LLNL Evaluation, September 2005 1 0 0 0 2.204800+4 4.794795+1 -1 0 0 02231 1451 1 0.000000+0 0.000000+0 0 0 0 62231 1451 2 2.014102+0 2.000000+7 0 0 10020 62231 1451 3 0.000000+0 0.000000+0 0 0 62 32231 1451 4 22-Ti- 48 LLNL EVAL-Aug05 R. D. Hoffman, K. Kelley, et al. 2231 1451 5 DIST- REV- 2231 1451 6 LLNL Evaluation, September 2005 2231 1451 7 2231 1451 8 R. D. Hoffman, K. Kelley, F. S. Dietrich, R. Bauer, M. Mustafa, 2231 1451 9 D. Brown 2231 1451 10 2231 1451 11 ******************************************************************2231 1451 12 2231 1451 13 MF=3: CROSS SECTIONS FOR TARGET 48-TI (GS) 2231 1451 14 2231 1451 15 Cross sections to the ground state and any isomeric states in the 2231 1451 16 residual have been included for the following reactions: 2231 1451 17 2231 1451 18 (n,g) 2231 1451 19 (n,n') 2231 1451 20 (n,2n) 2231 1451 21 (n,np)+(n,pn) 2231 1451 22 (n,a) 2231 1451 23 (n,d) 2231 1451 24 (p,n) 2231 1451 25 (p,2n) 2231 1451 26 (d,n) 2231 1451 27 (d,2n) 2231 1451 28 2231 1451 29 Cross sections were calculated for incident energies from 5 keV 2231 1451 30 to 20 MeV, using the STAPRE code with a exiton model for 2231 1451 31 pre-equilibrium emission. Direct reaction contributions are not 2231 1451 32 included. 2231 1451 33 2231 1451 34 Exit particles considered are neutrons, protons, alpha particles, 2231 1451 35 and deuterons. Transmission coefficients for neutrons and protons 2231 1451 36 were obtained from the optical potential of Koning and Delaroche 2231 1451 37 using the ECIS code. The transmission coefficients for alpha 2231 1451 38 particles were obtained from the optical potential of McFadden 2231 1451 39 and Satchler. Those for deuterons are from the optical potential 2231 1451 40 of Perey and Perey. Alpha and deuteron transmission coefficients 2231 1451 41 were calculated using the SCAT2 routine. A simple Lorentzian is 2231 1451 42 assumed for the E1 photon strength function, and is normalized to 2231 1451 43 measured or systematic values of the average total s-wave 2231 1451 44 radiation width at the neutron binding energy. 2231 1451 45 2231 1451 46 Backshifted Fermi gas level density parameters are derived from 2231 1451 47 measured s-wave resonance spacings where available. For other 2231 1451 48 nuclei, systematic values are adopted. At low energies a constant 2231 1451 49 temperature form is adopted, and the two formulae are matched at 2231 1451 50 an energy between the backshift and the neutron binding energy so 2231 1451 51 as to give the best possible fit to known spectroscopic levels. 2231 1451 52 2231 1451 53 Discrete levels are taken from the Reference Input Parameter 2231 1451 54 Library (RIPL) with additional evaluations performed by R. Bauer. 2231 1451 55 2231 1451 56 Further details regarding this modeling effort can be found in R. 2231 1451 57 D. Hoffman, F. S. Dietrich, R. Bauer, K. Kelley, & M. Mustafa, 2231 1451 58 "Neutron and Charged- Particle Induced Cross Sections for 2231 1451 59 Radiochemistry for Isotopes of Scandium, Titanium, Vanadium, 2231 1451 60 Chromium, Manganese, and Iron", 2005, LLNL, UCRL-TR-211668, 2231 1451 61 available online at http://www.osti.gov/bridge 2231 1451 62 2231 1451 63 ******************************************************************2231 1451 64 2231 1451 65 *************************** DICTIONARY ***************************2231 1451 66 1 451 69 02231 1451 67 3 4 110 02231 1451 68 3 16 46 02231 1451 69 0.000000+0 0.000000+0 0 0 0 02231 1 099999 0.000000+0 0.000000+0 0 0 0 02231 0 0 0 2.204800+4 4.794795+1 0 0 0 02231 3 4 1 4.534510+6 4.534510+6 0 0 1 3212231 3 4 2 321 2 2231 3 4 3 1.000000+1 1.000000-8 1.120000+1 1.000000-8 1.260000+1 1.000000-82231 3 4 4 1.410000+1 1.000000-8 1.590000+1 1.000000-8 1.780000+1 1.000000-82231 3 4 5 2.000000+1 1.000000-8 2.240000+1 1.000000-8 2.520000+1 1.000000-82231 3 4 6 2.830000+1 1.000000-8 3.170000+1 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