LLNL Evaluation, September 2005 1 0 0 0 2.105000+4 4.995219+1 -1 0 0 02140 1451 1 0.000000+0 0.000000+0 0 0 0 62140 1451 2 2.014102+0 2.000000+7 0 0 10020 62140 1451 3 0.000000+0 0.000000+0 0 0 63 32140 1451 4 21-Sc- 50 LLNL EVAL-Aug05 R. D. Hoffman, K. Kelley, et al. 2140 1451 5 DIST- REV- 2140 1451 6 LLNL Evaluation, September 2005 2140 1451 7 2140 1451 8 R. D. Hoffman, K. Kelley, F. S. Dietrich, R. Bauer, M. Mustafa, 2140 1451 9 D. Brown 2140 1451 10 2140 1451 11 ******************************************************************2140 1451 12 2140 1451 13 MF=3: CROSS SECTIONS FOR TARGET 50-SC (GS) 2140 1451 14 2140 1451 15 Cross sections to the ground state and any isomeric states in the 2140 1451 16 residual have been included for the following reactions: 2140 1451 17 2140 1451 18 (n,g) 2140 1451 19 (n,n') 2140 1451 20 (n,2n) 2140 1451 21 (n,3n) 2140 1451 22 (n,np)+(n,pn) 2140 1451 23 (n,a) 2140 1451 24 (n,d) 2140 1451 25 (p,n) 2140 1451 26 (p,2n) 2140 1451 27 (d,n) 2140 1451 28 (d,2n) 2140 1451 29 2140 1451 30 Cross sections were calculated for incident energies from 5 keV 2140 1451 31 to 20 MeV, using the STAPRE code with a exiton model for 2140 1451 32 pre-equilibrium emission. Direct reaction contributions are not 2140 1451 33 included. 2140 1451 34 2140 1451 35 Exit particles considered are neutrons, protons, alpha particles, 2140 1451 36 and deuterons. Transmission coefficients for neutrons and protons 2140 1451 37 were obtained from the optical potential of Koning and Delaroche 2140 1451 38 using the ECIS code. The transmission coefficients for alpha 2140 1451 39 particles were obtained from the optical potential of McFadden 2140 1451 40 and Satchler. Those for deuterons are from the optical potential 2140 1451 41 of Perey and Perey. Alpha and deuteron transmission coefficients 2140 1451 42 were calculated using the SCAT2 routine. A simple Lorentzian is 2140 1451 43 assumed for the E1 photon strength function, and is normalized to 2140 1451 44 measured or systematic values of the average total s-wave 2140 1451 45 radiation width at the neutron binding energy. 2140 1451 46 2140 1451 47 Backshifted Fermi gas level density parameters are derived from 2140 1451 48 measured s-wave resonance spacings where available. For other 2140 1451 49 nuclei, systematic values are adopted. At low energies a constant 2140 1451 50 temperature form is adopted, and the two formulae are matched at 2140 1451 51 an energy between the backshift and the neutron binding energy so 2140 1451 52 as to give the best possible fit to known spectroscopic levels. 2140 1451 53 2140 1451 54 Discrete levels are taken from the Reference Input Parameter 2140 1451 55 Library (RIPL) with additional evaluations performed by R. Bauer. 2140 1451 56 2140 1451 57 Further details regarding this modeling effort can be found in R. 2140 1451 58 D. Hoffman, F. S. Dietrich, R. Bauer, K. Kelley, & M. Mustafa, 2140 1451 59 "Neutron and Charged- Particle Induced Cross Sections for 2140 1451 60 Radiochemistry for Isotopes of Scandium, Titanium, Vanadium, 2140 1451 61 Chromium, Manganese, and Iron", 2005, LLNL, UCRL-TR-211668, 2140 1451 62 available online at http://www.osti.gov/bridge 2140 1451 63 2140 1451 64 ******************************************************************2140 1451 65 2140 1451 66 *************************** DICTIONARY ***************************2140 1451 67 1 451 70 02140 1451 68 3 4 110 02140 1451 69 3 16 110 02140 1451 70 0.000000+0 0.000000+0 0 0 0 02140 1 099999 0.000000+0 0.000000+0 0 0 0 02140 0 0 0 2.105000+4 4.995219+1 0 0 0 02140 3 4 1 1.025850+7 1.025850+7 0 0 1 3212140 3 4 2 321 2 2140 3 4 3 1.000000+1 1.000000-8 1.120000+1 1.000000-8 1.260000+1 1.000000-82140 3 4 4 1.410000+1 1.000000-8 1.590000+1 1.000000-8 1.780000+1 1.000000-82140 3 4 5 2.000000+1 1.000000-8 2.240000+1 1.000000-8 2.520000+1 1.000000-82140 3 4 6 2.830000+1 1.000000-8 3.170000+1 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