95MO 95NB B- DECAY (3.61 D) 1999BEZS,1999BEZQ,2000HE1410NDS 201010
95MO H TYP=FUL$AUT=S. K. Basu, G. Mukherjee, A. A. Sonzogni$
95MO2 H CIT=NDS 111, 2555 (2010)$CUT=30-Jun-2009$
95MO C 1999BEZS,1999BEZQ: Evaluation by M.-M. Be, ^R. Helmer, ^N. Coursol,
95MO2C and F. Lagoutine, January 1998 and including information
95MO3C from a previous evaluation (1993Bu08). This evaluation was done as
95MO4C part of a collaboration of evaluators from Laboratoire National Henri
95MO5C Becquerel (LNHB) in France; Physikalisch-Technische Bundesanstalt
95MO6C (^PTB) in Germany; ^HMS Sultan and ^AEA Technology in the United
95MO7C Kingdom; Khlopin Radium Institute (KRI) in Russia; Centro de
95MO8C Investigaciones Energeticas, Medioambientales, y Tecnologicas
95MO9C (^CIEMAT) and Universidad Nacional a Distancia (^UNED) in Spain; and
95MOaC Brookhaven National Laboratory (^BNL), Lawrence Berkeley National
95MObC Laboratory (^LBNL), and Idaho National Engineering and Environmental
95MOcC Laboratory (^INEEL) in the United States.
95MO C Measurements include: measured |g's, Ge(Li) and Compton-suppressed
95MO2C Ge(Li), mixed and pure sources (1972Er08); see {+95}Zr |b{+-} decay
95MO3C for details (1974An22); see {+95}Nb |b{+-} decay (34.975 d) for
95MO4C details (1976Ho04).
95MO CB IB$The intensity of the |b- transition to the ground state has been
95MO2CB deduced by the evaluators from the |b spectrum analysis relative to
95MO3CB the intensity of the K electrons from the 235-keV isomeric decay |g
95MO4CB of 1974An22. 1974An22 report I|b- to ground state of 5.5% {I4} of
95MO5CB the IT decays and I|b- to 204-keV level of 0.5% {I1}. Current
95MO6CB I|g(204)/I|g(234) data imply that I{-|b-}(204) is more nearly 2.4% of
95MO7CB all decays of the isomer. Therefore, this evaluator has taken the
95MO8CB total |b- intensity to these two levels to be 5.6% and divided it
95MO9CB 3.2% and 2.4%. Since Kurie-Fermi plot of 1974An22 does not show two
95MOaCB components, the uncertainty in the total intensity may be larger than
95MObCB reported; the evaluator has assigned 5.6% {I10}. The I|b(204) is
95MOcCB assigned as 2.4% {I3} from the |g data, leaving the I|b(ground state)
95MOdCB = 3.2% {I10}.
95MO CG E$From 2000He14 where they are associated with the {+95m}Tc |e decay
95MO2CG (61 d), except 218, 253, and 616 |g's which are from the level
95MO3CG energies.
95MO CG RI$From 1976Ho04 with the addition of the data for the 218, 253, 616,
95MO2CG 1039 |g's from the {+95m}Tc |e decay (61 d).
95MO CG M,MR,CC$From the {+95}Mo Adopted Gammas
95MO CL J,T$From Adopted Levels
95MO D CC$ FROM BrIcc v2.2a (13-Jul-2008) 2008Ki07, "Frozen Orbitals" appr.
95NB P 234.70 14 1/2- 3.61 D 3 925.6 5
95MO N 1.00 0.056 6 17.857
95MO CN NR$From %I|g(204|g)=2.33 {I16} and I|g(204|g)=100 {I3}. %I|g is from
95MO2CN I|g(204|g)/I|g({+95}Nb 236|g)=0.094 {I34} (1976Ho04), %IT=94.4 {I6},
95MO3CN and |a({+95}Nb 236|g)=2.81. Note that I|g(204|g)/I|g({+95}Nb
95MO4CN 236|g)=0.022 {I4} and ce(K)(204|g)/ce(K)({+95}Nb 236|g)=4.5|*10{+-4}
95MO5CN {I11} (1974An22) are discrepant while I|g(204|g)/I|g({+95}Nb
95MO6CN 236|g)=0.095 {I22} derived by 1974An22 from the data of 1972Er08
95MO7CN agrees. Other %I|g: 2.36 {I7} (1976Ho04)
95MO PN 0.0233 16 1.0 3
95MO L 0.0 5/2+ STABLE
95MO B 1160 5 3.2 10 9.20 14 1U
95MOS B EAV=437.37 22
95MO CB E$from 1974An22
95MO CB LOGFT$observed 1{+st}-forbidden unique spectrum shape (1974An22)
95MO L 204.116 2 3/2+
95MO G 204.1161 17 41 M1+E2 -0.62 7 0.052 3
95MOS G KC=0.0449 23$LC=0.0058 4$MC=0.00103 7$NC=0.000154 9$OC=7.5E-6 4$
95MOS G NC+=0.000161 10
95MO B 2.4 3 8.4 1
95MOS B EAV=334.55 22
95MO L 786.201 3 1/2+
95MO G 582.0775 21 0.85
95MO G 786.1922 27 0.24
95MO B 0.071 9 8.4 1
95MOS B EAV=111.68 18
95MO L 820.628 4 3/2+
95MO G 616.507 8 0.0017
95MO G 820.622 7 0.0061
95MO B 0.00037 22 10.6 3 ?
95MOS B EAV=100.06 18
95MO L 1039.269 4 1/2+
95MO G 218.640 8 0.000001LE ?
95MO G 253.070 3 0.00002LE ?
95MO G 835.146 6 0.001 LE ?
95MO G 1039.260 6 0.0001 LE ?
95MO B 0.000027LE 10.3 GE ?
95MOS B EAV=32.20 15