LLNL Evaluation, September 2005                                      1 0  0    0
 2.505000+4 4.995424+1         -1          0          0          02511 1451    1
 2.290000+5 0.000000+0          3          1          0          62511 1451    2
 9.986200-1 2.000000+7          0          0      10010          62511 1451    3
 0.000000+0 0.000000+0          0          0         61          22511 1451    4
 25-Mn- 50 LLNL       EVAL-Apr05 R. D. Hoffman, K. Kelley, et al. 2511 1451    5
           DIST-      REV-                                        2511 1451    6
LLNL Evaluation, September 2005                                   2511 1451    7
                                                                  2511 1451    8
R. D. Hoffman, K. Kelley, F. S. Dietrich, R. Bauer, M. Mustafa,   2511 1451    9
D. Brown                                                          2511 1451   10
                                                                  2511 1451   11
******************************************************************2511 1451   12
                                                                  2511 1451   13
MF=3: CROSS SECTIONS FOR TARGET 50-MN (M1)                        2511 1451   14
                                                                  2511 1451   15
Cross sections to the ground state and any isomeric states in the 2511 1451   16
residual have been included for the following reactions:          2511 1451   17
                                                                  2511 1451   18
  (n,g)                                                           2511 1451   19
  (n,n')                                                          2511 1451   20
  (n,2n)                                                          2511 1451   21
  (n,np)+(n,pn)                                                   2511 1451   22
  (n,a)                                                           2511 1451   23
  (n,d)                                                           2511 1451   24
  (p,n)                                                           2511 1451   25
  (d,n)                                                           2511 1451   26
  (d,2n)                                                          2511 1451   27
                                                                  2511 1451   28
Cross sections were calculated for incident energies from 5 keV   2511 1451   29
to 20 MeV, using the STAPRE code with a exiton model for          2511 1451   30
pre-equilibrium emission. Direct reaction contributions are not   2511 1451   31
included.                                                         2511 1451   32
                                                                  2511 1451   33
Exit particles considered are neutrons, protons, alpha particles, 2511 1451   34
and deuterons. Transmission coefficients for neutrons and protons 2511 1451   35
were obtained from the optical potential of Koning and Delaroche  2511 1451   36
using the ECIS code. The transmission coefficients for alpha      2511 1451   37
particles were obtained from the optical potential of McFadden    2511 1451   38
and Satchler. Those for deuterons are from the optical potential  2511 1451   39
of Perey and Perey. Alpha and deuteron transmission coefficients  2511 1451   40
were calculated using the SCAT2 routine. A simple Lorentzian is   2511 1451   41
assumed for the E1 photon strength function, and is normalized to 2511 1451   42
measured or systematic values of the average total s-wave         2511 1451   43
radiation width at the neutron binding energy.                    2511 1451   44
                                                                  2511 1451   45
Backshifted Fermi gas level density parameters are derived from   2511 1451   46
measured s-wave resonance spacings where available. For other     2511 1451   47
nuclei, systematic values are adopted. At low energies a constant 2511 1451   48
temperature form is adopted, and the two formulae are matched at  2511 1451   49
an energy between the backshift and the neutron binding energy so 2511 1451   50
as to give the best possible fit to known spectroscopic levels.   2511 1451   51
                                                                  2511 1451   52
Discrete levels are taken from the Reference Input Parameter      2511 1451   53
Library (RIPL) with additional evaluations performed by R. Bauer. 2511 1451   54
                                                                  2511 1451   55
Further details regarding this modeling effort can be found in R. 2511 1451   56
D. Hoffman, F. S. Dietrich, R. Bauer, K. Kelley, & M. Mustafa,    2511 1451   57
"Neutron and Charged- Particle Induced Cross Sections for         2511 1451   58
Radiochemistry for Isotopes of Scandium, Titanium, Vanadium,      2511 1451   59
Chromium, Manganese, and Iron", 2005, LLNL, UCRL-TR-211668,       2511 1451   60
available online at http://www.osti.gov/bridge                    2511 1451   61
                                                                  2511 1451   62
******************************************************************2511 1451   63
                                                                  2511 1451   64
*************************** DICTIONARY ***************************2511 1451   65
                                1        451         67          02511 1451   66
                                3          4         41          02511 1451   67
 0.000000+0 0.000000+0          0          0          0          02511 1  099999
 0.000000+0 0.000000+0          0          0          0          02511 0  0    0
 2.505000+4 4.995424+1          0          0          0          02511 3  4    1
-8.748740+6-8.748740+6          0          0          1        1122511 3  4    2
        112          2                                            2511 3  4    3
 8.925246+6 6.54605-12 9.000000+6 5.973600-7 9.100000+6 1.703400-62511 3  4    4
 9.200000+6 3.479600-6 9.300000+6 6.014200-6 9.400000+6 9.395500-62511 3  4    5
 9.500000+6 1.371200-5 9.600000+6 3.647600-5 9.700000+6 1.061400-42511 3  4    6
 9.800000+6 1.789900-4 9.900000+6 2.632400-4 1.000000+7 3.575500-42511 3  4    7
 1.010000+7 4.643200-4 1.020000+7 5.828800-4 1.030000+7 7.153600-42511 3  4    8
 1.040000+7 8.603000-4 1.050000+7 1.019600-3 1.060000+7 1.189800-32511 3  4    9
 1.070000+7 1.371900-3 1.080000+7 1.565600-3 1.090000+7 1.772200-32511 3  4   10
 1.100000+7 1.989500-3 1.110000+7 2.218100-3 1.120000+7 2.457100-32511 3  4   11
 1.130000+7 2.706900-3 1.140000+7 2.966700-3 1.150000+7 3.237000-32511 3  4   12
 1.160000+7 3.517200-3 1.170000+7 3.807500-3 1.180000+7 4.107700-32511 3  4   13
 1.190000+7 4.418200-3 1.200000+7 4.738400-3 1.210000+7 5.068800-32511 3  4   14
 1.220000+7 5.408900-3 1.230000+7 5.759000-3 1.240000+7 6.118800-32511 3  4   15
 1.250000+7 6.488500-3 1.260000+7 6.867900-3 1.270000+7 7.257000-32511 3  4   16
 1.280000+7 7.655900-3 1.290000+7 8.064700-3 1.300000+7 8.483300-32511 3  4   17
 1.310000+7 8.911600-3 1.320000+7 9.349600-3 1.330000+7 9.797400-32511 3  4   18
 1.340000+7 1.025500-2 1.350000+7 1.072100-2 1.360000+7 1.119800-22511 3  4   19
 1.370000+7 1.168300-2 1.380000+7 1.217900-2 1.390000+7 1.268300-22511 3  4   20
 1.400000+7 1.319800-2 1.410000+7 1.372100-2 1.420000+7 1.425500-22511 3  4   21
 1.430000+7 1.479800-2 1.440000+7 1.535000-2 1.450000+7 1.590400-22511 3  4   22
 1.460000+7 1.645900-2 1.470000+7 1.700300-2 1.480000+7 1.753700-22511 3  4   23
 1.490000+7 1.805200-2 1.500000+7 1.854900-2 1.510000+7 1.902200-22511 3  4   24
 1.520000+7 1.947300-2 1.530000+7 1.989900-2 1.540000+7 2.030000-22511 3  4   25
 1.550000+7 2.067100-2 1.560000+7 2.101600-2 1.570000+7 2.133200-22511 3  4   26
 1.580000+7 2.162100-2 1.590000+7 2.188100-2 1.600000+7 2.211500-22511 3  4   27
 1.610000+7 2.232100-2 1.620000+7 2.250500-2 1.630000+7 2.266500-22511 3  4   28
 1.640000+7 2.280400-2 1.650000+7 2.292400-2 1.660000+7 2.302700-22511 3  4   29
 1.670000+7 2.311400-2 1.680000+7 2.318800-2 1.690000+7 2.324900-22511 3  4   30
 1.700000+7 2.330000-2 1.710000+7 2.334000-2 1.720000+7 2.337300-22511 3  4   31
 1.730000+7 2.339700-2 1.740000+7 2.341500-2 1.750000+7 2.342700-22511 3  4   32
 1.760000+7 2.343300-2 1.770000+7 2.343600-2 1.780000+7 2.343400-22511 3  4   33
 1.790000+7 2.342900-2 1.800000+7 2.342100-2 1.810000+7 2.340800-22511 3  4   34
 1.820000+7 2.339400-2 1.830000+7 2.337600-2 1.840000+7 2.335600-22511 3  4   35
 1.850000+7 2.333400-2 1.860000+7 2.330900-2 1.870000+7 2.328100-22511 3  4   36
 1.880000+7 2.325200-2 1.890000+7 2.321900-2 1.900000+7 2.318500-22511 3  4   37
 1.910000+7 2.314900-2 1.920000+7 2.311000-2 1.930000+7 2.306800-22511 3  4   38
 1.940000+7 2.302300-2 1.950000+7 2.297700-2 1.960000+7 2.292800-22511 3  4   39
 1.970000+7 2.287700-2 1.980000+7 2.282400-2 1.990000+7 2.276800-22511 3  4   40
 2.000000+7 2.276800-2                                            2511 3  4   41
 0.000000+0 0.000000+0          0          0          0          02511 3  099999
 0.000000+0 0.000000+0          0          0          0          02511 0  0    0
 0.000000+0 0.000000+0          0          0          0          0   0 0  0    0
 0.000000+0 0.000000+0          0          0          0          0  -1 0  0    0