192PB 196PO A DECAY 1985VA03,1989DE18 12NDS 201209 192PB H TYP=FUL$AUT=Coral M. Baglin$CIT=NDS 113, 1871 (2012)$CUT=15-Jun-2012$ 192PB C Others: 1967SI09, 1967TR06, 1971HO01, 1993WA04, 1994WA13, 1995DE43, 192PB2C 1996TA18, 1997PU01, 2003VA16, 2005UU02, 2005UU03. 192PB C 1985VA03: sources from 20NE bombardments of tungsten foil 192PB2C (natural), E(20NE) LE 225 MEV, on-line mass separation (^LISOL); 192PB3C measured EA, IA (silicon surface-barrier detectors), parent T. 192PB C 1989DE18: sources from 182W(20NE,6N), E(20NE) LT 240 MEV, mass 192PB2C separation; measured EA, ACE(T); deduced mixing between 192PB3c |p(2p-2h) 192PB4C intruder state (767 level) and ground state. 192PB C 1993WA04: mass separated product (^LISOL separator) from 20NE (E LE 240 192PB2C MEV) bombardment of 182W target; measured EA, parent T. |a branching 192PB3C determined from study of 200RN A DECAY to 196PO. 192PB C 1996TA18: 196PO from 200RN A DECAY; measured EA (FWHM AP 28 KEV), 192PB2C T(196PO). 192PB C 2009NI11: CALCULATED 196PO |a DECAY HALF-LIFE USING GENERALIZED DENSITY 192PB2C DEPENDENT CLUSTER MODEL WITH DOUBLE FOLDED Woods-Saxon POTENTIALS. 192PB C 2009WA01: CALCULATED |a DECAY BRANCHING TO GS AND EXCITED 0+ STATES 192PB2C WITHIN THE FRAMEWORK OF THE GENERALIZED LIQUID DROP MODEL. 192PB DA HF R0(192PB)=1.506 6 IF T=6.5 S 4 (1998AK04). 192PB CA HF R0(192PB)=1.513 3 from HF(to GS)=1.0. This assumes 192PB2CA T=5.60 S 8 for 196PO. 192PB3CA See 1995DE43 for discussion of hindrance for decay to 0+ 767 intruder 192PB4CA state; these authors report HF(to 767)=2.5 1 cf. 2.9 7 in 1985VA03 192PB5CA AND 2.74 16 CALCULATED HERE. 192PB CA IA Measured, but not stated, in 1985VA03. 1994WA13 indicate 192PB2CA I(6518A):I(5769A)=94:0.021. 192PB CA E(A) Weighted average of 6526 8 (1967SI09), 6518 5 192PB2CA (1967TR06, after 0.7 KEV increase recommended in 1991RY01), 6522 8 192PB3CA (1971HO01, after 1.3 KEV increase recommended in 1991RY01), 192PB4CA 6521 5 (1985VA03), 6521 5 (1993WA04), 6518 5 (1996TA18; |DE|a=1 KEV 192PB5CA (statistical), LE 5 KEV (systematic)), 6533 6 (2005UU03). 192PB6CA 1991RY01 recommended EA=6520 3 based on the pre-1991 data above. 192PB7CA Other EA: 6520 (1977DE32), 6520 30 (1997PU01). 192PB CG M FROM Adopted Gammas. 192PB CL J,T FROM Adopted Levels. 196PO P 0.0 0+ 5.60 S 8 6658.0 24 196PO CP T 5.60 S 8 IS WEIGHTED AVERAGE OF 5.5 S 5 (1967SI09), 196PO2CP 5.8 S 2 (1985VA03), 5.8 S 2 (1993WA04), 5.5 S 1 (1997PU01). 196PO3CP OTHERS: 5.1 S +31-14 (2005UU02), 6.8 S 3 (1996TA18). 196PO4CP The datum from 1996TA18 IS a statistical outlier. 192PB N 0.94 5 192PB CN BR %A(196PO)=94 5 from 1993WA04. This is a little larger than 192PB2CN expected on the basis of the calculated partial |b decay half-life 192PB3CN of 39.5 S (1997MO25); the latter implies %(EC+B+)=14. 192PB L 0.0 0+ 3.5 M 1 192PB A 6521.9 21 99.978 1.0 A 192PB CA EA=6521.9 21 IMPLIES QA=6657.8 21 cf. 6658.0 24 FROM 192PB2CA 2011AUZZ. 192PB L 767 0+ 0.75 NS 10 192PB CL E based on EA. 192PB CL T from ACE(T) (1989DE18). 192PB A 5769 0.022 2.74 16 192PB CA E from 1985VA03. Authors do not state uncertainty; however, 192PB2CA DE=6 KEV IS QUOTED IN SUMMARY TABLE ^II BY 2003VA16. 192PB3CA Also observed by 1989DE18. 192PB CA COINCIDENT WITH PB X-RAYS (2000VA34). 192PB G 769 E0 192PB CG E rounded value from Adopted Gammas; conversion electrons 192PB2CG observed in coincidence with 5769A (1989DE18). 192PB L 854 2+ ? 192PB CL E rounded-off value from Adopted Levels. 192PB A 5687 CA 0.0065 LE 3.6 GE ? 192PB CA E deduced from E(level) and QA (no peak visible in |a spectrum 192PB2CA from 1985VA03). 192PB CA HF calculated by 1985VA03. 192PB CA IA 1985VA03 obtained (but did not state) an upper limit for 192PB2CA this intensity. Based on HF GE 3.6 given in 1985VA03, IA LE 0.0065. 192PB3CA An upper limit of 0.024 is imposed by the requirement that HF GE 1.0.