161W ADOPTED LEVELS 11NDS 201111 161W H TYP=FUL$AUT=C. W. Reich$CIT=NDS 112,2497 (2011)$CUT=1-Jun-2011$ 161W D DATA SET UPGRADED (JUNE, 2009) BY CW REICH TO INCLUDE NEW Q VALUES AND 161W 2D ASSOCIATED COMMENTS. 161W Q -9.7E3 SY9.3E3 SY1.97E3 SY5923 4 2012WA38 161W cQ $Note: Current evaluation has used the following Q record 161W 2cQ $ -9531 syst 9116 syst 1820 syst 5922.8 {I36} 2009AuZZ 161W cQ Q(|b{+-}),S(n),S(p): the uncertainties assigned to these 161W 2cQ estimated values by 2009AuZZ are as follows: for Q(|b{+-}), 286; for 161W 3cQ S(n), 286; and, for S(p), 215. 161W cQ For Q(|b{+-}) and S(n), 2003Au03 report the following: 161W 2cQ for Q(|b{+-}), -9530 {i290}; for S(n), 9120 {i290}. 2003Au03 report 161W 3cQ the same values for S(p) and Q(|a) as those listed by 2009AuZZ, 161W 4cQ although with somewhat different uncertainties. 161W c All data are from the |a decay of {+161}W to {+157}Hf. See, also, the 161W 2c {+165}Os |a Decay data set. 161W L 0 409 MS 18 161W 2 L %A=73 3 $%EC+%B+=27 3 161W cL E The evaluator assumes the |a decay half-life is associated 161W 2cL with the ground state. 161W cL T from 1996Pa01. Other: 410 ms 40 (1979Ho10). 161W cL %EC+%B+ computed by the evaluator assuming that this is the only 161W 2cL other significant decay mode for {+161}W. 161W cL %A measured value (1996Pa01). Others: 90% {I29} (1989Wo02); 161W 2cL 82% {I26} (1981Ho10). 161W 165OS A DECAY 11NDS 201111 161W H TYP=FUL$AUT=C. W. Reich$CIT=NDS 112,2497 (2011)$CUT=1-Jun-2011$ 161W D DATA SET UPGRADED (JUNE, 2009) BY CW REICH TO INCLUDE NEW Q VALUE, 161W 2D JPI VALUE FOR THE 165OS GS, NEW REFERENCE AND REVISED COMMENTS. 161W c {+165}Os produced by {+106}Cd({+64}Zn,2p3n) (2002Ap03), 161W 2c {+106}Cd({+63}Cu,p3n) (1978Ca11), by a {+58}Ni beam on a Sn target 161W 3c (1981Ho10), and by {+58}Ni and {+70}Ge beams on {+112}Sn and {+106}Cd 161W 4c targets (1996Pa01). In 1981Ho10, the reaction products were separated 161W 5c with a velocity selector and counted after ion-implantation in a Si 161W 6c detector. In 1996Pa01 and 2002Ap03, the reaction products 161W 5c were separated in-flight using recoil mass separation and detected 161W 6c in double-sided silicon-strip detectors and recoil-decay tagging. 161W D Experimental methods: 161W D 1977Ca23: Shorter version of 1978Ca11. 161W D 1978Ca11: 106CD(62CU,P3N) reaction on enriched (86.2%) target with 161W 2D He-jet transfer and ALPHA counting. 161W D 1981Ho10: Several targets irradiated with 58NI and 107AG beams. 161W 2D Reaction products separated in velocity 161W 3D selector and implanted in position-sensitive detector. 161W D 1996Pa01, 2002Ap03: SEE THE BRIEF DISCUSSION ABOVE. 165OS P 0 (7/2-) 71 MS 3 6336 50 165OS DP E Evaluator assumes that the decaying level is the G.S. 165OS DP J FROM 1997Da07, FROM PROTON DECAYS FROM 166IR AND SYSTEMATICS 165OS DP T From 1996Pa01. OTHERS: 65 ms +70-30 (1981Ho10); 73 ms 8 165OS2DP (1991Se01). 165OS DP QP FROM 2009AuZZ. 2003Au03 REPORT QA=6340 50. THIS LARGE 165OS2DP UNCERTAINTY IN QA MAY BE TO ALLOW FOR THE POSSIBILITY THAT THE |a 165OS3DP TRANSITION DOES NOT CONNECT THE TWO GROUND STATES. 161W N 0.8 2 161W cN BR reported as 1.0 {I4} (1981Ho10). The evaluator has taken this 161W 2cN to mean 1.0 {I+0-4}. 161W L 0+X 161W cL E level populated by the |a branch is not known, but it 161W 2cL may be the ground state. 161W A 6183 9 100 161W cA E weighted average of: 6200 {I20} (1978Ca11); 6164 {I10} 161W 2cA (1981Ho10); and 6188 {I7} (1996Pa01). 161W cA IA only one |a branch reported.