Nuclear Data Sheets for A=60
References for A=60 (251)
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Cited by (28)
A comparison between neutron-fluence measurements using metal-activation monitors and standard glasses calibrated via thin uranium-fission monitors and via ηq method
2013, Radiation MeasurementsCitation Excerpt :The results can be seen in Figs. 4–7. The constant values used for fluence calculations with Equation (1) through (3) were: (NUε)CN5 = (4.17 ± 0.15) × 1013 cm-2 (Iunes et al., 2002); Θ235 = 0.00720 (Steiger and Jäger, 1977); σ235 = 580 b (Holden and Holden, 1989); g235 = 1 (Holden, 1999); AU = 238; [2R]un/[2R]ed = 1.142 (Enkelmann et al., 2005); ged = 0.5; Gth = 0.998 (CN-5; Bellemans et al., 1995), 0.997 (IRMM; De Corte et al., 1998); NA = 6.022 × 1023 mol−1; [U] = (15.0 ± 0.9) μg/g (IRMM540R; IRMM official certification), (12.2 ± 0.6) μg/g (CN5; Bellemans et al., 1995), (49.4 ± 2.7) μg/g (IRMM541; IRMM official certification); d = 2.45 g/cm3(CN-5; IRMM); γ = 95.56% (411.8 keV; Hoppes and Schima, 1982), 99.88% (1173.2 keV), 99.982% (1332.5 keV) (Andersson et al., 1986); Mx = 58.9332 g mol-1(59Co), 196.96654 g mol-1 (197Au)(De Corte et al., 1998); Θmetal = 100% (59Co), 100% (197Au); σmetal = 37.13 b (59Co), 98.65 b (197Au) (Holden and Holden, 1989); λmetal = 4.170 × 10−9 s−1 (60Co; Andersson et al., 1986), 2.976 × 10−6 s−1 (198Au; Hoppes and Schima, 1982). The names presented on the x-axis (Monitors) from Figs. 4–7 are metal monitors (Co, Au) or uranium doped glasses: 540R = IRMM540R; CN5 = CN5; 541 = IRMM541.
Reduced electric-octupole transition probabilities, B(E3;0<inf>1</inf><sup>+</sup> → 3<inf>1</inf><sup>-</sup>) - An update
2002, Atomic Data and Nuclear Data TablesHPGe detector efficiency calibration for extended sources in the 50-1400 keV energy range
1993, Applied Radiation and IsotopesFusion of <sup>59</sup>Co with light projectiles at near barrier energies
1991, Nuclear Physics, Section A