60-Nd-148

 60-Nd-148 JAEA+      EVAL-Dec09 N.Iwamoto,A.Zukeran,K.Shibata    
                      DIST-MAY10                       20100119   
----JENDL-4.0         MATERIAL 6043                               
-----INCIDENT NEUTRON DATA                                        
------ENDF-6 FORMAT                                               
                                                                  
History                                                           
09-12 The resolved resonance parameters were evaluated by         
      A.Zukeran,K.Shibata.                                        
      The data above the resolved resonance region were evaluated 
      and compiled by N.Iwamoto.                                  
                                                                  
MF= 1 General information                                         
  MT=451 Descriptive data and directory                           
                                                                  
MF= 2  Resonance parameters                                       
  MT=151 Resolved and unresolved resonance parameters             
    Resolved resonance region (MLBW formula): below 8.0 keV       
      Resonance energies were taken from Tellier/1/ and Musgrove  
      et al./2/  Neutron widths were adopted from Tellier, and    
      radiation widths were deduced from capture areas measured by
      Musgrove et al.  The average radiation widths were assumed  
      to be 0.046 eV for s-wave resonances and 0.040 eV for p-wave
      ones.  A negative resonance was added so as to reproduce the
      capture cross section of 2.5+-0.2 barns at 0.0253 eV/3/.    
      In JENDL-4, the data for 94.93 - 398.84 eV were replaced    
      with the ones obtained by Barry et al./4/  The parameters   
      for the negative resonance were re-adjusted.                
                                                                  
    Unresolved resonance region : 8.0 keV - 300.0 keV             
      The unresolved resonance paramters (URP) were determined by 
      ASREP code /5/ so as to reproduce the evaluated total and   
      capture cross sections calculated with optical model code   
      OPTMAN /6/ and CCONE /7/. The unresolved parameters         
      should be used only for self-shielding calculation.         
                                                                  
      Thermal cross sections and resonance integrals at 300 K     
      ----------------------------------------------------------  
                       0.0253 eV           res. integ. (*)        
                        (barn)               (barn)               
      ----------------------------------------------------------  
       Total           6.8516e+00                                 
       Elastic         4.2699e+00                                 
       n,gamma         2.5816e+00           1.3863e+01            
       n,alpha         3.0429e-10                                 
      ----------------------------------------------------------  
         (*) Integrated from 0.5 eV to 10 MeV.                    
                                                                  
MF= 3 Neutron cross sections                                      
  MT=  1 Total cross section                                      
    Sum of partial cross sections.                                
                                                                  
  MT=  2 Elastic scattering cross section                         
    Obtained by subtracting non-elastic scattering cross sections 
      from total cross section.                                   
                                                                  
  MT=  4 (n,n') cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 16 (n,2n) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 17 (n,3n) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 22 (n,na) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 24 (n,2na) cross section                                    
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 28 (n,np) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 32 (n,nd) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 33 (n,nt) cross section                                     
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 51-91 (n,n') cross section                                  
    Calculated with CCONE code /7/.                               
                                                                  
  MT=102 Capture cross section                                    
    Calculated with CCONE code /7/.                               
                                                                  
  MT=103 (n,p) cross section                                      
    Calculated with CCONE code /7/.                               
                                                                  
  MT=104 (n,d) cross section                                      
    Calculated with CCONE code /7/.                               
                                                                  
  MT=105 (n,t) cross section                                      
    Calculated with CCONE code /7/.                               
                                                                  
  MT=106 (n,He3) cross section                                    
    Calculated with CCONE code /7/.                               
                                                                  
  MT=107 (n,a) cross section                                      
    Calculated with CCONE code /7/.                               
                                                                  
MF= 4 Angular distributions of emitted neutrons                   
  MT=  2 Elastic scattering                                       
    Calculated with CCONE code /7/.                               
                                                                  
MF= 6 Energy-angle distributions of emitted particles             
  MT= 16 (n,2n) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 17 (n,3n) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 22 (n,na) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 24 (n,2na) reaction                                         
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 28 (n,np) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 32 (n,nd) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 33 (n,nt) reaction                                          
    Calculated with CCONE code /7/.                               
                                                                  
  MT= 51-91 (n,n') reaction                                       
    Calculated with CCONE code /7/.                               
                                                                  
  MT=102 Capture reaction                                         
    Calculated with CCONE code /7/.                               
                                                                  
                                                                  
                                                                  
***************************************************************** 
       Nuclear Model Calculation with CCONE code /7/              
***************************************************************** 
                                                                  
  Models and parameters used in the CCONE calculation             
  1) Optical model                                                
    * coupled channels calculation                                
      coupled levels: 0,1,2,4 (see Table 1)                       
                                                                  
    * optical model potential                                     
      neutron  omp: Kunieda,S. et al./8/ (+)                      
      proton   omp: Koning,A.J. and Delaroche,J.P./9/             
      deuteron omp: Lohr,J.M. and Haeberli,W./10/                 
      triton   omp: Becchetti Jr.,F.D. and Greenlees,G.W./11/     
      He3      omp: Becchetti Jr.,F.D. and Greenlees,G.W./11/     
      alpha    omp: McFadden,L. and Satchler,G.R./12/             
      (+) omp parameters were modified.                           
                                                                  
  2) Two-component exciton model/13/                              
    * Global parametrization of Koning-Duijvestijn/14/            
      was used.                                                   
    * Gamma emission channel/15/ was added to simulate direct     
      and semi-direct capture reaction.                           
                                                                  
  3) Hauser-Feshbach statistical model                            
    * Width fluctuation correction/16/ was applied.               
    * Neutron, proton, deuteron, triton, He3, alpha and gamma     
      decay channel were taken into account.                      
    * Transmission coefficients of neutrons were taken from       
      optical model calculation.                                  
    * The level scheme of the target is shown in Table 1.         
    * Level density formula of constant temperature and Fermi-gas 
      model were used with shell energy correction/17/.           
      Parameters are shown in Table 2.                            
    * Gamma-ray strength function of enhanced generalized         
      Lorentzian form/18/,/19/ was used for E1 transition.        
      For M1 and E2 transitions the standard Lorentzian form was  
      adopted. The prameters are shown in Table 3.                
                                                                  
                                                                  
------------------------------------------------------------------
                              Tables                              
------------------------------------------------------------------
                                                                  
Table 1. Level Scheme of Nd-148                                   
  -------------------                                             
  No.  Ex(MeV)  J  PI                                             
  -------------------                                             
   0  0.00000   0  +  *                                           
   1  0.30170   2  +  *                                           
   2  0.75220   4  +  *                                           
   3  0.91680   0  +                                              
   4  0.99920   3  -  *                                           
   5  1.02312   1  -                                              
   6  1.17090   2  +                                              
   7  1.24214   5  -                                              
   8  1.24881   2  +                                              
   9  1.27969   6  +                                              
  10  1.40000   0  +                                              
  11  1.43200   1  -                                              
  12  1.47500   1  -                                              
  13  1.51151   3  +                                              
  14  1.51560   2  -                                              
  15  1.52146   1  -                                              
  16  1.57700   2  +                                              
  17  1.60000   0  +                                              
  18  1.60200   4  +                                              
  19  1.64460   7  -                                              
  20  1.64558   0  +                                              
  21  1.65400   3  -                                              
  22  1.65991   2  +                                              
  23  1.68340   4  +                                              
  24  1.68791   3  +                                              
  25  1.72500   3  -                                              
  26  1.72900   3  +                                              
  27  1.77800   3  -                                              
  28  1.80860   0  +                                              
  29  1.82440   0  +                                              
  30  1.83700   1  -                                              
  31  1.85630   8  +                                              
  32  1.85860   0  +                                              
  33  1.88700   4  +                                              
  -------------------                                             
  *) Coupled levels in CC calculation                             
                                                                  
Table 2. Level density parameters                                 
  --------------------------------------------------------        
  Nuclide      a*    Pair  Eshell       T      E0  Ematch         
            1/MeV     MeV     MeV     MeV     MeV     MeV         
  --------------------------------------------------------        
   Nd-149 20.9000  0.9831  3.5199  0.4992 -1.1865  5.3955         
   Nd-148 21.1000  1.9728  2.8636  0.4784  0.2048  5.9010         
   Nd-147 19.7000  0.9897  2.4886  0.4934 -0.5694  4.7470         
   Nd-146 18.1900  1.9863  1.6792  0.5692  0.1138  6.4542         
   Pr-148 15.5000  0.0000  3.2403  0.6014 -1.8696  4.4395         
   Pr-147 17.0632  0.9897  3.0053  0.5856 -1.1357  5.6888         
   Pr-146 17.5893  0.0000  2.4188  0.5462 -1.6453  4.0472         
   Pr-145 16.8637  0.9965  1.7883  0.6002 -0.8883  5.5766         
   Ce-147 18.4207  0.9897  2.8111  0.5589 -1.1482  5.6286         
   Ce-146 17.6964  1.9863  2.1733  0.5745  0.0448  6.5077         
   Ce-145 18.2180  0.9965  1.7406  0.5686 -0.8969  5.4793         
   Ce-144 17.4894  2.0000  1.0129  0.5822  0.3675  6.2813         
   Ce-143 19.6000  1.0035  0.4100  0.4774  0.1189  3.9645         
   Ce-142 18.9500  2.0140 -0.3155  0.5558  0.6875  5.9346         
  --------------------------------------------------------        
                                                                  
Table 3. Gamma-ray strength function for Nd-149                   
  --------------------------------------------------------        
  K0 = 1.800   E0 = 4.500 (MeV)                                   
  * E1: ER = 12.97 (MeV) EG = 3.47 (MeV) SIG = 122.11 (mb)        
        ER = 15.97 (MeV) EG = 5.17 (MeV) SIG = 244.23 (mb)        
  * M1: ER =  7.73 (MeV) EG = 4.00 (MeV) SIG =   1.12 (mb)        
  * E2: ER = 11.88 (MeV) EG = 4.32 (MeV) SIG =   3.33 (mb)        
  --------------------------------------------------------        
                                                                  
References                                                        
 1) Tellier, H.: CEA-N-1459 (1971).                               
 2) Musgrove, A.R. de L., et al.: AEEC/E401 (1977).               
 3) Fedorova, A.F., et al.: "Proc. 3rd All-union Conf. on Neutron 
    Physics, Kiev 1975", Vol. 1, 169.                             
 4) Barry, D.P. et al.: Nucl. Sci. Eng., 153, 8 (2006).           
 5) Kikuchi,Y. et al.: JAERI-Data/Code 99-025 (1999)              
    [in Japanese].                                                
 6) Soukhovitski,E.Sh. et al.: JAERI-Data/Code 2005-002 (2004).   
 7) Iwamoto,O.: J. Nucl. Sci. Technol., 44, 687 (2007).           
 8) Kunieda,S. et al.: J. Nucl. Sci. Technol. 44, 838 (2007).     
 9) Koning,A.J. and Delaroche,J.P.: Nucl. Phys. A713, 231 (2003)  
    [Global potential].                                           
10) Lohr,J.M. and Haeberli,W.: Nucl. Phys. A232, 381 (1974).      
11) Becchetti Jr.,F.D. and Greenlees,G.W.: Ann. Rept.             
    J.H.Williams Lab., Univ. Minnesota (1969).                    
12) McFadden,L. and Satchler,G.R.: Nucl. Phys. 84, 177 (1966).    
13) Kalbach,C.: Phys. Rev. C33, 818 (1986).                       
14) Koning,A.J., Duijvestijn,M.C.: Nucl. Phys. A744, 15 (2004).   
15) Akkermans,J.M., Gruppelaar,H.: Phys. Lett. 157B, 95 (1985).   
16) Moldauer,P.A.: Nucl. Phys. A344, 185 (1980).                  
17) Mengoni,A. and Nakajima,Y.: J. Nucl. Sci. Technol., 31, 151   
    (1994).                                                       
18) Kopecky,J., Uhl,M.: Phys. Rev. C41, 1941 (1990).              
19) Kopecky,J., Uhl,M., Chrien,R.E.: Phys. Rev. C47, 312 (1990).