127I 127XE EC DECAY (36.4 D) 1967GE10,1968SC14,1977GE1011NDS 201108
127I H TYP=FUL$AUT=A. HASHIZUME$CIT=NDS 112, 1647 (2011)$CUT=1-Oct-2009$
127I c 1967Ge10: {+126}Xe(n,|g) mass separation, magnetic spectrometer ce,
127I 2c semi |g, |g|g(t), |g|g(|q)
127I c 1974Co05: {+127}I(p,n), semi |g, absolute photon intensity measurement
127I c 1977Ge10: {+126}Xe(n,|g), semi |g, absolute photon intensity
127I xc measurement
127I c Others: |g|g(|q): 1964Jh02, 1966Le09, 1970Le16
127I c The level scheme is that proposed by 1967Ge10 and 1968Sc14
127I cL E From a least-squares fit to E(|g's)
127I cL J,T From adopted levels
127I cG E 1977Ge10
127I cG RI I|g's are relative to I(202.86|g)=100 (1977Ge10)
127I cG CC$Theoretical conversion coefficients are calculated using BrIcc code
127I 2cG for the multipolarity indicated.
127I cG M From L1:L2:L3
127I cG MR From adopted levels, gammas
127I cG I(K| x ray)/I(0.2029|g)=1.17 {I7} (1958Fo48)
127XE P 0.0 1/2+ 36.4 D 1 662.3 20
127I N 0.687 120.687 121.0 1.0
127I cN NR No direct |e decay to g.s. is assumed. The uncertainty of
127I 2cN I(202.86|g) is assumed 2%. Total transition intensity is obtained by
127I 3cN using conversion coefficients calculated by BrIcc (evaluator).
127I 4cN (I(202.86|g)/100 |e decays)=70.6 {I22} from absolute measurement;
127I 5cN (I(202.86|g)/100 |e decays)=68.3 {I4} from relative photon intensity
127I 6cN measurement combined with theoretical HSIcc conversion coefficients
127I 7cN and from decay scheme (1977Ge10)
127I PN 3
127I L 0.0 5/2+ STABLE
127I L 57.60911 7/2+ 1.86 NS 11
127I cL T from (ce(K) 145|g)(K| x ray)(t) (1965Ge04). Others: 1.5 ns
127I 2cL {I3} (1964Jh02), 2.0 ns {I2} (1962Th12)
127I G 57.61 2 1.79 10M1+E2 -0.083 5 3.72 8.5 5 C
127I 3 G K/L=6.8 (1967Ge10)$ L/M=4.7 6 (1967Ge10)$ M/(N+O)=5.4 +41-19 (1967Ge10)
127I S G K/T=0.669 6$L/T=0.0951 18$M/T=0.0193 4$N+/T=0.00432 9
127I S G N/T=0.00388 8$O/T=0.000443 9
127I cG $ce(K)/(I{-|g}+I{-ce})=0.669 {i6}; ce(L)/(I{-|g}+I{-ce})=0.0951 {i18};
127I 2cG ce(M)/(I{-|g}+I{-ce})=0.0193 {i4}; ce(N+)/(I{-|g}+I{-ce})=0.00432 {i9}
127I cG From L1:L2:L3=1.0:0.118 {I4}:0.068 {I4} (1967Ge10)
127I cG TI from I(|g+ce)(145|g)
127I L 202.860 8 3/2+ 0.39 NS 1
127I cL (|eK)(|w(K))=0.750 {I16} (1964Br26)
127I cL T unweighted av of 0.38 ns {I1} (1966Ge13) and 0.40 ns {I1}
127I 2cL (1968Ko01) from |g|g(t)
127I E 53.0 14 6.607 13
127I S E CK=0.8418$CL=0.12441 7$CM+=0.03377 2
127I G 145.252 10 6.28 19E2 0.471 C
127I 3 G K/L=3.6 3$ L/M=4.9 9$ M/(N+O)=4.3 +19-12 (1967Ge10)
127I S G KC=0.357 5$LC=0.0906 13$MC=0.0189 3$NC+=0.00405 6
127I S G NC=0.00369 6$OC=0.000362 5
127I cG L1:L2:L3=1.0:0.76 {I10}:0.87 {I11} (1967Ge10)
127I cG M from L1:L2:L3
127I G 202.860 10 100 M1+E2 +0.52 5 0.1143 22 C
127I 3 G K/L=6.5 1$ L/M=5.5 5$ M/(N+O)=2.3 4 (1967Ge10)
127I S G KC=0.0965 17$LC=0.0142 5$MC=0.00289 10$NC+=0.000645 20
127I S G NC=0.000580 18$OC=6.50E-5 17
127I cG L1:L2:L3=1.0:0.160 {I15}:0.121 {I13} (1967Ge10)
127I L 374.992 9 1/2+ 0.135 NS LE
127I cL T from X|g(t), ce|g(t) (1968Ko01)
127I cL (|eK)(|w(K))=0.705 {I4} (1964Br26)
127I E 47.6 14 6.210 15
127I S E CK=0.8303 3$CL=0.13317 19$CM+=0.03654 6
127I G 172.132 10 37.4 11M1+E2 -0.085 6 0.1649 24 C
127I 3 G K/L=7.6 5$ L/M=4.8 6 (1967Ge10)
127I S G KC=0.1419 20$LC=0.0185 3$MC=0.00373 6$NC+=0.000843 12
127I S G NC=0.000754 11$OC=8.82E-5 13
127I cG L1:L2:L3=1.0:0.066 {I3}:0.016 {I4}, M/(N+O)=4.0 {I+9-7}
127I xcG (1967Ge10)
127I G 374.991 12 25.2 8 E2 0.0199
127I 3 G K/L=5.4 5 (1967Ge10)
127I S G KC=0.01671 24$LC=0.00257 4$MC=0.000524 8$NC+=0.0001158 17
127I S G NC=0.0001044 15$OC=1.144E-5 16
127I cG L1:L2:L3=1.0:0.26 {I5}:0.17 {I5} (1967Ge10)
127I L 618.4 33/2+
127I E 0.0143 9 7.41 10
127I S E CK=0.31 7$CL=0.52 5$CM+=0.170 18
127I G 618.4 3 0.0208 12
127I cG E from {+127}Te |b{+-} decay (1970Ap02)