136I 136TE B- DECAY (17.63 S) 1979KE02,1977SC21 NDS18 201810
136I H TYP=FUL$AUT=E.A. MCCUTCHAN$CIT=NDS 152, 331 (2018)$CUT=1-Apr-2018$
136I c 1979Ke02: {+136}Te activity from {+235}U(n,F), E=thermal followed by
136I 2c mass separation at LOHENGRIN. Measured E|g, I|g, E|b, I|b, |b-|g
136I 3c coincidences using Ge(Li) detector and |b-detector telescope
136I 4c consisting of two plastic scintillators operated as |DE-E detectors;
136I 5c deduced decay Q values.
136I c 1979Bo26: {+136}Te activity from {+235}U(n,F) and {+241}Pu(n,F),
136I 2c E=thermal. High precision measurement of E|g using curved crystal
136I 3c spectrometer.
136I c 1978Ze08: {+136}Te activity from {+235}U(n,F), E=thermal followed by
136I 2c chemical separation. Measured E|g, I|g using Ge(Li) detectors. Report
136I 3c |g-ray energies and intensities for transitions below 800 keV.
136I c 1977Sc21: {+136}Te activity from {+235}U(n,F), E=thermal followed by
136I 2c mass separation at LOHENGRIN. Measured E|g, I|g, E|b, I|b, |b-|g
136I 3c coincidences using Ge(Li) detector and |b-detector telescope
136I 4c consisting of two plastic scintillators operated as |DE-E detectors.
136I 5c Similar results by same group are reported in 1977Pf01.
136I c Other: 1977Wo06
136I c $A total energy release of 5060 keV {I190} is calculated by the
136I 2c evaluator using the RadList code. This is in reasonable agreement
136I 3c with the decay Q value of 5120 keV {I14}.
136I cL E$From a least-squares fit to E|g, by evaluator.
136I cL J$From the Adopted Levels.
136I cL J(B)$1977Sc21 suggest possible configurations of [(|n h9/2)(|p
136I 2cL h11/2)(|p g7/2){+2}{-0+}]{-1+} and [(|n f7/2)(|p h11/2)(|p
136I 3cL g7/2){+2}{-2+}]{-0+,1+}.
136I cG E,RI$From 1977Sc21, except where noted.
136I cG M,MR$From the Adopted Gammas. Support from assignments derived from
136I 2cG this dataset are indicated in the comments.
136I cG E(A)$From 1979Bo26. Assignment based on agreement with E|g given by
136I 2cG 1977Bl12.
136I cG E(D),RI(E)$Alternate placement suggested by evaluator due to
136I 2cG intensity imbalance problems for the 579 level. I|g=7 divided by
136I 3cG evaluator to give zero imbalance at 579 level
136I cB IB(A)$Estimated from |DJ|p (evaluator).
136I D CC 1977Sc21 CALL THIS EKC BUT FROM THEIR DISCUSSION IT IS
136I 2D APPARENTLY ECC
136I tB
136I 2tB Level E|b (|b|g)|:
136I 3tB ----------------------------------------------------------
136I 4tB 222 4890 {I200} (87|g), 4710 {I200} (135|g)
136I 5tB 334 4825 {I150}, 4750 {I160} (1977Sc21) (333|g)
136I 6tB 579 4420 {I200} (491|g), 4340 {I200} (579|g)
136I 7tB 631 4525 {I200} (297|g), 4470 {I150}, 4460 {I150} (1977Sc21) (631|g
136I +tB )
136I 8tB 738 4290 {I170} (738|g)
136I 9tB 2656 2600 {I200} (579|g and 2569|g), 2465 {I150}, 2480 {I190} (1977
136I +tB Sc21) (2078|g)
136I AtB --------------------------------------------------------------
136I BtB |: From 1979Ke02 (|b|g-coin. Ge(Li),scin), except as noted
136I CtB --------------------------------------------------------------
136TE P 0.0 0+ 17.63 S 9 5120 14
136I N 0.186 21 1.0 1.0
136I cN NR$from |SI(|g+c.e.)(to g.s.)=95 {I4} assuming %|b{+-}n=1.1 {I6}
136I 2cN (1983ReZX,1984Ma39) and I|b(g.s.)<8.6% (from |DJ|p). 10% uncertainty
136I 3cN added in quadrature to the uncertainty in I|g-normalization since
136I 4cN |DI|g were not given.
136I PN 3
136I G 644.8 5 3
136I G 684.9 5 4
136I G 1341.2 5 10
136I G 1566.9 5 7
136I L 0.0 (1-)
136I B 8.6 LT 6.7 GT
136I F B FLAG=A
136I S B EAV=2234.5 66
136I cB E$others: 5095 {I100} (1979Ke02), 5100 {I150} (1977Sc21)
136I L 86.73 6 (2-,1-,0-)
136I G 87.3 2 64 M1(+E2) 0.18 LT 1.22 6 C
136I S G KC=0.960 21$LC=0.135 11$MC=0.0273 24$NC=0.0055 5$OC=0.00063 4
136I cG RI$other: 53 {I5} (1978Ze08)
136I cG CC$experimental value from I|g(x) (1977Sc21), corrected for 12 % {I2}
136I 2cG contribution to I(x) from conversion of other transitions.
136I cG M,MR$from |a(exp) in 1977Sc21.
136I L 222.11 6
136I G 135.385 3 15 [M1,E2] 0.46 15 C
136I F G FLAG=A
136I S G KC=0.36 9$LC=0.08 5$MC=0.016 10$NC=0.0032 18$OC=0.00033 16
136I cG RI$other: 13 {I2} (1978Ze08)
136I cG M$assumed M1+E2 for the purpose of balancing intensity through
136I 2cG the 87.3-keV level.
136I B 2.0 6 7.25 13
136I S B EAV=2129.8 66
136I cB E$other: 4800 {I200}, weighted average of |b|g data, see table.
136I L 333.97 6 (0-,1)
136I G 333.99 6 100 C
136I F G FLAG=A
136I B 15.8 18 6.3 1
136I S B EAV=2077.0 66
136I cB E$other: 4790 {I150}, weighted average of |b|g data, see table.
136I L 578.77 3 (0,1,2)
136I G 356.78 6 11 C
136I F G FLAG=A
136I cG RI$other: 19 {I3} (1978Ze08)
136I G 491.3 3 13 C
136I cG RI$other: 16 {I3} (1978Ze08)
136I G 578.75 3 98 C
136I F G FLAG=A
136I cG RI$other: 98 {I2} (1978Ze08)
136I B 0.5 LE 7.7 GE
136I S B EAV=1961.6 66
136I cB E$other: 4380 {I200}, weighted average of |b|g data, see table.
136I L 630.53 16 (0-,1)
136I G 297.3 5 3 C
136I cG RI$other: 8 {I2} (1978Ze08)
136I G 543.2 3 12 C
136I cG RI$other: 10 {I3} (1978Ze08)
136I G 630.7 2 56 C
136I cG RI$other: 55 {I4} (1978Ze08)
136I B 12.2 14 6.3 1
136I S B EAV=1937.2 66
136I cB E$other: 4480 {I150}, weighted average of |b|g data, see table.
136I L 738.21 19 (0,1,2)
136I G 738.2 2 29 C
136I cG RI$other: 29 {I3} (1978Ze08)
136I B 0.56 7 7.6 1
136I S B EAV=1886.5 66
136I cB E$other: 4290 {I170} from |b|g data, see table.
136I L 2656.42 22 1+ B
136I G 2077.9 3 119 C
136I G 2569.4 3 82 C
136I G 2656.0 6 3.6 AP * ?
136I F G FLAG=DE
136I B 38 4 4.7 1
136I S B EAV=990.8 65
136I cB E$other: 2520 {I150}, weighted average of |b|g data, see table.
136I L 3137.1 5 1+ B
136I G 2804.0 6 12
136I G 3049.5 6 11
136I B 4.3 5 5.3 1
136I S B EAV=771.9 64
136I L 3235.2 3 1+ B
136I G 2496.9 5 26 C
136I G 2604.8 6 6 C
136I G 2656.0 6 3.4 AP * ?
136I F G FLAG=E
136I G 3235.1 4 80
136I B 21.4 24 4.5 1
136I S B EAV=727.8 63