211BI 211PB B- DECAY 13NDS 201306
211BI H TYP=FUL$AUT=E.A. McCutchan, C.M. Baglin, O. Gorbachenko, N. Todorovic$
211BI2 H CIT=NDS 114, 661 (2013)$CUT=28-FEB-2013$
211BI cB IB Calculated from I(|g+ce) imbalance at each level.
211BI tG $The data presented include information from the following references:
211BI2tG E|g,I|g: 1988Hi14, 1976Bl13, 1971Da34, 1968Br17, 1968Go15, 1968Ha21
211BI+tG ,
211BI+tG 1967Da10,
211BI+tG 1967Da20, 1965Me07
211BI3tG |a: 1971Ra30, 1968Go15, 1965Br35, 1965Co06, 1965Me07, 1963Va05, 193
211BI+tG 8Ch04
211BI4tG |g|g,sum |g|g: 1971Da34, 1968Go15, 1968Ha21, 1967Da10, 1965Me07, 19
211BI+tG 63Va
211BI+tG 05
211BI5tG |g|g(|q),|g|g(|q,pol): 1968Da07, 1968Go15, 1965Ag03, 1965Co06, 19
211BI+tG 1964Uh01,
211BI+tG 1963Va05
211BI6tG |g|g(t): 1966Go19
211BI7tG |b{+-}: 1967Sc39, 1965Co06, 1963Va05
211BI8tG |b|g: 1967Sc39
211BI9tG |b|g(t): 1963Va05
211BIAtG |b|g(|q): 1971Ra30
211BIBtG
211BI cG Others: 1967CaZY, 1962Gi03.
211BI cG All ce intensities have been measured relative to
211BI2cG I(ce(K) 351.06|g). The evaluator has renormalized all Ice to give
211BI3cG |a(K)(351.06|g, {+207}Tl)=0.199. The |a(exp) quoted are the weighted
211BI4cG averages of all measured and renormalized Ice divided by adopted I|g.
211BI tG K|a{-1}| x ray(Tl)/K|a{-1}| x ray(Bi)=3.12 {I4} (1971Da34).
211BI tG K|a{-1}| x ray(Tl)/I(65.420|g)=15.5 {I2} (1971Da34).
211BI tG I(65.402|g)/x-ray(Tl)=0.029 {I10} (1965Me07).
211BI cG E From 1976Bl13, unless otherwise noted. The energies quoted by
211BI2cG 1976Bl13 have been adjusted by the evaluator for a change in
211BI3cG calibration energies (compare 1979He19). The change is +10 eV for 300
211BI4cG 600 keV.
211BI cG RI Weighted average of measurements by 1988Hi14, 1976Bl13,
211BI2cG 1971Da34, 1968Br17, 1968Go15, 1968Ha21, 1967Da10, 1967Da20, and
211BI3cG 1965Me07, unless otherwise noted.
211BI cG MR If |d is given without a sign, then the sign of |d is not
211BI2cG known.
211BI cG E(B),RI(B,F)$From 1971Da34.
211BI cG E(C,E),RI(C)$From 1988Hi14.
211BI cG E(D),RI(D)$From 1968Ha21.
211BI cL The decay scheme is that proposed by 1965Me07 with
211BI2cL modifications from 1967Da10, 1968Ha21, and 1971Da34.
211BI cL E From least-squares fit to E|g, excluding the 677|g which fits
211BI2cL its placement poorly; this results in a reduced |h{+2} of 4.2
211BI3cL compared with a critical value of 2.25 and a value of 25.9 when all
211BI4cL E|g data are included.
211BI cL J,T From Adopted Levels.
211PB P 0.0 9/2+ 36.1 M 2 1367 6
211BI N 0.1291 11 1.0 1.0
211BI PN 3
211BI cN NR from (0.99724 {I4})|*(0.1295 {I11})=0.1291 {I11}; where
211BI2cN {+211}Bi |a decay branching=99.724% {I4} and
211BI3cN I(351.06|g,{+207}Tl)=12.95% {I11} of {+211}Bi |a decay. All
211BI4cN I|g({+211}Pb) have been measured relative to I(351.06|g in
211BI5cN {+207}Tl)=100 in sources where {+211}Pb is in equilibrium with its
211BIxcN daughter, {+211}Bi.
211BI cN BR 100%.
211BI G 81.0 2 0.35 9 B
211BI G 83.8 1 0.45 7 B
211BI G 88.2 2 0.13 3 B
211BI G 94.3 3 0.09 2 B
211BI G 97.3 2 0.09 1 B
211BI G 244 0.3 1 D
211BI G 478.0 4 0.10 2 B
211BI G 479.62 20 0.04 1 C
211BI G 481.1 4 0.20 4 B
211BI G 481.92 12 0.08 1 C
211BI G 491.82 12 0.032 6 C
211BI G 494.2 3 0.013 5 C
211BI G 500.4 5 0.09 2 B
211BI G 502.0 2 0.028 6 C
211BI G 1090.5 5 0.020 5 B
211BI L 0.0 9/2- 2.14 M 2
211BI B 91.32 12 5.990 8
211BIS B EAV=471.3 24
211BI cB E E|b=1378 {I8}, from F-K analysis (1965Co06). Other: 1355
211BI2cB {I25} (1963Va05).
211BI cB IB from I(|g+ce) imbalance at {+211}Bi g.s. Others (from F-K
211BI2cB analysis): 93 {I2} (1965Co06), 92.4 {I15} (1963Va05).
211BI L 404.866 9 7/2- 0.317 NS 12
211BI2 L G=1.27 20
211BI cL J |g|g(|q), |g|g(pol) establish J=7/2 (1968Da07,1968Go15)
211BI cL T weighted average of 0.318 ns {I14} (|g|g(t) 1966Go19) and
211BI2cL 0.315 ns {I20} (|b|g(t) 1963Va05).
211BI cL G from |g|g(|q,h) (liquid source, H=18.3 kG and T{-1/2}=0.317
211BI2cL ns {I11}, 1965Ag03).
211BI B 1.63 9 7.19 3
211BIS B EAV=313.7 23
211BI cB E,IB E|b=951 {I25}, I|b=1.4 {I5} from F-K analysis of
211BI2cB |b(404|g+427|g) (1963Va05).
211BI G 404.853 10 29.3 4 M1+E2 -1.1 1 0.122 8
211BIS G KC=0.095 7$LC=0.0206 8$MC=0.00498 17$NC+=0.00156 6
211BIS G NC=0.00127 5$OC=0.000254 10$PC=2.79E-5 13
211BI cG M $from ce data. |a(K)exp=0.099 {I5} (average of renormalized
211BI2cG measurements of 1971Ra30,1968Go15,1965Co06,1965Me07,1963Va05);
211BI3cG L1/L2=2.1 (1965Br35); K/L=4 {I1} (1965Co06) (theory: L1/L2=3.12
211BIxcG {I27},K/L=4.6 {I4})
211BI cG MR from -1.15 (|g|g(|q,pol) 1968Go15) and 0.98 {I+8-7} (from
211BIxcG |a(K)exp).
211BI L 766.539 16 (9/2,11/2)-
211BI G 362.072 17 0.33 2 C ?
211BIL G FL=404.866
211BI cG E a 361-keV |g was deduced from |g|g data (1968Ha21).
211BI cG RI from 1976Bl13.
211BI G 766.51 3 4.78 12 M1 0.0382
211BIS G KC=0.0313 5$LC=0.00527 8$MC=0.001234 18$NC+=0.000388 6
211BIS G NC=0.000316 5$OC=6.45E-5 9$PC=7.71E-6 11
211BI cG M from |a(K)exp=0.041 {I5} (weighted average of renormalized
211BI2cG values of 1968Go15 and 1965Me07).
211BI L 831.960 12 9/2- 90 PS LT
211BI cL J |g|g(|q) establishes J=9/2.
211BI cL T from |b|g(t) (1963Va05).
211BI B 6.28 10 5.7330 18
211BIS B EAV=160.2 21
211BI cB E,IB E|b=525 {I25}, I|b=5.5 {I8} from F-K analysis of |b(830|g)
211BIxcB (1963Va05).
211BI G 65.420 14 0.60 4 M1 6.58 F
211BIS G LC=5.02 7$MC=1.182 17$NC+=0.372 6
211BIS G NC=0.302 5$OC=0.0618 9$PC=0.00735 11
211BI cG M from L1/L2=6.8 (1965Br35), 10 (1938Ch04); |a(L)exp=7.2
211BI2cG (Ice(L)(1938Ch04)/I|g). (theory: L1/L2=9.39 {I20})
211BI G 427.088 10 13.6 3 M1+E2 -0.022 9 0.1784 C
211BIS G KC=0.1457 21$LC=0.0250 4$MC=0.00586 9$NC+=0.00184 3
211BIS G NC=0.001497 21$OC=0.000306 5$PC=3.65E-5 6
211BI cG M from |a(K)exp=0.143 {I17} (weighted average of renormalized
211BI2cG values of 1968Go15,1965Co06,1965Me07,1963Va05); K/L=7 {I2} (1965Co06);
211BI3cG L1/L2=5.0 (1965Br35). (theory: K/L=5.84 {I12}, L1/L2=9.78 {I23})
211BI cG MR from |g|g(|q): 9/2(427|g)7/2(405|g)9/2 cascade with
211BI2cG |d(405|g)=-1.1 {I1} and A{-2}=-0.094 {I6} (weighted average of
211BI3cG measurements by 1968Da07,1968Go15,1965Co06,1964Uh01,1963Va05).
211BI4cG Other: 0.17 {I15} |g|g(|q,pol) (1968Go15).
211BI G 832.01 3 27.3 4 M1+E2 0.39 +18-250.0281 24
211BIS G KC=0.0230 20$LC=0.0039 3$MC=0.00092 7$NC+=0.000288 22
211BIS G NC=0.000235 18$OC=4.8E-5 4$PC=5.7E-6 5
211BI cG M,MR from |a(K)exp=0.023 {I2} (weighted average of renormalized
211BI2cG values of 1968Go15,1965Me07,1963Va05).
211BI L 951 ?
211BI B 0.022 13 7.8 3 ?
211BIS B EAV=120.7 20
211BI G 546 C ?
211BI cG E |g not observed; existence deduced from |g|g data (1968Ha21).
211BI G 951 0.17 10 ?
211BI cG E,RI$from 1968Ha21, not observed by other investigators.
211BI L 1014.40 4 7/2-,9/2-,11/2-
211BI G 609.38 4 0.33 5
211BI G 1014.64 5 0.134 4
211BI L 1080.15 5
211BI B 0.056 6 6.90 6
211BIS B EAV=80.2 19
211BI G 313.59 9 0.24 3 F
211BIL G FL=766.539
211BI G 676.69 7 0.10 3
211BI2 G FL=404.866
211BI cG E fits poorly; E|g excluded from least-squares fit.
211BI G 1080.16 6 0.095 5
211BI2 G FL=0.0
211BI L 1103.5 2
211BI B 0.0046 7 7.87 8
211BIS B EAV=73.1 18
211BI G 1103.52 20 0.036 5 E
211BI L 1109.485 23 9/2-
211BI B 0.83 4 5.58 4
211BIS B EAV=71.3 18
211BI G 95.0 2 0.14 2 M1+E2 1.6 +5-3 9.4 4 BC
211BIS G KC=3.0 9$LC=4.8 5$MC=1.25 12$NC+=0.38 4
211BIS G NC=0.32 3$OC=0.059 6$PC=0.0048 4
211BI cG M,MR from |a(K)exp=2.8 {I9} (K| x ray/|g in |g|g, 1965Me07).
211BI G 342.91 4 0.27 4 [M1,E2] 0.20 12 F
211BIS G KC=0.16 11$LC=0.035 11$MC=0.0085 22$NC+=0.0027 7
211BIS G NC=0.0022 6$OC=0.00043 13$PC=4.7E-5 20
211BI G 704.64 3 3.58 8 M1+E2 -0.022 7 0.0476
211BIS G KC=0.0390 6$LC=0.00657 10$MC=0.001540 22$NC+=0.000484 7
211BIS G NC=0.000394 6$OC=8.05E-5 12$PC=9.61E-6 14
211BI cG M from |a(K)exp=0.036 {I5} (weighted average of renormalized
211BI2cG values of 1968Go15 and 1963Va05); |g|g(|q).
211BI cG MR $from |g|g(|q): 9/2(705|g)7/2(405|g)9/2 cascade with
211BI2cG |d(405|g)=-1.1 {I1} and A{-2}=-0.094 {I4} (weighted average of
211BI3cG measurements by 1968Da07,1968Go15,1965Ag03,1965Co06,1963Va05); |d=0.4
211BIxcG {I+3-4} from |a(K)exp.
211BI G 1109.48 5 0.89 3
211BI L 1196.33 5
211BI B 0.017 3 6.71 9
211BIS B EAV=45.9 18
211BI G 430 1 0.05 2 B
211BI G 1196.33 5 0.079 3
211BI L 1234.3 4
211BI B 0.0013 3 7.49 12
211BIS B EAV=35.3 17
211BI G 1234.3 4 0.010 2 B
211BI L 1270.72 6 (7/2,9/2,11/2)
211BI B 0.0186 11 5.91 9
211BIS B EAV=25.3 17
211BI G 504.12 12 0.045 6 C
211BI G 865.93 14 0.046 3 C
211BI G 1270.71 8 0.053 4