LLNL Evaluation, September 2005 1 0 0 0 2.104400+4 4.395940+1 -1 0 0 02122 1451 1 0.000000+0 0.000000+0 0 0 0 62122 1451 2 2.014102+0 2.000000+7 0 0 10020 62122 1451 3 0.000000+0 0.000000+0 0 0 62 32122 1451 4 21-Sc- 44 LLNL EVAL-Aug05 R. D. Hoffman, K. Kelley, et al. 2122 1451 5 DIST- REV- 2122 1451 6 LLNL Evaluation, September 2005 2122 1451 7 2122 1451 8 R. D. Hoffman, K. Kelley, F. S. Dietrich, R. Bauer, M. Mustafa, 2122 1451 9 D. Brown 2122 1451 10 2122 1451 11 ******************************************************************2122 1451 12 2122 1451 13 MF=3: CROSS SECTIONS FOR TARGET 44-SC (GS) 2122 1451 14 2122 1451 15 Cross sections to the ground state and any isomeric states in the 2122 1451 16 residual have been included for the following reactions: 2122 1451 17 2122 1451 18 (n,g) 2122 1451 19 (n,n') 2122 1451 20 (n,2n) 2122 1451 21 (n,np)+(n,pn) 2122 1451 22 (n,a) 2122 1451 23 (n,d) 2122 1451 24 (p,n) 2122 1451 25 (p,2n) 2122 1451 26 (d,n) 2122 1451 27 (d,2n) 2122 1451 28 2122 1451 29 Cross sections were calculated for incident energies from 5 keV 2122 1451 30 to 20 MeV, using the STAPRE code with a exiton model for 2122 1451 31 pre-equilibrium emission. Direct reaction contributions are not 2122 1451 32 included. 2122 1451 33 2122 1451 34 Exit particles considered are neutrons, protons, alpha particles, 2122 1451 35 and deuterons. Transmission coefficients for neutrons and protons 2122 1451 36 were obtained from the optical potential of Koning and Delaroche 2122 1451 37 using the ECIS code. The transmission coefficients for alpha 2122 1451 38 particles were obtained from the optical potential of McFadden 2122 1451 39 and Satchler. Those for deuterons are from the optical potential 2122 1451 40 of Perey and Perey. Alpha and deuteron transmission coefficients 2122 1451 41 were calculated using the SCAT2 routine. A simple Lorentzian is 2122 1451 42 assumed for the E1 photon strength function, and is normalized to 2122 1451 43 measured or systematic values of the average total s-wave 2122 1451 44 radiation width at the neutron binding energy. 2122 1451 45 2122 1451 46 Backshifted Fermi gas level density parameters are derived from 2122 1451 47 measured s-wave resonance spacings where available. For other 2122 1451 48 nuclei, systematic values are adopted. At low energies a constant 2122 1451 49 temperature form is adopted, and the two formulae are matched at 2122 1451 50 an energy between the backshift and the neutron binding energy so 2122 1451 51 as to give the best possible fit to known spectroscopic levels. 2122 1451 52 2122 1451 53 Discrete levels are taken from the Reference Input Parameter 2122 1451 54 Library (RIPL) with additional evaluations performed by R. Bauer. 2122 1451 55 2122 1451 56 Further details regarding this modeling effort can be found in R. 2122 1451 57 D. Hoffman, F. S. Dietrich, R. Bauer, K. Kelley, & M. Mustafa, 2122 1451 58 "Neutron and Charged- Particle Induced Cross Sections for 2122 1451 59 Radiochemistry for Isotopes of Scandium, Titanium, Vanadium, 2122 1451 60 Chromium, Manganese, and Iron", 2005, LLNL, UCRL-TR-211668, 2122 1451 61 available online at http://www.osti.gov/bridge 2122 1451 62 2122 1451 63 ******************************************************************2122 1451 64 2122 1451 65 *************************** DICTIONARY ***************************2122 1451 66 1 451 69 02122 1451 67 3 4 110 02122 1451 68 3 16 59 02122 1451 69 0.000000+0 0.000000+0 0 0 0 02122 1 099999 0.000000+0 0.000000+0 0 0 0 02122 0 0 0 2.104400+4 4.395940+1 0 0 0 02122 3 4 1 6.257780+6 6.257780+6 0 0 1 3212122 3 4 2 321 2 2122 3 4 3 1.000000+1 1.000000-8 1.120000+1 1.000000-8 1.260000+1 1.000000-82122 3 4 4 1.410000+1 1.000000-8 1.590000+1 1.000000-8 1.780000+1 1.000000-82122 3 4 5 2.000000+1 1.000000-8 2.240000+1 1.000000-8 2.520000+1 1.000000-82122 3 4 6 2.830000+1 1.000000-8 3.170000+1 1.000000-8 3.560000+1 1.000000-82122 3 4 7 4.000000+1 1.000000-8 4.490000+1 1.000000-8 5.040000+1 1.000000-82122 3 4 8 5.660000+1 1.000000-8 6.350000+1 1.000000-8 7.130000+1 1.000000-82122 3 4 9 8.000000+1 1.000000-8 8.940000+1 1.000000-8 1.000000+2 1.000000-82122 3 4 10 1.120000+2 1.000000-8 1.260000+2 1.000000-8 1.410000+2 1.000000-82122 3 4 11 1.590000+2 1.000000-8 1.780000+2 1.000000-8 2.000000+2 1.000000-82122 3 4 12 2.240000+2 1.000000-8 2.520000+2 1.000000-8 2.830000+2 1.000000-82122 3 4 13 3.170000+2 1.000000-8 3.560000+2 1.000000-8 4.000000+2 1.000000-82122 3 4 14 4.490000+2 1.000000-8 5.040000+2 1.000000-8 5.660000+2 1.000000-82122 3 4 15 6.350000+2 1.000000-8 7.130000+2 1.000000-8 8.000000+2 1.000000-82122 3 4 16 8.940000+2 1.000000-8 1.000000+3 1.000000-8 1.120000+3 1.000000-82122 3 4 17 1.260000+3 1.000000-8 1.410000+3 1.000000-8 1.590000+3 1.000000-82122 3 4 18 1.780000+3 1.000000-8 2.000000+3 1.000000-8 2.240000+3 1.000000-82122 3 4 19 2.520000+3 1.000000-8 2.830000+3 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1.548830-7 9.150000+5 4.848130-72122 3 4 46 9.560000+5 2.220550-6 1.000000+6 4.485780-6 1.100000+6 8.885820-62122 3 4 47 1.200000+6 2.670470-5 1.300000+6 6.713960-5 1.400000+6 1.519980-42122 3 4 48 1.500000+6 3.117130-4 1.600000+6 5.933430-4 1.700000+6 1.059230-32122 3 4 49 1.800000+6 1.790290-3 1.900000+6 2.881120-3 2.000000+6 4.441170-32122 3 4 50 2.100000+6 6.592090-3 2.200000+6 9.459650-3 2.300000+6 1.316670-22122 3 4 51 2.400000+6 1.783680-2 2.500000+6 2.356470-2 2.600000+6 3.038990-22122 3 4 52 2.700000+6 3.836310-2 2.800000+6 4.749470-2 2.900000+6 5.778970-22122 3 4 53 3.000000+6 6.906990-2 3.100000+6 8.130010-2 3.200000+6 9.446640-22122 3 4 54 3.300000+6 1.082300-1 3.400000+6 1.226860-1 3.500000+6 1.372820-12122 3 4 55 3.600000+6 1.520590-1 3.700000+6 1.665050-1 3.800000+6 1.807980-12122 3 4 56 3.900000+6 1.944730-1 4.000000+6 2.074720-1 4.100000+6 2.197240-12122 3 4 57 4.200000+6 2.311230-1 4.300000+6 2.415920-1 4.400000+6 2.510840-12122 3 4 58 4.500000+6 2.595910-1 4.600000+6 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1.610500-1 8.600000+6 1.583510-12122 3 4 72 8.700000+6 1.557350-1 8.800000+6 1.532800-1 8.900000+6 1.510430-12122 3 4 73 9.000000+6 1.489290-1 9.100000+6 1.469350-1 9.200000+6 1.450620-12122 3 4 74 9.300000+6 1.432780-1 9.400000+6 1.416190-1 9.500000+6 1.399980-12122 3 4 75 9.600000+6 1.384210-1 9.700000+6 1.368870-1 9.800000+6 1.354040-12122 3 4 76 9.900000+6 1.340330-1 1.000000+7 1.326170-1 1.010000+7 1.313180-12122 3 4 77 1.020000+7 1.304230-1 1.030000+7 1.291090-1 1.040000+7 1.277480-12122 3 4 78 1.050000+7 1.264190-1 1.060000+7 1.251890-1 1.070000+7 1.239460-12122 3 4 79 1.080000+7 1.227270-1 1.090000+7 1.214950-1 1.100000+7 1.203190-12122 3 4 80 1.110000+7 1.191970-1 1.120000+7 1.181020-1 1.130000+7 1.170390-12122 3 4 81 1.140000+7 1.159760-1 1.150000+7 1.149320-1 1.160000+7 1.139470-12122 3 4 82 1.170000+7 1.129860-1 1.180000+7 1.120360-1 1.190000+7 1.110850-12122 3 4 83 1.200000+7 1.101910-1 1.210000+7 1.093010-1 1.220000+7 1.084500-12122 3 4 84 1.230000+7 1.076170-1 1.240000+7 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1.217790-1 1.830000+7 1.210000-12122 3 16 53 1.840000+7 1.200990-1 1.850000+7 1.191920-1 1.860000+7 1.183230-12122 3 16 54 1.870000+7 1.175220-1 1.880000+7 1.165790-1 1.890000+7 1.156610-12122 3 16 55 1.900000+7 1.148440-1 1.910000+7 1.138940-1 1.920000+7 1.130690-12122 3 16 56 1.930000+7 1.121080-1 1.940000+7 1.111440-1 1.950000+7 1.103010-12122 3 16 57 1.960000+7 1.093400-1 1.970000+7 1.084830-1 1.980000+7 1.075390-12122 3 16 58 1.990000+7 1.065630-1 2.000000+7 1.056750-1 2122 3 16 59 0.000000+0 0.000000+0 0 0 0 02122 3 099999 0.000000+0 0.000000+0 0 0 0 02122 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