111CD 111IN EC DECAY 09NDS 200905
111CD H TYP=FUL$AUT=Jean Blachot$CIT=NDS 110, 1239 (2009)$CUT=1-Feb-2008$
111CD c 1999BeZS: evaluation by V. P. Chechev, April 1998 including some
111CD2c general comments from previous evaluation (1996Bl12).
111CD3c This evaluation was done as part of a collaboration of evaluators
111CD4c from Laboratoire National Henri Becquerel (LNHB) in France;
111CD5c Physikalisch-Technische Bundesanstalt (PTB) in Germany; HMS
111CD6c Sultan and AEA Technology in the United Kingdom; Khlopin Radium
111CD7c Institute (KRI) in Russia; Centro de Investigaciones
111CD8c Energeticas, Medioambientales, y Tecnologicas (CIEMAT) and
111CD9c Universidad Nacional a Distancia (UNED) in Spain; and Brookhaven
111CD0c National Laboratory (BNL), Lawrence Berkeley National Laboratory
111CDAc (LBNL), and Idaho National Engineering and Environmental
111CDBc Laboratory (INEEL) in the United States.
111CD c Other reference: 1968Da24
111CD cE Limits on the |e branches to the levels at 0 and 245 keV
111CD2cE can be deduced from the log {Ift} systematics of 1998Si17. The
111CD3cE transitions to these levels are 4{+th} and 2{+nd} forbidden with
111CD4cE expected log {Ift}'s of >22 and >10.6, respectively. The
111CD5cE corresponding I{-|e} limits are <1.0x10{+-14}% and <5x10{+-4}%,
111CD5cE respectively.
111CD cG E From weighted average of values from 1951Mc61, 1966Sp04,
111CD2cG 1974HeYW, and 1975Sh29, except 150-keV |g which is from 1975Sh29.
111IN P 0.0 9/2+ 2.8047 D 4 862 5
111CD N 1.00 1 1.0 1.0
111CD PN 2
111CD L 0.0 1/2+ STABLE
111CD L 245.35 4 5/2+ 84.5 NS 4
111CD cL T from {+111}Cd Adopted Levels.
111CD G 245.35 4 94.09 18 E2 0.0628 C
111CD2 G EKC=0.0525 12$ EKC=0.0494 11 (1966SP04)$ EKC=0.054 5 (1951MC61)
111CDS G KC= 0.0526 $ LC=0.0083 $ MC=0.0016 $NC+=0.00032
111CD cG RI from 100.0/[1.0 + |a(245)] = 100.0 / 1.0628 {I19} where
111CD2cG an uncertainty of 3% has been assigned to |a(245).
111CD cG M from K:L1:L2:L3:M=100 {I1}:10.2 {I2}:2.30 {I15}:2.21
111CD2cG {I15}:2.73 {I10} (1966Sp04), 100/11.5 {I16}/2.06 {I25}/1.9
111CD3cG {I3}/2.7 {I4} (1975Sh29)
111CD L 396.16 5 11/2- 48.50 M 9 M1
111CD cL T from {+111}Cd Adopted Levels
111CD E 0.005 5 9.0 GE
111CDS E CK= 0.8522 15 $ CL= 0.1181 11 $ CM+= 0.0298 6
111CD cE IE from < 0.01 from 1972MeZD; other: |? 0.01 from I{-|g}(150)
111CD2cE = 0.003 and |a(150) = 2.30.
111CD cE CK,CL computed from tables of 1998Sc28
111CD G 150.81 3 0.003 AP E3 2.31
111CDS G KC= 1.45 $ LC= 0.69 $ MC= 0.138 $ NC+= 0.0259
111CD cG RI from 1975Sh29; other: 0.0028 deduced from %|e=0.0086
111CD2cG (1972MeZD) and < 0.003 from limit of 1972MeZD
111CD cG M from {+111}Cd IT decay (48.50 min)
111CD L 416.63 5 7/2+ 0.12 NS 3
111CD cL T from (ce(K) Auger)(ce(L) 171|g)-coin (1964Sp07)
111CD E 100.000 5 5.02
111CDS E CK= 0.8516 15 $ CL= 0.1186 11 $ CM+= 0.021 5
111CD cE E |eK/|e exp=0.867 {I7} (1966Sp05) via (ce(K) Auger)(ce(K)
111CD2cE 245|g)-coin
111CD cE CK,CL computed from tables of 1998Sc28
111CD G 171.28 3 90.65 25 M1+E2 -0.144 3 0.103 C
111CD2 G EKC=0.0868 25 (1966SP04)
111CDS G KC=0.089 $ LC=0.011 $ MC=0.0021 $NC+=0.00047
111CD cG RI from I{-|g} = [100.0 - I{-|b}(396)] / [1.0 + |a(171)] =
111CD2cG 99.995 {I5} / 1.103 {I3}
111CD cG MR average of -0.146 {I3} (1956St64) |g|g(|q), -0.141 {I3}
111CD2cG (1973Bu31) |g|g(|q); 0.145 (1974Kr03) |g|g(|q, linear pol) sign
111CD3cG inconsistent. |d=0.196 {I+46-55} from L3/L1=0.042 {I12}
111CD4cG (1966Sp04,1975Sh29). Penetration effects may account for exp
111CD5cG L1/L2/L3 ratios (1966Sp04,1975Sh29); incompatible with predictions
111CD cG M other |a(K)exp: 0.110 {I5} (1975Sh29), 0.10 {I1} (1951Mc61)
111CD2cG normalized to |a(K)(245|g)=0.0536 (E2 theory)