Recommended value (August, 2015): | 70.617 ± 0.020 s | |||
Summary Table of Uncertainty Analysis: | (PDF); | Summary Chart of All Values: | (PDF) | |
Measured values: | 70.696 ± 0.052 s | (2006BU12) | ||
70.641 ± 0.020 s | (2004BA78) | |||
70.560 ± 0.049 s | (2001GA59) | |||
70.684 ± 0.077 s | (1978BE61) | |||
70.613 ± 0.025 s | (1978WI04) | |||
70.43 ± 0.18 s | (1974AZ01) | |||
70.588 ± 0.028 s | (1973CL12, 1971CL07) | |||
70.48 ± 0.15 s | (1972AL01) | |||
70.32 ± 0.12 s | (1972SI50) | |||
71.3 ± 0.1 s | (1963FR10) (Excluded) | |||
71.00 ± 0.13 s | (1962BA26) (Excluded) | |||
70.91 ± 0.04 s | (1961HE03) (Excluded) | |||
72.1 ± 0.4 s | (1954GE38) (Excluded) | |||
Other Reviews: | 70.620 ± 0.015 s | (2009HA12) | ||
70.599 ± 0.022 s | (1975HA45) |
Decay to 14N* (MeV) |
Jπ | Eβ+(max) (keV) | Branching Ratio (%) | ft (sec) | |||
---|---|---|---|---|---|---|---|
0 | 1+ | (1954GE38, 1955SH84) | 4145 ± 20 | (1954GE38, 1955SH84) | 0.60 ± 0.10 | (1954GE38, 1955SH84) | (2.0 ± 0.3) x 107 |
(1962BA26) | 4124 ± 2 | (1963FR10, 1965FR09) | 0.65 ± 0.05 | (1963FR10, 1965FR09) | (1.7 ± 0.2) x 107 | ||
(1963FR10, 1965FR09) | 4085 ± 30 | (1965KAZX, 1966SI05) | 0.61 ± 0.01 | (1965KAZX, 1966SI05) | (2.14 ± 0.03) x 107 | ||
(1969KA1B) | (1.9 ± 0.2) x 107 | ||||||
(1980WI13) | 7.266 ± 0.009 h | ||||||
2.31 | 0+ | (1954GE38, 1955SH84) | 1835 ± 8 | (1954GE38, 1955SH84) | 99.4 ± 0.1 | (1954GE38, 1955SH84) | 3725 ± 75 |
(1954PE1B) | 1830 ± 30 | (1963FR10, 1965FR09) | 99.35 ± 0.05 | (1957BR18) | 3088 ± 56 | ||
(1961BU04) | 1809.7 ± 1.5 | a | 99.328 ± 0.012 | (1961HE03) | 3061 ± 10 | ||
(1962BA26) | 1812.6 ± 1.4 b | c | 99.332 ± 0.011 | (1961BU04) | 3057 ± 20 | ||
(1963FR10, 1965FR09) | 1821 ± 7 | d | 99.336 ± 0.010 | (1962BA26) | 3074 ± 10 e | ||
(1963FR10, 1965FR09) | 3137 ± 70 | ||||||
(1969KA1B) | 3076 ± 7 | ||||||
(1975HA45) | 3084.3 ± 3.6 | ||||||
(1978WI04) | 3086.5 ± 2.7 | ||||||
(1981WH03) | 3084.4 ± 1.1 f | ||||||
3.95 | 1+ | (1965KAZX, 1966SI05) | 0.062 ± 0.007 g | (1965KAZX, 1966SI05) | 1200 ± 150 g | ||
(1980WI13) | 0.0577 ± 0.0043 | (1980WI13) | 3.112 ± 0.034 h | ||||
(1981HE19) | 0.0528 ± 0.0023 | (1981HE19) | 1446 ± 63 |
a) Obtained by adopting 0.61 ± 0.01 % (1966SI05) and 0.062 ± 0.007 % (1969KA1B) for the branching ratio to 14N*(0, 3.95) [both 1+; 0 states]. Sum of εK and β-decay in ratio 6/4 (R.W. Kavanagh, private communication to Fay Ajzenberg-Selove, (1981AJ01) |
b) 1890.1 ± 1.5 keV is obtained from measurements of the threshold energy of the 14N(p, n)14O reaction and the energy of 14N*(2.31). This value leads to a 0.8% decrease in the ft value of (1962BA26) (1968FR08). |
c) Obtained by adopting 0.61 ± 0.01 % (1966SI05) and 0.058 ± 0.004 % (1980WI1H) for the branching ratio to 14N*(0, 3.95) [both 1+; 0 states]. |
d) Obtained by adopting 0.61 ± 0.01 % (1966SI05) and 0.054 ± 0.002 % (weighted mean of (1980WI13 and 1981HE19) for the branching ratio to 14N*(0, 3.95) [both 1+; 0 states]. |
e) Using τ(partial) = [71.36 ± 0.009] sec; includes form-factor and screening corrections. Radiative corrections of (1959KI1C) increase ft to 3126 sec: see also (1966BA1A, 1966FR15, 1967SU1E). |
f) This is the fRt value. |
g) And private communication: 0.025 β+ (1969KA1B). |
h) This is the log ft value. |
Back to Ground-State Decays Data Main Page
Last modified: 14 August 2017