87ZR 87ZR IT DECAY (14.0 S) 1972TU03,1974VO03,1977KO0515NDS 201510
87ZR H TYP=FUL$AUT=T.D. Johnson and W.D. Kulp(a)$CIT=NDS 129, 1 (2015)$
87ZR2 H CUT=27-Jul-2015$
87ZR DG CC$FROM BrIcc v2.3a (30-Jun-2013) 2008Ki07, "Frozen Orbitals" appr.
87ZR P 335.84 19(1/2)- 14.0 S 2
87ZR c 1972Tu03: produced by {+89}Y(p,3n); measured |g singles, |g|g
87ZR2c coincidences
87ZR c 1974Vo03: produced by spallation by 660 MeV p on Ag target
87ZR c 1977Ko05: produced by {+58}Ni({+32}S,3p)
87ZR cL J From {+87}Zr Adopted Levels
87ZR cG The decay curves of the 135- and 201-keV |g's show
87ZR2cG a half-life of 14 s.
87ZR cG E From Adopted Levels
87ZR2cG
87ZR CG RI,M,MR$ Given I|g(135|g)/I|g(201|g)=0.285 {I 8}
87ZR2CG from 1972To03,
87ZR3CG mult(201|g)=M1+E2 with MR=-0.35 or -2.6 from |g(|q) in (HI,xn|g),
87ZR4CG the requirement of an intensity balance at the 201 level, and
87ZR5CG I|g normalization to I|g(1+|a)=100 for each transition, one gets
87ZR6CG |a(135|g)(exp)=2.79 {I11} or 2.64 {I11} for the two values of
87ZR7CG |d, either of which establishes mult=E3 with |a=2.67 {I4} and thus
87ZR8CG I|g(135|g)=27.2 {I3}. One then has I|g(201|g)=95.8 {I31} which
87ZR9CG gives |a(201|g)(exp)=0.044 {I33} from which one gets |d LT 2,
87ZRACG eliminating the larger solution. With |a(201|g)=0.037 for |d=-0.35
87ZRBCG one gets I|g(201|g)=96.4 with an uncertainty depending on that for
87ZRCCG |d, unspecified by the authors. For an uncertainty of 30%, one gets
87ZRDCG I|g=96.4 {I 4}.
87ZR N 1.0 1.0 1.0
87ZR PN 3
87ZR L 0.0 9/2+
87ZR L 200.91 12 7/2+
87ZR G 201.02 14 96.4 M1+E2 -0.35 0.0370 C
87ZRS G KC=0.0323 5$LC=0.00386 6$MC=0.000671 10
87ZRS G NC=9.41E-5 14$OC=6.17E-6 9
87ZR cG M,MR from Adopted Levels.
87ZR L 335.84 19 1/2- 14.0 S 2 M1
87ZR cL T from 1972Tu03, |g(t)
87ZR G 134.93 15 27.2 3 E3 2.67 4 C
87ZR3 G ECC=2.64 16
87ZR cG M from |a(exp).
87ZRB G BE3W=0.0643 15
87ZRS G KC=1.97 4$LC=0.568 10$MC=0.1014 18
87ZRS G NC=0.01286 22$OC=0.000313 5