102RU 102RH EC DECAY (207.3 D) 09NDS 200908
102RU H TYP=ERR$AUT=J. Tuli,B. Singh$DAT=7-Jun-11$COM=corrected T(475)$
102RU H TYP=FUL$AUT=D. DE FRENNE$CIT=NDS 110, 1745 (2009)$CUT=31-Dec-2008$
102RU c Because of the many close-lying doublets, the internal conversion
102RU2c data of 1961Bo35, 1961Hi06 and 1968Ad02 are not included.
102RU c Coincidence measurements by 1969Ko24, 1970Ta03 and 1971Ta01 are
102RU2c summarized on the decay scheme.
102RU c Absolute intensities were calculated from
102RU2c I|b{+-}(g.s.):I|b{++}(g.s.):I|b{++}(475)=100.0 {I15}:54.6 {I10}:21.2
102RU3c {I5}, |e/|b{++}(g.s.)=1.69 {I4}, |e/|b{++}(475)=7.80 {I25}.
102RU4c If the g.s. transition is first-forbidden unique, as would follow from
102RU5c the J|p=2- assignment of 1975Sc09 for the 207.3-d {+102}Rh isomer, the
102RU6c intensities will have to be recalculated using |e/|b{++}(g.s.)=5.89.
102RU cE TI From |g-intensity balance at each level, except for
102RU2cE the g.s.
102RU cG E,RI$|g-ray energies and intensities are primarily from 1969Ge02,
102RU2cG unless noted otherwise.
102RUxcG Other references: 1969Ko24, 1970Hu02, 1970Ta03, 1971Ta01, 1981Ko23
102RU CG M,MR$From |g|g(|q) results of 1970Si13. See also 1968Ad02.
102RU2CG Mixed transitions have multipolarity=E2+M1 from known J|p.
102RU CL J$From adopted levels
102RU CL E$From a least-squares procedure using observed gammas
102RH P 0.0 (1-,2-) 207.3 D 17 2323 5
102RU N 1.28 0.78 5 1.28
102RU cN NR$Normalization based on %|e+%|b{++}=78 {I5} and %|e+%|b{++} to g.s.
102RUxcN of 29 {I1}
102RU PN 1.0 1.0 3
102RU L 0 0+
102RU E 2321 7 10.5 5 17.2 7 8.97223 29 1
102RU2 E EAV= 582 10$CK= 0.539 11$CL= 0.0664 14$CM+= 0.0156 4
102RU cE E from E|b=1299 {I7}; weighted average of 1303 {I10} (1963Bo17)
102RU2cE and 1295 {I10} (1961Hi06). |b-ray does not have first-forbidden
102RU3cE unique shape (see also 1969Ko24)
102RU cE IB from 1969Ge02 based on I|b{++}(g.s.)/I|b{+-}(g.s.) in
102RUxcE {+102}Rh (T{-1/2}=207 d) 10
102RU L 475.07 4 2+ 18.4 PS 3
102RU CL T$Adopted value. 12.2 PS 20 from |g|g(t) (1963De21)
102RU E 1847 11 4.2 5 30.818 8.52 3
102RU2 E EAV= 372 10$CK= 0.764 8$CL= 0.0946 11$CM+= 0.02227 24
102RU cE E from E|b=825 {I11}; weighted average of 830 {I15} (1963Bo17)
102RU2cE and 820 {I15} (1961Hi06)
102RU G 475.06 4 46 3 E2 C
102RU L 943.67 5 0+
102RU CL J (469)(475)(|q) is consistent with J(Q)2(Q)0 for
102RU2CL J(944 level)=0, mult. (469|g)=E2 (1970Si13)
102RU E 0.018 5 2.6820 9.32 4
102RU2 E EAV= 170 9$CK= 0.8609 13$CL= 0.10730 21$CM+= 0.02529 5
102RU G 468.58 4 2.9 2 E2 C
102RU2 G EKC=5.9E-3 7 (1981KO23)$ KC=5.63E-3
102RU G 943.48 E0 0.0031 5
102RU CG |r(E0)=0.12 {I1} (1986Gi04). Other: 0.092 (1981Ko23)
102RU CG B(E0)/B(E2)=0.013 {I2} (1986Gi04,1981Ko23)
102RU CG TI calculated by evaluator from Ice values of 1986Gi04
102RU CG E completely converted |g-transition observed by 1981Ko23,
102RUxCG 1986Gi04
102RU L 1103.14 5 2+
102RU E 6.6 4 8.83 4
102RU2 E CK= 0.8656$CL= 0.1083$CM+= 0.02553
102RU G 628.05 5 4.5 4 E2(+M1)+E0-60 20 C
102RU CG CC from 1986Gi04
102RU CG M from |a(K)exp=2.58|*10{+-3} {I11} (1993Fa11)
102RU G 1103.16 6 2.9 1 E2 C
102RU CG B(E0)/B(E2)<0.032 (1986Gi04)
102RU CG M from |a(K)exp=2.58|*10{+-3} {I11} (1993Fa11)
102RU L 1106.37 6 4+
102RU E 0.10 LE 10.6 GE
102RU2 E CK= 0.8656$CL= 0.1083$CM+= 0.02553
102RU G 631.29 5 0.10 3 E2 C
102RU CG M from |a(K)exp=6.27|*10{+-4} {I30} (1993Fa11)
102RU L 1521.66 6 3+
102RU E 0.17 LE 10.0 GE
102RU2 E CK= 0.8642$CL= 0.10986 12$CM+= 0.02596 4
102RU G 415.25 150.03 2 C
102RU G 418.52 180.12 2 E2+M1 -7.2 10 C
102RU G 1046.59 7 0.43 3 E2+M1 -7.0 6 C
102RU L 1580.55 7 2+
102RU CL J (1106)(475)(|q) is consistent with J(d,Q)2(Q)0 for
102RU2CL J(1581 level)=2 or 3. Not consistent with J=1 (1970Si13)
102RU G 636.81 100.23 3 C
102RU G 1105.7 3 0.39 3 E2+M1+E0 +0.25 3 C
102RU CG M from |a(K)exp=8.20|*10{+-4} {I54} (1993Fa11)
102RU G 1580.5 3 0.05 1 C
102RU L 1837.10 9 0+
102RU CL J (1362)(475)(|q) is consistent with J(Q)2(Q)0 for
102RU2CL J(1837 level)=0, mult. (1362|g)=E2 (1970Si13)
102RU E 0.51 6 9.13 7
102RU2 E CK= 0.8605$CL= 0.1128 4$CM+= 0.02676 10
102RU G 256.8 4 0.02 1
102RU CG E observed by 1969Ko24 and 1970Hu02.
102RU G 733.93 8 0.10 2 C
102RU G 1362.1 2 0.39 5 E2 C
102RU CG ce(K)(1837)/ce(K)(1362)|<3.7|*10{+-2}
102RU CG B(E0)/B(E2)<0.019 (1986Gi04)
102RU L 2036.99 132+
102RU CL J (1562)(475)(|q) is consistent with J(d,Q)2(Q)0 for
102RU2CL J(8037 level)=2 and |d(1562|g)=-1.9 {I4}. Not consistent with J=1 or 3
102RU3CL for any |d (1970Si13)
102RU E 0.23 5 9.0112
102RU2 E CK= 0.8536 14$CL= 0.1181 11$CM+= 0.0282 3
102RU G 456.42 150.08 2 C
102RU G 930.5 3 0.03 2
102RU G 933.2 4 0.02 1 ?
102RU CG E observed by 1969Ko24 only.
102RU G 1562.2 4 0.11 3 E2+M1+E0 -1.9 4 C
102RU CG M from |a(K)exp=6.8|*10{+-4} {I16} (1993Fa11)
102RU G 2037.0 3 0.03 2
102RU L 2044.2 3 3-
102RU G 1568.7 6 0.01 1 C
102RU G 2044.1 4 0.001 1 ?
102RU CG E observed by 1971Ta01 only.
102RU L 2261.23 6 2-
102RU CL J (1152)(1103)(|q) is consistent with J(d,Q)2(Q)0 for
102RU2CL J(2261 level)=2 and |d(1158|g)=-0.25 {I5}. Not consistent with J=1 or
102RU3CL 3. For additional |g|g(|q) data, see 1970Si13
102RU CL J the parity is obtained from |a(K)exp measurements of 1993Fa11
102RU E 1.8 1 6.7 4
102RU2 E CK= 0.78 7$CL= 0.17 5$CM+= 0.044 14
102RU G 216.9 3 0.01 1 C
102RU CG E observed by 1970Ta03 only.
102RU CG RI deduced from 1971Ta01.
102RU G 224.9 4 0.05 3 ?
102RU CG E observed by 1969Ko24 only.
102RU G 680.66 5 0.58 4 E1 C
102RU CG M from |a(K)exp=6.8|*10{+-4} {I24} (1993Fa11)
102RU G 739.58 7 0.53 8 (E1+M2) -0.1 1 C
102RU G 1158.10 6 0.58 4 E1 C
102RU CG M from |a(K)exp=2.64|*10{+-4} {I25} (1993Fa11)
102RU G 1786.4 4 0.01 1
102RU G 2261.3 4 0.02 2