169RE 173IR A DECAY (2.16 S) 2021HA32,1996PA01,1992SC1626NDS 202603
169RE H TYP=FUL$AUT=M. Shamsuzzoha Basunia$CIT=NDS 209, 1 (2026)$
169RE2 H CUT=1-Oct-2025$
169RE c 2021Ha32: Source obtained from proton induced spallation of UC{-x}
169RE2c target with E=1.4 GeV protons. Selective ionization using RILIS at CERN
169RE3c followed by mass separation. Ions of interest transported to the
169RE4c Windmill decay station. Measured E|a, I|a, |a(t) using surface barrier
169RE5c silicon detector and E|g, I|g, |a|g, |g(t) using a low energy Ge
169RE6c detector.
169RE c 1996Pa01: sources from heavy-ion fusion-evaporation reactions; recoil
169RE2c mass separator, double-sided Si strip detector (FWHM|<20 keV);
169RE3c measured E|a, parent T{-1/2} and %|a.
169RE c 1992Sc16: source from {+141}Pr({+36}Ar,xn), E=175-204 MeV;
169RE2c measured |a excit, E|a, I|a, E|g, I|g, I(K| x ray),
169RE3c |a-(K| x ray) coin, |a|g coin, |a(t); deduced |a branching; Si and Ge
169RE4c detectors.
169RE c 1986Ke03: sources from {+90}Zr bombardments of yttrium, zirconium
169RE2c and molybdenum (E({+90}Zr)=321-390 MeV; velocity-filter,
169RE3c evaporation-residue separation); enriched targets; measured
169RE4c E|a, I|a, %|a({+173}Ir) (silicon surface-barrier detectors, FWHM=25,
169RExc 50 keV).
169RE c 1967Si02: sources from {+162}Er({+19}F,8n) E=185 MeV with 14.1%
169RE2c {+162}Er target, {+164}Er({+19}F,10n) E=145-175 MeV with 35.1%
169RE3c {+164}Er target; helium-jet transport, Au-Si surface barrier
169RE4c detectors; measured E|a, I|a, parent T{-1/2}.
169RE c 1982De11: sources from {+63}Cu bombardments of indium and tin
169RE2c (E({+63}Cu)=245-300 MeV, helium-jet transport); enriched
169RE3c targets; measured E|a, I|a (surface-barrier detector).
169RE cA HF$The nuclear radius parameter r{-0}({+169}Re)=1.5690 {I81}
169RE2cA is deduced from interpolation (or unweighted average) of radius
169RE3cA parameters of the adjacent even-even nuclides: {+168}W (1.583 {I13})
169RE2cA and {+170}Os (1.5551 {I32}) in 2020Si16.
169RE cG RI Photon intensity (1992Sc16), relative to I(Re K| x ray)=41
169RExcG {I3}.
169RE cL E From E|g.
169RE cL J From Adopted Levels.
169RE cA IA From 2021Ha32
169RE dG CC$From BrIcc v2.3e (17-Jun-2020) 2008Ki07, "Frozen Orbitals" appr.
173IR P 219 16 11/2- 2.16 S 5 5716 9
173IR cP E$weighted average of 226 keV {I18} (2009An14) and 213 keV {I16}
173IR2cP (2021Ha32). Uncertainty is the lower experimental one from 2021Ha32.
173IR cP J$from {+173}Ir Adopted Levels in the ENSDF database (update).
173IR cP T$weighted average of 2.20 s {I5} (1992Sc16), 2.4 s {I9}
173IR2cP (1996Pa01) and 2.11 s {I5} (2004GoZZ). Uncertainty from 1992Sc16,
173IR3cP the lowest of the input uncertainties.
173IR cP QP$from 2021Wa16
169RE N 9.6 18 0.11 2
169RE cN BR weighted average of 12 {I1} (1992Sc16), 7 {I2}
169RE2cN (1996Pa01), and 14 {I3} (2004GoZZ). Other: 2.02 {I8} (1986Ke03), the
169RE3cN evaluator of 2008Ba31 revises the value to 0.031 {I1} based on the
169RE4cN 1996Pa01 report that only the lower energy |a from {+177}Au (I|a=65%
169RE5cN in 1986Ke03) is correlated with the |a from {+173}Ir (2.16 s).
169RE cN NR From I(|g+ce)(136|g)=94 {I1}
169RE PN 1.06 7 3
169RE L 0.0 (9/2-) 8.1 S 5
169RE A 5815 15 6 1 101 27 ?
169RE cA E$from 2021Ha32
169RE L 136.2 2 (11/2-)
169RE A 5673 4 94 1 1.7 4
169RE cA E weighted average of 5666 {I5} (5665 datum of 1967Si02 after
169RE2cA adjustment by 1991Ry01), 5676 {I4} (1982De11), 5681 {I13} (1996Pa01),
169RE3cA 5672 {I5} (2004GoZZ), and 5675 {I5} (2021Ha32).
169RE cA Coincident with 136|g (1992Sc16).
169RE G 136.2 2 31 2M1+E2 0.66 8 1.87 5
169RE2 G %IG=32.8 7
169RES G KC=1.37 7$LC=0.381 17$MC=0.092 5
169RES G NC=0.0220 11$OC=0.00343 14$PC=0.000146 8
169RE cG E from 1992Sc16. Other E|g: 136.4 {I5} (2004GoZZ).
169RE cG M,MR from |a(K)exp=1.37 {I6} (1992Sc16).