58FE 58CO EC DECAY (70.86 D) 10NDS 201004
58FE H TYP=FUL$AUT=CAROLINE D. NESARAJA, SCOTT D. GERAEDTS AND BALRAJ SINGH$
58FE2 H CIT=NDS 111, 897 (2010)$CUT=12-Jan-2010$
58FE c 1992So04: measured p(K)|w(K)=0.313 {I3} in the decay of {+58}Co. This
58FE2c gives the fluorescence yield |w(K)=0.352 {I4} using a calculated
58FE3c value of p(K)=0.889 {I3}
58FE c 1992BeZE: measured electron capture to positron emission ratio in the
58FE2c decay of {+58}Co
58FE c 1991BaZS: evaluation and recommended values by the IAEA coordinated
58FE2c research project on x-ray and |g-ray standards for detector
58FE3c calibration. Recommended values from this evaluation are
58FE4c indicated in comments.
58FE c 2001Kr26: Measured |b|g coin, deduced end-point energy for |b
58FE2c transition to the first excited state
58FE c Measured |g: 1982Gr10, 1979Gr01, 1978He21, 1972DyZY, 1971He20,
58FE2c 1968Ri03, 1956Fr17, 1946Go01
58FE c Measured ce: 1962Fr13, 1962Ma33
58FE c Measured |g|g(|q): 1971Si15, 1969Si13, 1969Sc11, 1966Ra22, 1964Ma09,
58FE2c 1962Ma33, 1956Fr17
58FE c Measured |b{++},|b-shape: 1963Rh02
58FE c Measured |b(|q), |g(|q) from polarized {+58}Co: 1983Le13
58FE c Measured |g(|q,temp or H): 1980Bo33, 1972Fo05, 1962Ma33, 1961Ch12,
58FE2c 1958Da05, 1956Gr52, 1952Da19
58FE c Measured: |b{++}: 1968Ba49, 1966Bi13, 1963Rh02, 1961Ra13, 1958Da03,
58FE2c 1958Ko64, 1955Co31, 1952Ch31, 1944De01
58FE c Measured |b(|q): 1983Le13, 1973An06, 1958Po59, 1957Po35, 1957Am51
58FE c Measured |b|g(|q): 1970Wo07, 1968Sa01
58FE c Measured |b|g(circular polarization)(|q): 1971Pi05, 1968Me21, 1967Be20,
58FE2c 1967Bh04, 1965Co18, 1965Da03, 1965Ma06, 1958Bo90
58FE c |e/|b{++}=5.05 {I9} (1968Ba49), 4.9 {I9} (1961Jo22);
58FE2c |eL(exp)/|eK(exp)=0.110 {I8} (1973Ba67)
58FE D 2007LI49: CALCULATED EC DECAY RATE AS A FUNCTION OF MAGNETIC FIELD
58FE d 2007Li72: calculated neutrino energy loss by |e decay of {+58}Co
58FE c The level scheme is consistent since the total decay
58FE2c energy computed by RADLST is 2307.6 {I29} compared to the Q
58FE3c value of 2307.5 {I12}.
58FE c 1968Ba49: measured |e/|b{++}=5.05 {I9}, I(K x ray).
58FE cE $ The probability for K-shell electron shakeoff =
58FE2cE 16.6|*10{+-4} {I21} (1983Sc09), 13.8|*10{+-4} {I24} (1983Nh01)
58FE cG E$ From 2000He14
58FE cG RI$ I{-K x ray}=26.7 {I3} calculated from this decay scheme; the
58FE2cG same value is given in the 1991BaZS evaluation where I{-Kx|a}
58FE3cG =23.5 {I3} and I{-Kx|b} = 3.2 {I1}.
58FE cG M,MR$ From 'Adopted Gammas'
58FE cL J$ From 'Adopted Levels'
58CO P 0.0 2+ 70.86 D 6 2307.6 12
58CO cP T$ weighted average of 70.75 d {I7} (1982HoZJ), 70.916 d
58CO2cP {I22} (1980Ho17), 70.81 d {I3} (1976Va30), 70.78 d {I4}
58CO3cP (1975La16), 72 d 6 (1973ArZI), 71.1 d {I2} (1972We17), 70.8 d
58CO4cP {I9} (1972Cr02), 70.4 d {I10} (1972Cr02), 71.5 d {I8} (1968De08).
58CO5cP Older measurements: 1956Sc87, 1955Co31, 1952Ru23, 1952Ho58, 1941Li01
58FE N 0.9945 1 1 1
58FE CN NR$ I{-|g+ce}(811)+I{-|g+ce}(1674)=100
58FE PN 3
58FE L 0.0 0+
58FE E 0.00063 0.00012 12.8 0.00075
58FES E EAV=553.12 54$CK=0.1473 4$CL=0.01566 4$CM+=0.002735 7
58FE cE IB from 1958Da03
58FE L 810.7666 20 2+ 1 NS LT
58FE cL T from 1964Ma09
58FE E 1496 5 14.9 2 83.9 2 6.61 1 98.8 2
58FES E EAV=201.10 51$CK=0.7546 11$CL=0.08046 11$CM+=0.014062 20
58FE cE E$ from E(|b{++})=474 {I5} (1963Rh02). Others: 471 {I8} (2001Kr26),
58FE2cE 472 {I6} (1952Ch31)
58FE cE IB calculated from I(|g+ce) and |e/|b{++}=5.61 {I8} from
58FE2cE LOGFT code; measured values include:
58FE3cE 14.96 {I18} (1968Ba49), 15.2 {I2} (1966Bi13)
58FE4cE |e/|b{++}=5.65 {I11} (1992BeZE), 5.76 {I6} (1970Wi14), 5.82 {I10}
58FE5cE (1962Kr02), |eK(exp)/|b{++}=4.85 {I9} (1992BeZE), 4.94 {I8}
58FE6cE (1970Bi02), 5.05 {I5} (1968Ba49) 4.83 {I10} (1962Kr02), 4.92 {I9}
58FE7cE (1961Jo22); |eL(exp)/|eK(exp)=0.108 {I4} (1963Mo12)
58FE G 810.7593 20 100 E2 3.32E-4
58FES G KC=0.000299
58FE cG M |a(K)exp=3.0|*10{+-4} {I1}, K/(L+M)=8 {I1}, |a=3.4|*10{+-4}
58FE2cG {I1} (1962Fr13). Other: K/L=11.8 (1962Ma33)
58FE L 1674.736 5 2+
58FE E 1.21 2 7.69 1 1.21 2
58FES E CK=0.8875$CL=0.09573$CM+=0.01675
58FE G 863.951 6 0.69 1 M1+E2 -0.69 5 2.33E-4 4
58FES G KC=0.000210
58FE cG RI from weighted average of 0.77 {I4} (Hill, report
58FE2cG BNWL-SA-315, 1965), 0.81 {I3} (1968Ri03), 0.70 {I2} (1972DyZY),
58FE3cG 0.645 {I15} (1973Ba67), 0.69 {I2} (Denecke as quoted in
58FE4cG 1973Ba67), 0.69 {I2} [Legrand et al., Atomic Energy Review 11
58FE5cG (1973) 524], 0.74 {I4} (1974HeYW), and 0.682 {I17} (1982Gr10).
58FE6cG The internal uncertainty is 0.008, the reduced-|h{+2} is 4.4,
58FE7cG and the external uncertainty 0.016.
58FE cG M |a(K)exp=0.00024 {I4} (1962Ma33)
58FE cG MR from |g|g(|q) and |g(|q,t) (1972Fo05)
58FE G 1674.725 7 0.52 1 E2
58FE cG RI from weighted average of 0.68 {I5} (Hill, report
58FE2cG BNWL-SA-315, 1965), 0.57 {I3} (1968Ri03), 0.49 {I3} (1972DyZY),
58FE3cG 0.506 {I15} (1973Ba67), 0.527 {I15}
58FE4cG (Denecke as quoted in 1973Ba67), 0.525 {I13} [Legrand et al.,
58FE5cG Atomic Energy Review 11, 524 (1973)], 0.54 {I4} (1974HeYW), and
58FE6cG 0.511 {I15} (1982Gr10). The internal uncertainty is 0.007, the
58FE7cG reduced |h{+2} is 2.2, and the external uncertainty 0.01.
58FE DG $ 1969DYZX SUPERSEDED BY 1972DYZY