126TE 126I EC DECAY 1977JA04,1998FO05 22NDS 202205
126TE H TYP=FUL$AUT=H. Iimura, J.Katakura, S. Ohya$CIT=NDS 180, 1 (2022)$
126TE2 H CUT=1-Oct-2021$
126TE c 1977Ja04: {+127}I(n,2n), Compton suppression spectrometer, semi |g.
126TE c 1998Fo05: {+127}I(n,2n); HPGe, scin, gas counter |g, |b, K| x ray;
126TExc 4|p|b|g, X|g coin
126TE c Others: semi |g: 1970Ga32, 1970Si05, 1971Mi20, 1971Zh01, 1972Ka20,
126TE2c 1975Ok04, 1976Gr04; magnetic spectrometer: 1970Ga32, 1971Zh01;
126TE3c |g|g(|q): 1959Sa05, 1971Gr14, 1971Ta04.
126TE c The decay scheme is that proposed by 1977Ja04.
126TE2c Evaluators note that the 1396(0+), 1685(0+), 2601(0+) and
126TE3c 2051 states in {+126}Te in the decay proposed by 1971Zh01
126TE4c have not been confirmed by 1975Ok04, 1976Gr04 or 1977Ja04.
126TE c See also {+126}I |b{+-} decay.
126TE tG
126TE2tG |g|g(|q) data
126TE3tG
126TE4tG 1971Ta04
126TE5tG cascade A{-2} A{-4}
126TE6tG -------------------------------------------------------------------
126TE7tG 754-666 +0.102 {I10} +0.34 {I3}
126TE8tG -------------------------------------------------------------------
126TE9tG
126TE cG E From 1977Ja04. The evaluators have added 10 eV in
126TE2cG quadrature to the uncertainties of 1977Ja04 to account for
126TE3cG the uncertainty in calibration.
126TE cG RI$From 1998Fo05, unless otherwise noted
126TE cG RI(A)$I|g from 1977Ja04 is normalized to the value of 1998Fo05 at the
126TE2cG strong 666|g
126TE cG M,MR From adopted levels, gammas
126TE cG I(|g{+|+})/I(666|g)=0.0587 {I7} (1977Ja04)
126TE cE IB,IE,TI$From inensity balance at each level except where noted
126TE2cE otherwise.
126TE cE TI(B)$From |SI(|g+ce)(to gs)=33.3% {I4} and %(|e+|b{++})=52.7% {I5}.
126TE cL J Spin and parity values are those given under adopted levels.
126I P 0.0 2- 12.93 D 5 2154 4
126TE N 1.898 0.527 5 1.898
126TE cN BR from X|g coin and 4|p|b|g (1998Fo05).
126TE2cN Other: I(|b{++})/I(|b{+-})=0.028 {I1}; I(406|b{++})/I(1110|b{++})=0.21
126TExcN (1955Ko14)
126TE PN 3
126TE L 0.0 0+
126TE E 0.80 3 18.6 7 9.201 18 19.4 7 B1U
126TES E EAV=529.3 18$CK=0.8179 5$CL=0.11137 8$CM+=0.02953 2
126TE L 666.33812 2+
126TE E 0.196 8 28.7 7 7.448 13 28.9 7
126TES E EAV=216.0 18$CK=0.8494 2$CL=0.11370 4$CM+=0.03007 1
126TE cE IB from |b{++}(666 level)/|b{++}(g.s.)=0.29 {I1} (1955Ko14)
126TE G 666.331 12 32.9 4 E2 0.00378 5
126TES G KC=0.00324 5$LC=0.000430 6$MC=8.59E-5 12
126TE L 1361.3 3 4+
126TE E 0.0002 LE 12.4 GE 0.0002 LE 1U
126TES E CK=0.8382 2$CL=0.1275 1$CM+=0.03434 4
126TE G 695.0 2E-4 APE2 0.00340 5 A ?
126TES G KC=0.00292 4$LC=0.000384 6$MC=7.67E-5 11
126TE L 1420.16616 2+
126TE E 4.46 10 7.625 13 4.46 10
126TES E CK=0.8503$CL=0.11828 5$CM+=0.03145 2
126TE G 753.819 13 4.15 5 M1+E2 -4.25 +15-100.00282 4
126TES G KC=0.00243 4$LC=0.000314 5$MC=6.27E-5 9
126TE G 1420.19 3 0.304 8 E2
126TE cG RI other: 0.293 {I6} (1977Ja04)
126TE L 1873.1 3 0+
126TE E 0.0004614 10.13 14 0.00046 14 1U
126TES E CK=0.7679 22$CL=0.1806 16$CM+=0.0515 6
126TE G 1206.8 3 4.6E-4 13 E2 A
126TE L 2045.11 52+
126TE E 0.0070 4 8.55 5 0.0070 4
126TES E CK=0.768 6$CL=0.180 4$CM+=0.0511 13
126TE G 1378.76 2.37E-316M1+(E2) A
126TE G 2045.09 5 4.6E-3 4E2 A