13C 13N EC DECAY 24NDS 202410
13C H TYP=FUL$AUT=J.H. Kelley, C.G. Sheu and J. E. Purcell$
13C 2 H CIT=NDS 198, 1 (2024)$CUT=1-Aug-2024$
13C c
13C c 1935Ru01: {+13}N(|b{++}); {+10}B(|a,n) was used to produce {+13}N,
13C 2c which was found to decay with T{-1/2}|?14 minutes.
13C c 1939Wa09: measured T{-1/2}=9.93 min {I3}
13C c 1948Co24: {+13}N(|b{++}); measured T{-1/2}=10.2 min {I1}
13C c 1950Ho01: {+13}N(|b{++}); measured end-point energy
13C 2c E{-|b}(max)=1.202 MeV {I5} and T{-1/2}=10.05 min {I10}.
13C c 1953Ch34: {+13}N(|b{++}); measured
13C 2c T{-1/2}=602.9 sec {I19}=10.05 min {I3}.
13C c 1954Gr66: {+13}N(|b{++}); measured E{-|b}(max)=1.185 MeV {I25}.
13C c 1955Wi43: {+13}N; measured T{-1/2}=10.08 min {I4}.
13C c 1957Da08: {+13}N(|b{++}); measured T{-1/2}=9.96 min {I3}.
13C c 1957De22: {+13}N(|b{++}); measured T{-1/2}=10.02 min {I10}.
13C c 1957No17: {+13}N(|b{++}); measured T{-1/2}=10.07 min {I6}.
13C c 1958Ar15: {+13}N(|b{++}); measured T{-1/2}=9.96 min {I3}.
13C c 1958Da09: {+13}N(|b{++}); measured E{-|b}(max)=1.190 MeV {I3} and
13C 2c T{-1/2} as in (1957Da08).
13C c 1960Ja12: {+13}N(|b{++}); measured T{-1/2}=9.9965 min {I5}
13C c 1960Ki02: {+13}N(|b{++}); measured T{-1/2}=9.93 min {I5}
13C c 1961Ra06: {+13}N(|b{++}); measured T{-1/2}=12.3 min {I7} (excluded)
13C c 1965Bo42: {+13}N(|b{++}); measured T{-1/2}=10.05 min {I5}
13C c 1965Eb01: {+13}N(|b{++}); measured T{-1/2}=9.96 min {I2}
13C c 1968Ri15: {+13}N(|b{++}); measured T{-1/2}=9.963 min {I9}
13C c 1971Go40: {+13}N(|b{++}); for decay to {+13}C{-g.s.},
13C 2c log{Ift}=3.667 {I1}.
13C c 1973SiYS: {+13}N(|b{++}); measured T{-1/2}=10.0 min {I5}
13C c 1977Az01: {+13}N(|b{++}); measured T{-1/2}=9.965 min {I10}
13C c 1980An40: {+13}N(|b{++}); measured T{-1/2}=9.967 min {I10}
13C c 1989KaYR: {+13}N(|b{++});
13C 2c measured T{-1/2}=9.962 min {I20}
13C c 2022Lo14: {+13}N(|b{++}); measured T{-1/2}=9.9508 min {I32};
13C 2c provided an analysis using only their value and
13C 3c (1968Ri15,1977Az01) and recommended T{-1/2}=9.9532 min {I37}
13C c 1995Va27: {+13}N(|b{++}); measured |b asymmetry following beam
13C 2c implantation in Pt; deduced beam polarization.
13C c
13C c {ITheory}:
13C c 1970Ko41: general model for |b decay in even-odd nuclei.
13C c 1970Da21: generalized pairing-force model analysis of log {Ift} values
13C c 1972Ma72: calculated |b shape spectra
13C c 1973Wi04: analysis of the Axial-Vector coupling constant
13C c 1973Su04: analysis of K-electron capture branching ratios
13C c 1975Kr14: developed O(5) symmetry model to analyzed log {Ift} values.
13C c 1977Ri08: Shell model analysis of log {Ift} values.
13C c 1980An31: analysis of K-electron capture rates
13C c 1984Ko40: analyzed isotensor component in isovectorial transition.
13C c 1991Na05: analyzed mirror nuclei decays
13C 2c in a search for evidence of right-handed currents.
13C c 1995Go34: analyzed |b-decay polarization asymmetry data
13C 2c in a search for evidence of right-handed chirality.
13C c 2008Se10: analyzed half-lives, branching ratios,
13C 2c electron-capture probabilities; deduced {Ift} values in mirror decays.
13C c 2008Pe13: analyzed correlations between
13C 2c |b decays in mirror nuclei and their magnetic moments.
13C c 2012Sa50: analysis of isospin related
13C 2c corrections for superallowed |b transitions.
13C c 2015Mo10, 2010MoZU: calculated improved beta
13C 2c spectra, shape factors, mean energies, experimental mean energies.
13C c 2015To02: developed parametrization of the
13C 2c statistical rate functions, {If}, for superallowed T=1/2 transitions.
13C c 2021Ir01: single-particle model analysis of
13C 2c the {+13}N(|b{++}) reaction. Emphasized asymptotic normalization
13C 3c coefficients (ANCs) and spectroscopic factor data.
13C c 2021Da11: analyzed the role of tensor forces in |b decay.
13C c 2024Fa01: analyzed decay between isobaric analog mirror states.
13C N 1 1 1
13C DE LOGFT,CK,CL,CM,CN$FROM BetaShape v2.4 (Jun-2024) 2019MO35.
13C DE EAV,LOGFT$FROM BetaShape v2.4 (Jun-2024) 2023MO21.
13N P 0 1/2- 9.9584 M 36 2220.47 27
13N cP T$From Adopted Levels of {+13}N
13N cP QP$From (2021Wa16)
13C L 0 1/2- STABLE
13C E 99.803 50.197 53.67174 44 100
13C S E EAV=492.21 12$CK=0.00182 5$CL=1.466E-4 42
13C cE $C1=0.001 {I24} (1958DA09)
13C cE $Cexp(W) = 1+C{-1}W