Li-8 activation 532 0 0 0 3.00800+ 3 7.93128+ 0 0 0 0 17038 1451 1 0.00000+ 0 1.00000+ 0 0 0 0 07038 1451 2 0.00000+ 0 0.00000+ 0 0 0 21 27038 1451 3 3-li- 8 inel eval-apr78 reich 7038 1451 4 dist-mar80 800317 7038 1451 5 mf=8, mt=457 radioactive decay data 7038 1451 6 references q(beta)- a.h. wapstra and k. bos, at. data and nucl. 7038 1451 7 data tables 19, 177 (1977). 7038 1451 8 other- see f. ajzenberg-selove and t. lauritsen, 7038 1451 9 nucl. phys. a227, 79-108 (1974). 7038 1451 10 note the beta decay proceeds almost entirely to the first 7038 1451 11 excited state (at 2.94 mev) in be-8. this state has 7038 1451 12 a large width (approx. 1.56 mev) and dissociates into7038 1451 13 two alpha particles. the beta transition thus has a 7038 1451 14 broad distribution of end-point energies. we have not7038 1451 15 included this the listed beta energy is that to the 7038 1451 16 center of the final state. the energy distribution of7038 1451 17 the beta-delayed alpha particles is also quite broad.7038 1451 18 we have computed the listed distribution using the 7038 1451 19 expression given by griffey and biedenharn (nucl. 7038 1451 20 phys. 15, 636 (1960)). the units of this intensity 7038 1451 21 distribution are alphas per kev per 100 decays and 7038 1451 22 the normalization is to 2 alphas per decay. 7038 1451 23 translated into endf/b-v format by mann and schenter (hedl) 7/797038 1451 24 1 451 26 17038 1451 25 8 457 23 17038 1451 26 0.00000+ 0 0.00000+ 0 0 0 0 07038 1 0 27 0.00000+ 0 0.00000+ 0 0 0 0 07038 0 0 28 3.00800+ 3 7.93128+ 0 0 0 0 27038 8457 29 8.42000- 1 6.00000- 3 0 0 6 07038 8457 30 6.29300+ 6 1.50000+ 4 0.00000+ 0 0.00000+ 0 3.97500+ 6 0.00000+ 07038 8457 31 2.00000+ 0 1.00000+ 0 0 0 6 17038 8457 32 1.00000+ 0 0.00000+ 0 1.60051+ 7 9.00000+ 2 1.00000+ 0 0.00000+ 07038 8457 33 0.00000+ 0 1.00000+ 0 0 0 6 17038 8457 34 1.00000- 2 0.00000+ 0 6.29300+ 6 1.50000+ 4 0.00000+ 0 0.00000+ 07038 8457 35 1.30650+ 7 3.00000+ 4 0 0 6 07038 8457 36 1.00000+ 0 1.00000+ 0 1.00000+ 2 0.00000+ 0 0.00000+ 0 0.00000+ 07038 8457 37 0.00000+ 0 4.00000+ 0 1 0 6 07038 8457 38 0.00000+ 0 0.00000+ 0 3.97500+ 6 0.00000+ 0 1.99768+ 0 0.00000+ 07038 8457 39 1.00000+ 0 0.00000+ 0 0 0 1 307038 8457 40 30 2 7038 8457 41 5.00000+ 5 0.00000+ 0 7.50000+ 5 1.79207- 8 8.75000+ 5 4.64537- 87038 8457 42 1.00000+ 6 7.56875- 8 1.12500+ 6 1.74201- 7 1.25000+ 6 4.23489- 77038 8457 43 1.37500+ 6 7.36852- 7 1.50000+ 6 9.43090- 7 1.60000+ 6 9.56105- 77038 8457 44 1.70000+ 6 8.60995- 7 1.80000+ 6 7.31846- 7 1.90000+ 6 6.05700- 77038 8457 45 2.00000+ 6 5.06585- 7 2.10000+ 6 4.26493- 7 2.20000+ 6 3.66423- 77038 8457 46 2.30000+ 6 3.17367- 7 2.40000+ 6 2.77320- 7 2.50000+ 6 2.42280- 77038 8457 47 2.75000+ 6 1.75202- 7 3.00000+ 6 1.30150- 7 3.25000+ 6 9.75127- 87038 8457 48 3.50000+ 6 7.28842- 8 3.75000+ 6 5.30613- 8 4.00000+ 6 3.83443- 87038 8457 49 4.25000+ 6 2.71313- 8 4.50000+ 6 1.88217- 8 4.75000+ 6 1.27147- 87038 8457 50 5.00000+ 6 8.30960- 9 5.50000+ 6 3.20370- 9 6.00000+ 6 0.00000+ 07038 8457 51 0.00000+ 0 0.00000+ 0 0 0 0 07038 8 0 52 0.00000+ 0 0.00000+ 0 0 0 0 07038 0 0 53 0.00000+ 0 0.00000+ 0 0 0 0 0 0 0 0 54 0.00000+ 0 0.00000+ 0 0 0 0 0 -1 0 0 54