CCONE code by N.Iwamoto MF= 1 General information MT=451 Descriptive data and directory MF= 2 Resonance parameters MT=151 Scattering radius only AP is assumed to be 8.01 fm. Thermal cross sections and resonance integrals at 300 K ---------------------------------------------------------- 0.0253 eV res. integ. (*) (barn) (barn) ---------------------------------------------------------- Total 8.38118E+00 Elastic 8.07329E+00 n,gamma 2.69086E-01 8.63137E+00 n,p 7.05910E-17 2.43798E-15 n,alpha 5.60100E-13 1.91125E-11 ---------------------------------------------------------- (*) Integrated from 0.5 eV to 10 MeV. MF= 3 Neutron cross sections MT= 1 Total cross section Calculated with CCONE code /1/. MT= 2 Elastic scattering cross section Calculated with CCONE code /1/. MT= 4,51-91 (n,n') cross section Calculated with CCONE code /1/. MT= 5 Total reaction (except fission) cross section Calculated with CCONE code /1/. MT= 16 (n,2n) cross section Calculated with CCONE code /1/. MT= 17 (n,3n) cross section Calculated with CCONE code /1/. MT= 22 (n,na) cross section Calculated with CCONE code /1/. MT= 28 (n,np) cross section Calculated with CCONE code /1/. MT= 32 (n,nd) cross section Calculated with CCONE code /1/. MT= 33 (n,nt) cross section Calculated with CCONE code /1/. MT= 41 (n,2np) cross section Calculated with CCONE code /1/. MT=102 Capture cross section Calculated with CCONE code /1/. The thermal cross section was derived from Shibata/2/. Below 89.16 eV the 1/v cross section was assumed. MT=103,600-649 (n,p) cross section Calculated with CCONE code /1/. MT=104,650-699 (n,d) cross section Calculated with CCONE code /1/. MT=105,700-749 (n,t) cross section Calculated with CCONE code /1/. MT=106,750-799 (n,He3) cross section Calculated with CCONE code /1/. MT=107,800-849 (n,a) cross section Calculated with CCONE code /1/. MF= 4 Angular distributions of secondary particles MT= 2 Elastic scattering Calculated with CCONE code /1/. MF= 6 Energy-angle distributions of emitted particles MT= 5 Total reaction (except fission) reaction Calculated with CCONE code /1/. MT= 16 (n,2n) reaction Calculated with CCONE code /1/. MT= 17 (n,3n) reaction Calculated with CCONE code /1/. MT= 22 (n,na) reaction Calculated with CCONE code /1/. MT= 28 (n,np) reaction Calculated with CCONE code /1/. MT= 32 (n,nd) reaction Calculated with CCONE code /1/. MT= 33 (n,nt) reaction Calculated with CCONE code /1/. MT= 41 (n,2np) reaction Calculated with CCONE code /1/. MT= 51- 91 (n,n') reaction Calculated with CCONE code /1/. MT=102 Capture reaction Calculated with CCONE code /1/. MT=600-649 (n,p) reaction Calculated with CCONE code /1/. MT=650-699 (n,d) reaction Calculated with CCONE code /1/. MT=700-749 (n,t) reaction Calculated with CCONE code /1/. MT=750-799 (n,He3) reaction Calculated with CCONE code /1/. MT=800-849 (n,a) reaction Calculated with CCONE code /1/. MF= 8 Information on decay data MT= 4 (n,n') reaction Decay chain is given in the decay data file. MT= 5 Total reaction (except fission) reaction Decay chain is given in the decay data file. MT= 16 (n,2n) reaction Decay chain is given in the decay data file. MT= 17 (n,3n) reaction Decay chain is given in the decay data file. MT= 22 (n,na) reaction Decay chain is given in the decay data file. MT= 28 (n,np) reaction Decay chain is given in the decay data file. MT= 32 (n,nd) reaction Decay chain is given in the decay data file. MT= 33 (n,nt) reaction Decay chain is given in the decay data file. MT= 41 (n,2np) reaction Decay chain is given in the decay data file. MT=102 Capture reaction Decay chain is given in the decay data file. MT=103 (n,p) reaction Decay chain is given in the decay data file. MT=104 (n,d) reaction Decay chain is given in the decay data file. MT=105 (n,t) reaction Decay chain is given in the decay data file. MT=106 (n,He3) reaction Decay chain is given in the decay data file. MT=107 (n,a) reaction Decay chain is given in the decay data file. MF= 9 Isomeric branching ratios MT= 22 (n,na) reaction Calculated with CCONE code /1/. MF=10 Nuclide production reactions MT= 32 (n,nd) reaction Calculated with CCONE code /1/. MT= 41 (n,2np) reaction Calculated with CCONE code /1/. MT=105 (n,t) reaction Calculated with CCONE code /1/. ------------------------------------------------------------------ nuclear model calculation with CCONE code /1/ ------------------------------------------------------------------ * Optical model potentials neutron : S.Kunieda et al./3/ proton : global OMP, A.J.Koning and J.P.Delaroche/4/ deuteron: Y.Han et al./5/ triton : folding OMP, A.J.Koning and J.P.Delaroche/4/ He-3 : Y.Xu et al./6/ alpha : M.Avrigeanu and V.Avrigeanu/7/ * Level scheme of Tl-201 ----------------------- No. Ex(MeV) J PI ----------------------- 0 0.000000 1/2 + 1 0.331160 3/2 + 2 0.692510 5/2 + 3 0.919160 9/2 - 4 1.098500 5/2 + 5 1.134880 7/2 + 6 1.157430 5/2 + 7 1.238150 11/2 - 8 1.238800 3/2 + 9 1.277110 5/2 + 10 1.290110 9/2 + 11 1.330410 5/2 + 12 1.401260 5/2 + 13 1.413410 11/2 + 14 1.419000 11/2 - 15 1.419990 7/2 + 16 1.445860 5/2 + 17 1.479850 5/2 + 18 1.550590 5/2 + 19 1.571300 13/2 - 20 1.575100 7/2 + 21 1.617460 5/2 + 22 1.639350 5/2 + 23 1.671950 5/2 + 24 1.712450 7/2 + 25 1.725000 7/2 + 26 1.755320 5/2 + 27 1.763000 9/2 + 28 1.834000 3/2 + 29 1.908000 13/2 - 30 1.913000 3/2 + 31 1.940000 7/2 + 32 1.961900 15/2 - 33 1.987800 7/2 - 34 2.014500 13/2 - 35 2.040000 15/2 - 36 2.103000 9/2 + 37 2.145000 9/2 - 38 2.181700 11/2 - 39 2.196000 15/2 + 40 2.254000 15/2 - ----------------------- * Level density parameters (Gilbert-Cameron model/8/) Energy dependent parameters of Mengoni-Nakajima/9/ were used. --------------------------------------------------------- a* Pair Eshell T E0 Ematch Elv_max 1/MeV MeV MeV MeV MeV MeV MeV --------------------------------------------------------- Tl-202 23.519 0.000 -5.850 0.559 -0.361 3.582 2.150 Tl-201 23.422 0.846 -4.911 0.518 0.488 3.959 2.343 Tl-200 23.325 0.000 -4.344 0.481 -0.244 2.623 0.754 Tl-199 23.228 0.851 -3.524 0.465 0.517 3.435 2.032 Hg-201 26.313 0.846 -5.262 0.512 0.208 4.435 2.478 Hg-200 24.807 1.697 -4.720 0.612 0.009 7.528 2.491 Hg-199 26.369 0.851 -4.088 0.555 -0.748 5.953 0.969 Hg-198 23.131 1.706 -3.417 0.594 0.075 6.940 2.400 Hg-197 23.033 0.855 -2.645 0.573 -0.792 5.805 1.120 Au-200 23.325 0.000 -4.616 0.615 -1.400 5.367 0.060 Au-199 23.228 0.851 -3.846 0.533 0.043 4.585 1.849 Au-198 23.970 0.000 -3.421 0.552 -1.316 4.520 1.209 Au-197 23.033 0.855 -2.658 0.500 0.014 4.280 1.584 Au-196 22.936 0.000 -2.057 0.568 -1.787 4.997 1.244 Au-195 22.839 0.859 -1.473 0.457 0.124 3.801 1.781 --------------------------------------------------------- * Gamma-ray strength functions for Tl-202 E1: hybrid model(GH)/10/ ER= 13.82 (MeV) EG= 3.92 (MeV) SIG= 567.56 (mb) M1: standard lorentzian model(SLO) ER= 6.99 (MeV) EG= 4.00 (MeV) SIG= 1.08 (mb) E2: standard lorentzian model(SLO) ER= 10.74 (MeV) EG= 3.69 (MeV) SIG= 5.25 (mb) References 1) O.Iwamoto, J. Nucl. Sci. Technol., 44, 687 (2007) 2) K.Shibata, J. Nucl. Sci. Technol., 51, 425 (2014) 3) S.Kunieda et al., J. Nucl. Sci. Technol. 44, 838 (2007) 4) A.J.Koning and J.P.Delaroche, Nucl. Phys. A713, 231 (2003) 5) Y.Han et al., Phys. Rev. C 74,044615(2006) 6) Y.Xu et al., Sci. China, Phys. Mech. & Astron., 54[11], 2005 (2011) 7) M.Avrigeanu and V.Avrigeanu, Phys. Rev. C82, 014606 (2010) 8) A.Gilbert and A.G.W.Cameron, Can. J. Phys, 43, 1446 (1965) 9) A.Mengoni and Y.Nakajima, J. Nucl. Sci. Technol., 31, 151 (1994) 10) S.Goriely, Phys. Lett. B436, 10 (1998)