156HF    160W A DECAY                  1996PA01                  12NDS    201210
156HF  H TYP=FUL$AUT=C. W. REICH$CIT=NDS 113, 2537 (2012)$CUT=1-Mar-2012$
156HF D  DATA SET MODIFIED (SEPTEMBER, 2011) BY CW REICH, TO INCLUDE QP
156HF2D   VALUE OF 2011AuZZ.
156HF c  The listed comments have been adapted, and in some cases modified, from
156HF2c  those in the evaluation by 1998Ak04.
160W   P 0.0         0+                91 MS     5              6066      5
160W  DP T         From 1996Pa01, |a(t). Other: 81 MS 15 (1981Ho10).
160W  DP QP        From 2011AuZZ. From E|a=5912 5 (1996Pa01), QA=6064 5 is
160W 2DP  computed.
156HF  N                       0.87    8
156HF cN BR$From 1996Pa01. Other: %|a=94~{I40} (1981Ho10).
156HF  L 0.0         0+
156HF  A 5912      5   100     1.0
156HF cA HF        r{-0}({+156}Hf)=1.557 {I10} is obtained from HF(5912|a)=1.0.
156HF cA E$From 1996Pa01. Other: E|a=5920~{I10}, (1979Ho10).
156HF cA IA        |a intensity per 100 |a decays.
156HF cA IA        Only one |a group is observed. An upper limit of 0.037% of
156HF2cA  |a decays is calculated for an unobserved |?5130-keV |a to the 2+
156HF3cA  state, expected at |?800 keV in {+156}Hf, by requiring HF(5130|a)>1.
156HF4cA  E(first 2+ state in {+156}Hf) is extrapolated as |?800 keV, from
156HF5cA  E(2+ state in {+158}Hf)=610, E(2+ state in {+160}Hf)=389 {I6}. The
156HF6cA  2+ state in {+156}Hf has not yet been observed in |a decay.