IAEA-NDS ENDF Download System, v-2008-07-22 0 0 0 0 3.008000+3 7.931275+0 -1 0 0 1 331 1451 1 0.000000+0 1.000000+0 0 0 0 6 331 1451 2 0.000000+0 0.000000+0 1 0 4 6 331 1451 3 0.000000+0 0.000000+0 0 0 25 2 331 1451 4 3-LI- 8 INEL EVAL-APR79 C.W.REICH 331 1451 5 DIST-SEP91 19910724 331 1451 6 ----ENDF/B-VI MATERIAL 331 331 1451 7 -----RADIOACTIVE DECAY DATA 331 1451 8 ------ENDF-6 FORMAT 331 1451 9 REVISIONS TO EBDF/B-V DATA: 03/26/90, CWR. THESE CHANGES INCLU 331 1451 10 THE HALF-LIFE, Q-BETA VALUE AND THE UNCERTAINTY IN E-BETA (DUE 331 1451 11 THE WIDTH OF THE ALPHA-EMITTING STATE). 331 1451 12 Q-BETA: A. H. WAPSTRA AND G. AUDI, NUCL. PHYS. A432, 1 (1985). 331 1451 13 OTHER: F. AJZENBERG-SELOVE, NUCL. PHYS. A490, 76, (1988). 331 1451 14 NOTE: THE LISTED VALUE WAS OBTAINED BY EXTRAPOLATION. 331 1451 15 NOTE: THE BETA DECAY PROCEEDS ALMOST ENTIRELY TO THE FIRST 331 1451 16 EXCITED STATE (AT 2.94 MEV) IN BE-8. THIS STATE HAS 331 1451 17 A LARGE WIDTH (APPROX. 1.56 MEV) AND DISSOCIATES INTO 331 1451 18 TWO ALPHA PARTICLES. THE BETA TRANSITION THUS HAS A 331 1451 19 BROAD DISTRIBUTION OF END-POINT ENERGIES. THE LISTED 331 1451 20 BETA ENERGY IS THAT TO THE CENTER OF THE FINAL STATE. 331 1451 21 THE ENERGY DISTRIBUTION OF THE BETA-DELAYED ALPHA 331 1451 22 PARTICLES IS ALSO QUITE BROAD. WE HAVE COMPUTED THE 331 1451 23 LISTED DISTRIBUTION USING THE EXPRESSION GIVEN BY 331 1451 24 GRIFFEY AND BIEDENHARN (NUCL. PHYS. 15, 636 (1960)). 331 1451 25 THE UNITS OF THIS INTENSITY DISTRIBUTION ARE ALPHAS 331 1451 26 PER KEV PER 100 DECAYS;AND THE NORMALIZATION IS TO 331 1451 27 2 ALPHAS PER DECAY. 331 1451 28 translated by Fred Mann (WHC) 331 1451 29 1 451 31 1 331 1451 30 8 457 23 1 331 1451 31 0.000000+0 0.000000+0 0 0 0 0 331 1 099999 0.000000+0 0.000000+0 0 0 0 0 331 0 0 0 3.008000+3 7.931275+0 0 0 0 2 331 8457 1 8.380000-1 6.000000-3 0 0 6 0 331 8457 2 6.290000+6 3.700000+5 0.000000+0 0.000000+0 3.975000+6 0.000000+0 331 8457 3 2.000000+0 1.000000+0 0 0 6 1 331 8457 4 1.400000+0 0.000000+0 1.600370+7 8.000001+2 1.000000+0 0.000000+0 331 8457 5 0.000000+0 1.000000+0 0 0 6 1 331 8457 6 1.000000-2 0.000000+0 6.290000+6 3.700000+5 0.000000+0 0.000000+0 331 8457 7 1.306400+7 7.800000+5 0 0 6 0 331 8457 8 1.000000+0 1.000000+0 1.000000+2 0.000000+0 0.000000+0 0.000000+0 331 8457 9 0.000000+0 4.000000+0 1 0 6 0 331 8457 10 0.000000+0 0.000000+0 3.975000+6 0.000000+0 1.995450+0 0.000000+0 331 8457 11 1.000000+0 0.000000+0 0 0 1 30 331 8457 12 30 1 331 8457 13 5.000000+5 0.000000+0 6.875000+5 1.794082-8 8.125000+5 4.650580-8 331 8457 14 9.375000+5 7.577238-8 1.062500+6 1.743967-7 1.187500+6 4.239645-7 331 8457 15 1.312500+6 7.376782-7 1.437500+6 9.441479-7 1.550000+6 9.571776-7 331 8457 16 1.650000+6 8.619610-7 1.750000+6 7.326668-7 1.850000+6 6.063795-7 331 8457 17 1.950000+6 5.071537-7 2.050000+6 4.269713-7 2.150000+6 3.668345-7 331 8457 18 2.250000+6 3.177228-7 2.350000+6 2.776316-7 2.450000+6 2.425518-7 331 8457 19 2.625000+6 1.753990-7 2.875000+6 1.302964-7 3.125000+6 9.762208-8 331 8457 20 3.375000+6 7.296600-8 3.625000+6 5.312085-8 3.875000+6 3.838733-8 331 8457 21 4.125000+6 2.716179-8 4.375000+6 1.884287-8 4.625000+6 1.272896-8 331 8457 22 4.875000+6 8.318925-9 5.250000+6 3.207296-9 5.750000+6 0.000000+0 331 8457 23 0.000000+0 0.000000+0 0 0 0 0 331 8 099999 0.000000+0 0.000000+0 0 0 0 0 331 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