108TE    112XE A DECAY                                           ENSDF    200810
108TE  H TYP=FUL$AUT=Jean Blachot$CIT=ENSDF$CUT=1-Jul-2008$
108TE  H TYP=FUL$AUT=Jean Blachot$CIT=NDS 91, 135 (2000)$CUT=1-Jun-2000$
108TE C  T1/2(112XE)=2.7 S 8, measured by 1979SC22, is used in calculations
108TExC  here.
108TE C
108TE C  The ALPHA branching of 0.8% +11-5 was determined by 1994PA11.
108TE2C  %A AP 0.84 was adopted by 1989DE33 from measurements of 1978RO19.
108TE3C  For the R0 calculations, %A=0.8 +11-5 is used here.
108TE C
108TE C  QA(112XE)=3330 7 is the recommended value of 1995AU04. The QA value of
108TE2C  3335 7, deduced by 1994PA11 from their measured EA (not quoted), was
108TE3C  used by 1995AU04 as input for their mass adjustment. EA=3199 12,
108TE4C  weighted average of EA's from 1981SC17 and 1992HEZU yields QA=3317 12.
108TE CA IA        ALPHA intensity per 100 A DECAYS.
108TE CA HF        R0(108TE)=1.64 6 is computed from HF(3211A)=1.0.
112XE  P 0.0          0+               2.7 S     8              3330      6
108TE  N                       0.0080  AP
108TE  L 0.0          0+
108TE  A 3211      7  100      1.0
108TE CA E         the measured ALPHA energies are 3190 15 (1992HEZU),
108TE2CA 3210 20 (1981SC17), and 3216 7 (1994PA11). The EA measured by 1994PA11
108TE3CA was used by 1995AU04 as an input. The adjusted QA value gives
108TE4CA EA=3211 7.
108TE CA IA        only one ALPHA group was observed. Intensity of a 2608-KEV
108TE2CA ALPHA to the first 2+ state at 625 KEV (observed in in-beam work) is
108TE3CA calculated as IA(2608A to 2+)/IA(3211A to GS)<8E-6 by requiring
108TE4CA HF(2608A)>1.