51TI 50TI(N,G) E=THERMAL: {~EGAF} 51TI c Evaluated Gamma-ray Activation File (EGAF). 51TI2c Evaluated by R.B. Firestone (LBNL), December 2003. 51TI c BR$|s{-0}=0.179 3 (1981MuZQ) 51TI cG RI$Elemental |s(|g) assuming %Abundance=5.18 2 51TI N 18.5 3 51TI PN C 51TI2PN Thermal cross section in barns. 51TI cN NR$Isotopic |s(|g)=NR*RI. 51TI2cN Divide by |s{-0} for intensity per neutron capture. 51TI L 0.0 3/2- 51TI L 1166.6 41/2- 51TI G 1166.6 4 0.0039 51TI L 1567.5 3 (5/2)- 51TI G 1567.5 4 0.0005 51TI L 2198.9 83/2- 51TI G 630.7 5 0.0005 51TI G 1031.3 5 0.0003 51TI G 2198.9 100.0016 51TI L 2905.1 81/2- 51TI G 707.8 5 0.0006 51TI G 1738.9 5 0.0009 51TI G 2904.2 100.0005 51TI L 3174.9 83/2- 51TI G 975.7 5 0.0001 51TI G 2007.0 108.0E-05 51TI G 3174.5 100.0008 51TI L 6372.6 61/2+ 51TI G 3197.3 100.0009 51TI G 3466.6 100.0027 51TI G 4173.6 100.0020 51TI G 5205.8 100.0033 51TI G 6373.1 100.0004 51TI 50TI(N,G) E=THERMAL:^BUDAPEST 51TI c Budapest Reactor data measured with thermal beam. 51TI cG RI$Elemental |s(|g) assuming %Abundance=5.18 2 51TI N 18.5 3 51TI PN C 51TI2PN Thermal cross section in barns. 51TI L 0.0 3/2- 51TI L 1166.6 41/2- 51TI G 1166.78 24 0.0158 19 51TI L 1567.5 3 (5/2)- 51TI L 2198.9 83/2- 51TI L 2905.1 81/2- 51TI L 3174.9 83/2- 51TI L 6372.6 61/2+ 51TI 50TI(N,G) E=THERMAL: ^L^A^N^L 1971AR39,1971TE01,1997ZH09 51TI c Only about 0.15% of the captures of thermal neutrons by 51TIAc natural titanium is by 50Ti. The only good data set for this reaction 51TIBc is Arnell et al. (1971) [1971Ar39]. This is the data set adopted by 51TICc the evaluation of Zhou (1997) [1997Zh09]. Other data for this reaction 51TIDc are very incomplete or with large errors, but are generally consistent 51TIEc with the adopted data. 51TI c The adopted gamma-ray energies are based on those from the 51TIAc levels in Zhou (1997). The data of Arnell et al. (1971) are only for 51TIBc transitions from the capture state or to the ground state, and their 51TICc intensities for these transitions were adopted unchanged. Intensities 51TIDc for gamma rays from the decay of the intermediate levels given in 51TIEc Arnell et al. (1971) were calculated using the branching ratios of 51TIFc Zhou (1997) and averaged using both the intensity of the gamma ray 51TIGc from the capture state and the intensity of the gamma ray decaying to 51TIHc the ground state. 51TI c The energies are good to about 0.5-1.0 keV. The intensities 51TIAc in Arnell et al. (1971) had no uncertainties but look fairly good. The 51TIBc data set is fairly complete based on the total decay energy and sums 51TICc from the capture state or into the ground state. A very crude estimate 51TIDc of the uncertainties of most intensities is of the order of 10%. 51TI N 1.0 51TI PN C 51TI2PN Per 100 neutron captures. 51TI L 0.0 3/2- 51TI L 1166.70 1/2- 51TI G 1166.69 41.700 51TI L 1437.30 7/2- 51TI L 1567.50 5/2- 51TI G 1567.47 5.600 51TI L 2144.00 5/2- 51TI L 2198.10 3/2- 51TI G 630.60 5.600 51TI G 1031.39 4.000 51TI G 2198.05 17.300 51TI L 2344.60 11/2- 51TI L 2691.40 7/2- 51TI L 2731.20 (7/2-) 51TI L 2754.20 15/2- 51TI L 2905.80 1/2- 51TI G 707.69 7.100 51TI G 1739.07 11.800 51TI G 2905.71 5.300 51TI L 2929.30 (5/2-) 51TI L 3062.30 (7/2-) 51TI L 3173.80 3/2- 51TI G 975.69 1.140 51TI G 2007.06 0.800 51TI G 3173.69 8.300 51TI L 3237.40 (7/2) 51TI L 3618.50 51TI L 3771.30 9/2+ 51TI L 6372.30 1/2+ 51TI G 3198.39 9.900 51TI G 3466.37 29.000 51TI G 4174.02 21.500 51TI G 5205.31 35.400 51TI G 6371.87 4.200