LLNL Evaluation, September 2005 1 0 0 0 2.605500+4 5.493830+1 -1 0 0 02628 1451 1 0.000000+0 0.000000+0 0 0 0 62628 1451 2 2.014102+0 2.000000+7 0 0 10020 62628 1451 3 0.000000+0 0.000000+0 0 0 62 32628 1451 4 26-Fe- 55 LLNL EVAL-Aug05 R. D. Hoffman, K. Kelley, et al. 2628 1451 5 DIST- REV- 2628 1451 6 LLNL Evaluation, September 2005 2628 1451 7 2628 1451 8 R. D. Hoffman, K. Kelley, F. S. Dietrich, R. Bauer, M. Mustafa, 2628 1451 9 D. Brown 2628 1451 10 2628 1451 11 ******************************************************************2628 1451 12 2628 1451 13 MF=3: CROSS SECTIONS FOR TARGET 55-FE (GS) 2628 1451 14 2628 1451 15 Cross sections to the ground state and any isomeric states in the 2628 1451 16 residual have been included for the following reactions: 2628 1451 17 2628 1451 18 (n,g) 2628 1451 19 (n,n') 2628 1451 20 (n,2n) 2628 1451 21 (n,np)+(n,pn) 2628 1451 22 (n,a) 2628 1451 23 (n,d) 2628 1451 24 (p,n) 2628 1451 25 (p,2n) 2628 1451 26 (d,n) 2628 1451 27 (d,2n) 2628 1451 28 2628 1451 29 Cross sections were calculated for incident energies from 5 keV 2628 1451 30 to 20 MeV, using the STAPRE code with a exiton model for 2628 1451 31 pre-equilibrium emission. Direct reaction contributions are not 2628 1451 32 included. 2628 1451 33 2628 1451 34 Exit particles considered are neutrons, protons, alpha particles, 2628 1451 35 and deuterons. Transmission coefficients for neutrons and protons 2628 1451 36 were obtained from the optical potential of Koning and Delaroche 2628 1451 37 using the ECIS code. The transmission coefficients for alpha 2628 1451 38 particles were obtained from the optical potential of McFadden 2628 1451 39 and Satchler. Those for deuterons are from the optical potential 2628 1451 40 of Perey and Perey. Alpha and deuteron transmission coefficients 2628 1451 41 were calculated using the SCAT2 routine. A simple Lorentzian is 2628 1451 42 assumed for the E1 photon strength function, and is normalized to 2628 1451 43 measured or systematic values of the average total s-wave 2628 1451 44 radiation width at the neutron binding energy. 2628 1451 45 2628 1451 46 Backshifted Fermi gas level density parameters are derived from 2628 1451 47 measured s-wave resonance spacings where available. For other 2628 1451 48 nuclei, systematic values are adopted. At low energies a constant 2628 1451 49 temperature form is adopted, and the two formulae are matched at 2628 1451 50 an energy between the backshift and the neutron binding energy so 2628 1451 51 as to give the best possible fit to known spectroscopic levels. 2628 1451 52 2628 1451 53 Discrete levels are taken from the Reference Input Parameter 2628 1451 54 Library (RIPL) with additional evaluations performed by R. Bauer. 2628 1451 55 2628 1451 56 Further details regarding this modeling effort can be found in R. 2628 1451 57 D. Hoffman, F. S. Dietrich, R. Bauer, K. Kelley, & M. Mustafa, 2628 1451 58 "Neutron and Charged- Particle Induced Cross Sections for 2628 1451 59 Radiochemistry for Isotopes of Scandium, Titanium, Vanadium, 2628 1451 60 Chromium, Manganese, and Iron", 2005, LLNL, UCRL-TR-211668, 2628 1451 61 available online at http://www.osti.gov/bridge 2628 1451 62 2628 1451 63 ******************************************************************2628 1451 64 2628 1451 65 *************************** DICTIONARY ***************************2628 1451 66 1 451 69 02628 1451 67 3 4 110 02628 1451 68 3 16 48 02628 1451 69 0.000000+0 0.000000+0 0 0 0 02628 1 099999 0.000000+0 0.000000+0 0 0 0 02628 0 0 0 2.605500+4 5.493830+1 0 0 0 02628 3 4 1 3.622580+6 3.622580+6 0 0 1 3212628 3 4 2 321 2 2628 3 4 3 1.000000+1 1.000000-8 1.120000+1 1.000000-8 1.260000+1 1.000000-82628 3 4 4 1.410000+1 1.000000-8 1.590000+1 1.000000-8 1.780000+1 1.000000-82628 3 4 5 2.000000+1 1.000000-8 2.240000+1 1.000000-8 2.520000+1 1.000000-82628 3 4 6 2.830000+1 1.000000-8 3.170000+1 1.000000-8 3.560000+1 1.000000-82628 3 4 7 4.000000+1 1.000000-8 4.490000+1 1.000000-8 5.040000+1 1.000000-82628 3 4 8 5.660000+1 1.000000-8 6.350000+1 1.000000-8 7.130000+1 1.000000-82628 3 4 9 8.000000+1 1.000000-8 8.940000+1 1.000000-8 1.000000+2 1.000000-82628 3 4 10 1.120000+2 1.000000-8 1.260000+2 1.000000-8 1.410000+2 1.000000-82628 3 4 11 1.590000+2 1.000000-8 1.780000+2 1.000000-8 2.000000+2 1.000000-82628 3 4 12 2.240000+2 1.000000-8 2.520000+2 1.000000-8 2.830000+2 1.000000-82628 3 4 13 3.170000+2 1.000000-8 3.560000+2 1.000000-8 4.000000+2 1.000000-82628 3 4 14 4.490000+2 1.000000-8 5.040000+2 1.000000-8 5.660000+2 1.000000-82628 3 4 15 6.350000+2 1.000000-8 7.130000+2 1.000000-8 8.000000+2 1.000000-82628 3 4 16 8.940000+2 1.000000-8 1.000000+3 1.000000-8 1.120000+3 1.000000-82628 3 4 17 1.260000+3 1.000000-8 1.410000+3 1.000000-8 1.590000+3 1.000000-82628 3 4 18 1.780000+3 1.000000-8 2.000000+3 1.000000-8 2.240000+3 1.000000-82628 3 4 19 2.520000+3 1.000000-8 2.830000+3 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