210BI 210PB B- DECAY 1981HE15,1990SC08,1990HI0314NDS 201408 210BI H TYP=FUL$AUT=M. SHAMSUZZOHA BASUNIA$CIT=NDS 121, 561 (2014)$ 210BI2 H CUT=31-Mar-2014$ 210BI C 1981He15: Measured G-ray energies using HPGe detector. 210BI C 1990Sc08: Measured G-ray and ^X-ray emission probabilities using two 210BI2C Ge(Li) and one Si(Li) detectors. 210BI C 1990HI03: Measured the emission rate of 46.5 keV G ray using 2|p|a 210BI2C spectrometer and HPGe detector (thin beryllium window). 210BI CG Absolute XL intensities measured with a high-purity germanium 210BI2CG detector (1990Sc08). 210BI TG 210BI TG 210BI XL 210BI TG 210BI TG Intensities 210BI2TG energy experimental deduced by 210BI3TG (KEV) (1990Sc08) evaluator#(2003Br13) 210BI4TG -------- ----------- ----------- 210BI5TG 9.42 XLL 0.55 3 0.48 5 210BI6TG 10.80 XLA 9.48 17 9.45 50 210BI7TG 11.68 XLC 0.075 4 0.083 5 210BI8TG 12.6 XLB4+XLB6 2.55 7 2.33 30 210BI9TG 13.0 XLB1+XLB2+XLB15 6.59 33 5.66 27 (XLB1+XLB2) 210BI2TG 13.3 XLB3+XLB5 1.54 9 2.79 40 210BI3TG 13.6 XLB10 0.23 1 210BI4TG 15.2 XLG1 0.682 27 0.75 5 210BI5TG 15.6 XLG2 1.38 4 0.75 12 210BI6TG 16.2 XLG4 0.30 2 210BI7TG 210BI TG $# using theoretical conversion coefficients for a pure M1 46.5G. 210BI CG Others: 1987Me17, 1971Fi04, 1971Ge11, 1969Fr07, 1958Cu91, 210BI6CG 1958To10, 1957Fi06, 1954Da23, 1935St05. See 1967Ha03 for measurements 210BI7CG of L-AUGER electrons with a magnetic spectrometer. 210BI DG CC$FROM BrIcc v2.3a (30-Jun-2013) 2008Ki07, "Frozen Orbitals" appr. 210BI CG MR$IF NO VALUE GIVEN IT WAS ASSUMED MR=1.00 FOR E2/M1, 210BI2CG MR=1.00 FOR E3/M2 AND MR=0.10 FOR THE OTHER MULTIPOLARITIES 210BI CL J,T From Adopted Levels. 210PB P 0.0 0+ 22.20 Y 22 63.5 5 210BI N 1.0 1.0 1.0 210BI PN 3 210BI CN NR$from absolute photon intensity measurements of 1990Sc08 and 210BIxCN 1990Hi03. 210BI L 0.0 1- 5.012 D 5 210BI B 16 3 7.9 1 210BI CB EB=61 (1957To16); EB=61.0 13 (1963Ro31). 210BI CB IB=15 5 (1956St99). Others: 1957To16, 1963Ro31, 1991SaZR, 210BI2CB 1993Am10, 1994Ha63, 1996Gr01, 1996Go47. 210BIS B EAV= 16.16 13 210BI L 46.539 1 0- 3 NS LT 210BI B 84 3 5.4 1 210BI CB EB=17 2 (1955Le29); EB=17.0 5 (1967Ha03). Others: 1952Ba02, 210BI2CB 1952In01, 1953Hu46, 1953Ja02, 1958To10, 1991SaZR, 1993Am10, 1994Ha63, 210BI3CB 1996Gr01, 1996Go47. 210BI CB IB=85 5 (1956St99). 210BIS B EAV= 4.16 13 210BI G 46.539 1 4.25 4 M1 17.86 210BIS G LC=13.64 19$MC=3.21 5 210BIS G NC=0.822 12$OC=0.1678 24$PC=0.0200 3 210BI CG E high-precision GE(LI) measurement of 1981He15, relative to 210BI2CG 53.161 KEV 2 from 133BA and 40.58347 KEV 17 from 99MO (value quoted 210BI3CG by 1980Lu11). Other values: 46.545 KEV 15, GE(LI) (1974HeYW); 210BI4CG 46.503 KEV 15, CE measurement with a magnetic spectrometer (1957Fr29); 210BI5CG 46.52 KEV 2, cryst (1952Ew17). Others: 2000He14. 210BI CG RI weighted average of 4.26 7 (1990Hi03) and 4.24 5 (1990Sc08), 210BI2CG both measurements used high-purity germanium detectors for photons, 210BI3CG and ion chambers for ALPHA particles. Other values: 4.18 9, 210BI4CG high-purity germanium detector (1983De11); 4.05 8, scin (1958Kr71); 210BI5CG 3.8 6 (1954Da23); 4.5 4 (1957Fi06). Others: 1996Ta22, 1996Hu07, 210BI6CG 1995Qu03, 1991Ga09, 1969Fr07, 1958To10, 1953Ba80, 1951Bu37, 1950Cr01, 210BI7CG 1935St05. 210BI CG M from conversion coefficients and sub-shell ratios. 210BI2CG CEL1:CEL2:CEL3 exp=100:10.6 2:0.93 5 (1959Se59); 210BI3CG CEL1:CEL2:CEL3 exp=100:10.3 2:0.87 3 (1969Ge01); 210BI4CG CEM1:CEM2:CEM3:CEM4:CEN1:CEO1 exp=100:10.9:AP 1:AP 0.1:23:5.5 210BI5CG (1957Fr29); ELC=15.6 8 (1958Kr71); ELC=14.3 15, semi (1971Ge11) using 210BI6CG OMEGA(L)=0.38 2 (1957Fi06); ELC=13.3 20 (1957Fi06). Others: 1966Ve01, 210BI7CG 1958To10, 1957Fr29, 1953Wu28, 1953Ba80, 1950Cr01.