169RE 173IR A DECAY (2.16 S) 1996PA01,1992SC16,1986KE03ENSDF 201505
169RE H TYP=FUL$AUT=Coral M. Baglin$CIT=ENSDF$CUT=15-Mar-2015$
169RE H TYP=FUL$AUT=CORAL M. BAGLIN$CIT=NDS 109, 2033 (2008)$CUT=15-Jun-2008$
169RE DG CC$FROM BrIcc v2.3 (29-Mar-2013) 2008Ki07, "Frozen Orbitals" appr.
169RE CG MR$IF NO VALUE GIVEN IT WAS ASSUMED MR=1.00 FOR E2/M1,
169RE2CG MR=1.00 FOR E3/M2 AND MR=0.10 FOR ANY OTHER MIXED MULTIPOLARITIES.
169RE C Others: 1967SI02, 1982DE11,
169RE2C 2012PO01 (CALCULATION OF 173IR A DECAY HALF-LIFE).
169RE C 1967SI02: sources from 162ER(19F,8n) E=185 MEV with 14.1% 162ER target,
169RE2C 164ER(19F,10N) E=145-175 MEV with 35.1% 164ER target; helium-jet
169RE3C transport, Au-Si surface barrier detectors; measured EA, IA, parent
169RE4C ^T{-1/2}.
169RE C 1982DE11: sources from 63CU bombardments of indium and tin
169RE2C (E(63CU)=245-300 MEV, helium-jet transport); enriched
169RE3C targets; measured EA, IA (surface-barrier detector).
169RE C 1986KE03: sources from 90ZR bombardments of yttrium, zirconium
169RE2C and molybdenum (E(90ZR)=321-390 MEV; velocity-filter,
169RE3C evaporation-residue separation); enriched targets; measured
169RE4C EA, IA, %A(173IR) (silicon surface-barrier detectors, FWHM=25, 50 KEV).
169RE C 1992SC16: source from 141PR(36AR,xn), E=175-204 MEV;
169RE2C measured |a excit, EA, IA, EG, IG, I(XK),
169RE3C |a-(XK) coin, AG coin, |a(T); deduced |a branching; Si and Ge
169RE4C detectors.
169RE C 1996PA01: sources from heavy-ion fusion-evaporation reactions; recoil
169RE2C mass separator, double-sided SI strip detector (FWHM LE 20 KEV);
169RE3C measured EA, parent ^T{-1/2} and %A.
169RE C Parent T=2.16 S 4 from weighted average of 2.20 S 5 (1992SC16),
169RE2C 2.4 S 9 (1996PA01) AND 2.11 S 5 (2004GOZZ).
169RE CA HF R0=1.556 20 (based on R0 for 168W (1.56 2) and 170OS
169RE2CA (1.553 14) in 1998AK04), assuming E(parent)=226 9 (2012AU07)
169RE CG RI Photon intensity (1992SC16), relative to I(RE XK)=41 3.
169RE CL E FROM EG.
169RE CL J From Adopted Levels.
173IR P 0.0+X (11/2-) 2.16 S 4 5716 10
173IR CP E X=226 9 FROM 2012AU07.
169RE N 1.14 8 0.110 21
169RE CN BR Four measurements of branching exist: 0.0202 8 from
169RE2CN I(5665A)(173IR) relative to I(6150A+6110A)(177AU) (1986KE03), which
169RE3CN the evaluator revises to 0.031 1 because 1996PA01 report that only the
169RE4CN lower energy |a from 177AU (IA=65% in 1986KE03) is correlated with
169RE5CN the |a from 173IR(2.20 S); 0.12 1 from I(5674A)(173IR)/I(92G)(173OS)
169RE6CN (1992SC16) in a study in which 173OS is fed simultaneously by EC decay
169RE7CN from both 173IR isomers; 0.07 2 from 6118A(177AU)-5681A(173IR)
169RE8CN correlation (1996PA01); 0.14 3 (2004GOZZ). The evaluator adopts the
169RE0CN unweighted average (0.110 21) of the latter three measurements;
169RE9CN the weighted average of all data, by contrast, is 0.032 6 and the
169REACN unweighted average is 0.090 25.
169RE CN NR FROM TI(136G)=100.
169RE PN 3
169RE L 0.0 (9/2-)
169RE L 136.2 2 (11/2-)
169RE A 5672 3 100 1.3 3
169RE CA E weighted average of 5666 5 (5665 datum of 1967SI02 after
169RE2CA adjustment by 1991RY01), 5676 4 (1982DE11), 5681 13 (1996PA01), 5672 5
169RE3CA (2004GOZZ); QA=5942-x 3, based on EA, where x is the excitation of the
169RE4CA 173IR parent state; QA=5716 10 in 2012WA38 ASSUMES E=226 9 (2012AU07)
169RE5CA FOR THE 173IR PARENT STATE.
169RE CA Coincident with 136G (1992SC16).
169RE CA HF IF PARENT EXCITATION ENERGY IS 226 9 (2012AU07).
169RE G 136.2 2 31 2M1+E2 0.71 7 1.84 5
169RES G KC=1.33 7$LC=0.391 16$MC=0.094 5$
169RES G NC=0.0227 10$OC=0.00351 13$PC=0.000141 8
169RE CG M,MR from EKC=1.37 6 in 1992SC16.
169RE CG E FROM 1992SC16. OTHER EG: 136.4 5 (2004GOZZ).