References quoted in the XUNDL dataset: 14N 14O B+ DECAY:XUNDL-7

9 references found.

Clicking on a keynumber will list datasets that reference the given article.


1955SH84

Phys.Rev. 100, 945 (1955)

R.Sherr, J.B.Gerhart, H.Horie, W.F.Hornyak

Decay Rates of C14, N14*, and O14

doi: 10.1103/PhysRev.100.945


1963FR10

Phys.Rev. 132, 2169 (1963)

G.Frick, A.Gallmann, D.E.Alburger, D.H.Wilkinson, J.P.Coffin

Positron Radioactivities of O14, Ne18, Si26, S30

NUCLEAR STRUCTURE 26Si, 14O, 18Ne, 30S; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.132.2169


1966SI05

Phys.Rev. 148, 1024 (1966)

G.S.Sidhu, J.B.Gerhart

Observation of the 4.12-MeV O14 A N14 Positron Spectrum Shape

NUCLEAR STRUCTURE 14O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.148.1024


2005HA27

Phys.Rev. C 71, 055501 (2005)

J.C.Hardy, I.S.Towner

Superallowed 0+ → 0+ nuclear β decays: A critical survey with tests of the conserved vector current hypothesis and the standard model

RADIOACTIVITY 10C, 14O, 18Ne, 22Mg, 26Si, 30S, 34Ar, 38Ca, 42Ti, 26mAl, 34Cl, 38mK, 42Sc, 46V, 50Mn, 54Co, 62Ga, 66As, 70Br, 74Rb; compiled, analyzed superallowed β-decay decay Q(EC), T1/2, ft, branching ratios; deduced limits on weak-interaction parameters.

doi: 10.1103/PhysRevC.71.055501


2012WA38

Chin.Phys.C 36, 1603 (2012)

M.Wang, G.Audi, A.H.Wapstra, F.G.Kondev, M.MacCormick, X.Xu, B.Pfeiffer

The AME2012 atomic mass evaluation (II). Tables, graphs and references

COMPILATION A=1-295; compiled, evaluated atomic mass data.


2013LA23

Phys.Rev. C 88, 015501 (2013)

A.T.Laffoley, C.E.Svensson, C.Andreoiu, R.A.E.Austin, G.C.Ball, B.Blank, H.Bouzomita, D.S.Cross, A.Diaz Varela, R.Dunlop, P.Finlay, A.B.Garnsworthy, P.E.Garrett, J.Giovinazzo, G.F.Grinyer, G.Hackman, B.Hadinia, D.S.Jamieson, S.Ketelhut, K.G.Leach, J.R.Leslie, E.Tardiff, J.C.Thomas, C.Unsworth

High-precision half-life measurements for the superallowed Fermi β+ emitter 14O

RADIOACTIVITY 14O(β+)[from 12C14O molecules in A=26 products produced in bombardment of SiC target by 500 MeV protons]; measured Eγ, Iγ, Eβ, Iβ, half-life of 14O superallowed β+ emitter using 8π detector array for γ rays and plastic scintillators for β radiation at TRIUMF-ISAC facility. Detailed analysis of statistical and systematic uncertainties. Comparison with previous experimental half-life values.

doi: 10.1103/PhysRevC.88.015501


2014GE07

Phys.Rev. C 90, 065501 (2014)

E.A.George, P.A.Voytas, G.W.Severin, L.D.Knutson

Measurement of the shape factor for the β decay of 14O

RADIOACTIVITY 14O(β+)[from 14N(p, n), E=8 MeV]; measured Eγ, Iγ using BGO detector, Eβ, Iβ using a superconducting beta spectrometer at University of Wisconsin Nuclear Physics Laboratory; deduced statistical shape S(E) of the β+ spectrum for the 0+ to 1+ β transition as a function of the positron kinetic energy. Comparison with predictions from theoretical calculations. Relevance to test of conserved vector current (CVC) hypothesis.

doi: 10.1103/PhysRevC.90.065501


2015VA08

Phys.Rev.Lett. 114, 232502 (2015)

A.A.Valverde, G.Bollen, M.Brodeur, R.A.Bryce, K.Cooper, M.Eibach, K.Gulyuz, C.Izzo, D.J.Morrissey, M.Redshaw, R.Ringle, R.Sandler, S.Schwarz, C.S.Sumithrarachchi, A.C.C.Villari

First Direct Determination of the Superallowed β-Decay QEC Value for 14O

RADIOACTIVITY 14O(EC), (β+) [from Be(16O, X)14O, E=150 MeV/nucleon]; measured time-of-flight cyclotron resonance, frequency ratios; deduced T1/2, ground-state Q-value, log ft. Comparison with available data.

doi: 10.1103/PhysRevLett.114.232502


2015VO18

Phys.Rev. C 92, 065502 (2015)

P.A.Voytas, E.A.George, G.W.Severin, L.Zhan, L.D.Knutson

Measurement of the branching ratio for the β decay of 14O

RADIOACTIVITY 14O(EC), (β+)[from N(p, n), E=8 MeV]; measured Eβ, Iβ positron spectra using a superconducting magnetic spectrometer and a thick Si(Li) detector at the University of Wisconsin Nuclear Physics Laboratory; deduced β branching ratio and partial half-life for superallowed 0+ to 0+ Fermi decay to the first excited state of 14N, logft, Ft. Discussed impact on the determination of the Vud element of the CKM matrix. Comparison with previous experimental measurements, and with evaluation of other superallowed 0+ to 0+ β transitions.

doi: 10.1103/PhysRevC.92.065502