47-Ag- 0

 47-AG-  0 JAERI      EVAL-MAR87 LIU T.J.,T.NAKAGAWA,K.SHIBATA    
                      DIST-SEP89 REV2-FEB94                       
----JENDL-3.2         MATERIAL 4700                               
-----INCIDENT NEUTRON DATA                                        
------ENDF-6 FORMAT                                               
HISTORY                                                           
87-03 NEW EVALUATION FOR JENDL-3/1/                               
87-07 COMPILED BY K.SHIBATA                                       
94-02 JENDL-3.2 WAS MADE BY JNDC FPND W.G.                        
                                                                  
     *****   MODIFIED PARTS FOR JENDL-3.2   ********************  
      (2,151)       RESOLVED RESONANCE PARAMETERS                 
      (3,2), (3,3), (3,4), (3,51-62), (3,64-71), (3,73-79)        
                    CURVES OF INELASTIC SCATTERING CROSS SECTIONS 
                    WERE SMOOTHED BY ADDING INTERPOLATED VALUES AT
                    SEVERAL ENERGY POINTS.                        
      (3,102)       ONLY Q-VALUE WAS MODIFIED.                    
     ***********************************************************  
                                                                  
                                                                  
MF=1  GENERAL INFORMATION                                         
  MT=451 COMMENTS AND DICTIONARY.                                 
                                                                  
MF=2  RESONANCE PARAMETERS                                        
  MT=151 RESOLVED AND UNRESOLVED RESONANCE PARAMETERS             
    THIS FILE WAS MADE OF AG-107 AND AG-109 DATA.                 
  RESOLVED RESONANCE PARAMETERS (BELOW 7.0095KEV)                 
       RESOLVED RESONANCE PARAMETERS (BELOW 7.0095 KEV) OF        
    JENDL-3.1 ARE THE SAME AS THOSE OF JENDL-2, WHICH WERE MADE BY
    NAKAJIMA /2/ ON THE BASIS OF EXPERIMENTAL DATA BY MOXON AND   
    RAE /3/, GARG ET AL./4/, ASGHAR ET AL./5/, PATTENDEN /6/,     
    MURADJAN AND ADAMCHUK /7/, DE BARROS ET AL./8/, PATTENDEN AND 
    JOLLY /9/, MACKLIN /10/ AND MIZUMOTO ET AL./11/. THERE ARE NO 
    NEW EXPERIMENTAL DATA AVAILABLE SINCE THE JENDL-2 EVALUATION. 
    TOTLA SPIN J AND ANGULAR MOMENTUM L OF SOME RESONANCES WERE   
    ESTIMATED WITH A RANDOM NUMBER METHOD AND A METHODOF BOLLINGER
    AND THOMAS/12/, RESPECTIVELY.                                 
      THE CAPTURE CROSS SECTION OF JENDL-3.1 BETWEEN 1.3 AND 2.6  
    KEV IS TOO LOW COMPARED WITH INTERPOLATED VALUES FROM THE     
    LOWER AND HIGHER ENERGY REGIONS.  TO COMPENSATE THE LOWER     
    CAPTURE CROSS SECTION, HYPOTHETICAL P-WAVE RESONANCES WERE    
    ADDED.  THE OTHER DATA ARE THE SAME AS JENDL-3.1, EXCEPT FOR  
    NEUTRON WIDTH WHICH WAS MODIFIED SO AS TO REPRODUCE THE       
    CAPTURE AREA MEASURED BY MACKLIN/10/.                         
  UNRESOLVED RESONANCE PARAMETERS (7.0095 - 100 KEV)              
    THE PARAMETERS WERE DETERMINED WITH THE CODE ASREP /13/ TO    
    REPRODUCE THE CAPTURE AND TOTAL CROSS SECTIONS, WHICH WERE    
    BASED ON EXPERIMENTAL DATA /14,15/ AND ADJUSTED FOR           
    CONSISTENCE BETWEEN THE DATA OF THE NATURAL ELEMENT AND ITS   
    ISOTOPES.                                                     
                                                                  
   CALCULATED 2200-M/S CROSS SECTIONS AND RES. INTEGRALS (BARNS): 
                     2200 M/S               RES. INTEG.           
      TOTAL          68.805                    -                  
      ELASTIC         5.180                    -                  
      CAPTURE        63.625                  762.9                
                                                                  
MF=3  NEUTRON CROSS SECTIONS                                      
                                                                  
 MT=1,102  TOTAL, CAPTURE                                         
  BELOW 100 KEV, RESONANCE PARAMETERS WERE GIVEN.  NO BACKGROUND  
  CROSS SECTIONS ARE ADOPTED.  ABOVE 100 KEV, CROSS SECTIONS WERE 
  EVALUATED ON THE BASIS OF EXPERIMENTAL DATA AND THEORETICAL     
  CALCULATIONS.  THE MAIN DATA WERE TAKEN FROM THE WORKS OF       
  POENITZ AND WHALEN /14/, FOSTER AND  GLASGOW /16/ FOR TOTAL     
  CROSS SECTOIN AND MIZUMOTO ET AL. /15/, POENITZ/17/ FOR CAPTURE 
  CROSS SECTION.  THE DATA WERE FITTED WITH SPLINE FUNCTION /18/, 
  AND WERE ADJUSTED FOR CONSISTENCE BETWEEN THE NATURAL ELEMENT   
  AND ITS ISOTOPES.                                               
 MT=2  ELASTIC                                                    
  ELASTIC = TOTAL - NONELASTIC                                    
 MT=3  NONELASTIC                                                 
  SUM OF MT=4,16,17,22,28,102,103,107                             
 MT=4  TOTAL INELASTIC                                            
  SUM OF MT=51-80,91                                              
 MT=16,17,22,28,51-80,91,103,107  (N,2N),(N,3N),(N,NA),(N,NP),    
 INELASTIC,(N,P),(N,A)                                            
  THEY WERE MADE OF AG-107 AND AG-109 DATA.  FOR THESE TWO        
  ISOTOPES, THE CROSS SECTIONS WERE CALCULATED WITH THE MULTISTEP 
  HAUSER-FESHBACH CODE TNG /19, 20/.  AT FIRST, THE OPTICAL MODEL 
  AND LEVEL DENSITY PARAMETERS WERE TAKEN FROM THE WORKS OF SMITH 
  ET AL. /21/ AND IIJIMA ET AL. /22/, RESPECTIVELY AND THEN THEY  
  WERE ADJUSTED TO REPRODUCE AVAILABLE EXPERIMENTAL DATA.         
                                                                  
      FOR JENDL-3.2, INELASTIC SCATTERING CROSS SECTIONS AT       
      THRESHOLD ENERGIES OF OTHER LEVELS WERE INSERTED BY         
      INTERPOLATING THE CALUCULATED VALUES WITH AKIMA'S METHOD.   
                                                                  
  THE OPTICAL MODEL PARAMETERS ARE:                               
                                                                  
               DEPTH (MEV)       RADIUS(FM)   DIFFUSENESS(FM)     
            -----------------   ------------  ---------------     
    NEUTRON V  = 48.25-0.3E      R0 = 1.249    A0 = 0.603         
            WS = 8.501-0.15E     RS = 1.270    AS = 0.575         
            VSO= 6.0             RSO= 1.249    ASO= 0.603         
    PROTON  V  = 66.061-0.550E   R0 = 1.150    A0 = 0.650         
            WS = 12.50-0.10E     RS = 1.250    AS = 0.470         
                                 RC = 1.150                       
    ALPHA   V  = 193.0-0.15E     R0 = 1.370    A0 = 0.560         
            WS = 21.00+0.25E     RS = 1.370    AS = 0.560         
                                 RC = 1.370                       
                                                                  
 THE LEVEL DENSITY PARAMETERS ARE:                                
                                                                  
         ECUT(MEV) EJO(MEV) T(MEV) A(1/MEV) C(MEV) CSPIN   EPAIR  
  RH-103   0.990    5.409   0.655    15.50  3.884  49.725  0.94   
  RH-104   0.230    4.351   0.650    15.43  17.72  49.820  0.00   
  RH-105   0.770    5.700   0.630    16.80  4.000  54.591  1.24   
  RH-106   0.150    3.869   0.575    17.50  17.18  57.230  0.00   
  PD-106   2.380    8.004   0.666    17.17  0.920  56.147  2.59   
  PD-107   0.700    7.693   0.769    14.98  6.956  49.293  1.35   
  PD-108   1.900    7.957   0.646    17.90  0.884  59.268  2.60   
  PD-109   0.360    7.380   0.687    17.50  9.479  58.301  1.35   
  AG-105   1.230    5.830   0.609    18.57  2.750  60.343  0.94   
  AG-106   0.400    3.549   0.563    17.16  12.92  56.110  0.00   
  AG-107   1.420    5.918   0.693    14.55  2.412  47.878  1.24   
  AG-108   0.270    3.014   0.576    15.04  6.004  49.799  0.00   
  AG-109   1.180    6.112   0.705    14.50  2.666  48.306  1.25   
  AG-110   0.320    3.150   0.454    17.01  2.513  57.015  0.00   
                                                                  
  THE LEVEL SCHEME IS GIVEN AS FOLLOWS:                           
                                                                  
   AG-107:                                                        
           NO.      ENERGY(MEV)    SPIN-PARITY                    
           GR.       0.0            1/2 -                         
            1        0.0930         7/2 +                         
            2        0.1260        (9/2)+                         
            3        0.3250         3/2 -                         
            4        0.4230         5/2 -                         
            5        0.7730       (11/2)+                         
            6        0.7870         3/2 -                         
            7        0.9220         5/2 +                         
            8        0.9500         5/2 -                         
            9        0.9730        (7/2)-                         
           10        0.9910       (13/2)+                         
           11        1.0610        (1/2 -)                        
           12        1.1420         1/2 +                         
           13        1.1470         7/2 -                         
           14        1.2230         5/2 +                         
           15        1.2590        (3/2)+                         
           16        1.3260        (3/2)+                         
   AG-109:                                                        
           NO.      ENERGY(MEV)    SPIN-PARITY                    
           GR.       0.0            1/2 -                         
            1        0.0880         7/2 +                         
            2        0.1330         9/2 +                         
            3        0.3110         3/2 -                         
            4        0.4150         5/2 -                         
            5        0.7020         3/2 -                         
            6        0.7070         3/2 +                         
            7        0.7240        (3/2)+                         
            8        0.7360         5/2 +                         
            9        0.8630         5/2 -                         
           10        0.8700        (5/2)+                         
           11        0.9110         7/2 +                         
           12        0.9120         7/2 -                         
           13        1.0910         9/2 -                         
           14        1.0990        (5/2 +)                        
 MT=251                                                           
  CALCULATED FROM MF=4,MT=2.                                      
                                                                  
MF=4  ANGULAR DISTRIBUTIONS OF SECONDARY NEUTRONS                 
 MT=2                                                             
  CALCULATED WITH THE CASTHY CODE /23/.                           
 MT=51-80                                                         
  CALCULATED WITH TNG.                                            
 MT=16,17,22,28,91                                                
  ASSUMED TO BE ISOTROPIC IN THE LABORATORY SYSTEM.               
                                                                  
MF=5  ENERGY DISTRIBUTIONS OF SECONDARY NEUTRONS                  
 MT=16,17,22,28,91                                                
  CALCULATED WITH TNG.                                            
                                                                  
MF=12,14,15  GAMMA-PRODUCTION DATA                                
 MT=4,16,17,22,28,102,103,107                                     
  CALCULATED WITH TNG.                                            
                                                                  
                                                                  
REFERENCES                                                        
 1) LIU, T. ET AL., JAERI-M 91-011 (1991).                        
 2) NAKAJIMA, Y., TO BE PUBLISHED.                                
 3) MOXON, M.C., RAE, E.R., "PROC. EANDC CONF. ON TIME-OF-FLIGHT  
    METHODS, SACLAY, 1961", 439.                                  
 4) GARG, J.B., ET AL., PHYS. REV., B137, 547(1965).              
 5) ASGHAR, M., ET AL., "PROC. INT. CONF. ON THE STUDY OF NUCLEAR 
    STRUCTURE WITH NEUTRONS, ANTWERP 1965", 65.                   
 6) PATTENDEN N.J.,IBID.,532.                                     
 7) MURADJAN, G.V., ADAMCHUK, JU. V., JADERNO-FIZICHESKIE         
    ISSLEDOVANIJA, 6, 64 (1968).                                  
 8) DE BARROS, S., ET AL., NUCL. PHYS., A131, 305(1969).          
 9) PATTENDEN, N.J., JOLLY, J.E., AERE-PR/NP-16(1969).            
10) MACKLIN, R.L., NUCL. SCI. ENG., 82, 400(1982).                
11) MIZUMOTO, M., ET AL., J. NUCL. SCI. TECHNOL., 20, 883(1983).  
12) BOLLINGER, L.M. AND THOMAS, G.E., PHYS. REV., 171,1293(1968). 
13) KIKUCHI Y., PRIVATE COMMUNICATION.                            
14) POENITZ, W.P., WHALEN, J.F., ANL-NDM-80(1983).                
15) MIZUMOTO, M., ET AL., "PROC. INTER. CONF. ON NUCL.DATA FOR    
    SCIENCE AND TECHNOLOGY", ANTWERP, P.226 (1982).               
16) FOSTER, JR., D.G., AND GLASGOW, D.W., PHYS. REV.,C3,          
    576 (1971).                                                   
17) POENITZ, W.P., ANL-83-4,239(1982).                            
18) NAKAGAWA, T., J. AT. ENE. SOC. JAPAN, 22, 559 (1980).         
19) FU, C.Y., ORNL/TM-7042(1980).                                 
20) SHIBATA, K., FU, C.Y., ORNL/TM-10093 (1986).                  
21) SMITH, A., ET AL, NUCL. PHYS., A415, 1 (1984).                
22) IIJIMA, S., ET AL, J. NUCL. SCI. TECHNOL., 21, 10 (1984).     
23) IGARASI, S. AND FUKAFORI, T., JAERTI 1321 (1991).