NSR Query Results
Output year order : Descending NSR database version of May 2, 2024. Search: Author = M.Cable Found 15 matches. 1988ZH15 Chin.J.Nucl.Phys. 10, 351 (1988) Zhou Zongyuan, J.Cerny, M.Cable, J.Honkanen, R.Parry Measurement of Half-Life of the β-Delayed Two-Proton Decay Nuclide 22Al RADIOACTIVITY 22Al(β+p); measured T1/2. Helium jet system.
1988ZH18 High Energy Phys. and Nucl.Phys. (China) 12, 246 (1988) Z.Zhou, J.Cerny, M.Cable, J.Honkanen, R.Parry Half-life measurement of the β-delayed two-proton decay nuclide 26P
1985ZH05 Phys.Rev. C31, 1941 (1985) Z.Y.Zhou, E.C.Schloemer, M.D.Cable, M.Ahmed, J.E.Reiff, J.Cerny Additional Beta-Delayed Protons form the T(z) = -(3/2) Nuclei 21Mg, 25Si, 29S, and 41Ti RADIOACTIVITY 21Mg, 25Si, 29S, 41Ti(β+p) [from 20Ne, 24Mg, 28Si, 40Ca(3He, 2n), E=31.5-41.5 MeV]; measured β-delayed Ep, Ip; deduced log ft. 21Na, 25Al, 29P, 41Sc levels deduced relative Ip.
doi: 10.1103/PhysRevC.31.1941
1984CA29 Phys.Rev. C30, 1276 (1984) M.D.Cable, J.Honkanen, E.C.Schloemer, M.Ahmed, J.E.Reiff, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decays of 22Al and 26P RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, p4n)]; 26P(β+p) [from 28Si(3He, p4n)]; measured beta-delayed two-proton pp-coin, Ep. 21Na, 25Al deduced levels, p-branching.
doi: 10.1103/PhysRevC.30.1276
1984TO07 Phys.Rev. C30, 712 (1984) K.S.Toth, D.M.Moltz, E.C.Schloemer, M.D.Cable, F.T.Avignone III, Y.A.Ellis-Akovali Beta-Delayed Proton Activities: 147Dy and 149Er NUCLEAR REACTIONS 144Sm(12C, xn), E ≈ 135 MeV; measured delayed proton spectra; deduced evidence for 149Er. RADIOACTIVITY 147Dy, 149Er(β+p) [from 142Nd, 144Sm(12C, xn)]; measured β-delayed Ep, Ip; deduced T1/2.
doi: 10.1103/PhysRevC.30.712
1983CA01 Phys.Rev.Lett. 50, 404 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Discovery of Beta-Delayed Two-Proton Radioactivity: 22Al RADIOACTIVITY 22Al(β+p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed pp-coin, total E(2p); deduced 2p, 1p emission relative intensity. Single step 2He emission, 21Na intermediate state sequential decay discussed.
doi: 10.1103/PhysRevLett.50.404
1983CA06 Phys.Lett. 123B, 25 (1983) M.D.Cable, J.Honkanen, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of the T(z) = -2 Isotope 26P NUCLEAR REACTIONS 28Si(3He, 4np), E=110-130 MeV; measured Ep, Ip; deduced evidence for 26P. RADIOACTIVITY 26P(β+p) [from 28Si(3He, 4np), E=110-130 MeV]; measured β-delayed Ep, Ip. 26P deduced T1/2. 26Si deduced T=2 level mass excess.
doi: 10.1016/0370-2693(83)90950-4
1983HO23 Phys.Lett. 133B, 146 (1983) J.Honkanen, M.D.Cable, R.F.Parry, S.H.Zhou, Z.Y.Zhou, J.Cerny Beta-Delayed Two-Proton Decay of 26P RADIOACTIVITY 26P(β+p) [from 28Si(3He, xnyp), E=110 MeV]; measured β-delayed two-proton Ep, Ip, summed spectra; deduced two-proton emission mechanism, decay scheme.
doi: 10.1016/0370-2693(83)90547-6
1983NI05 Z.Phys. A312, 265 (1983) J.M.Nitschke, M.D.Cable, W.-D.Zeitz New Beta-Delayed Proton Emitters in the Lanthanide Region NUCLEAR REACTIONS 90Zr(40Ca, npα), (40Ca, nα), E=196 MeV; 90Zr(40Ca, 3np), E=182 MeV; 92Mo(40Ca, α), E=188 MeV; 92Mo(40Ca, nα), E=213 MeV; 50Cr(92Mo, nα), E=480 MeV; 50Cr(92Mo, n2p), E=385 MeV; 92Mo(58Ni, n2pα), E=292 MeV; 92Mo(56Fe, nα), E=275 MeV; measured β-delayed proton activity; deduced evidence for precursors 124La, 126Pr, 127,128Nd, 137,139Gd, 143Dy. RADIOACTIVITY 125Ce, 126Pr, 127,128Nd, 137,139Gd(β+p) [from 92Mo, 90Zr, 54Fe, 50Cr(92Mo, xnypzα), (58Ni, xnypzα), (56Fe, xnypzα), (40Ca, xnypzα)]; measured β-delayed proton activity, < Ep >; deduced T1/2.
doi: 10.1007/BF01412173
1983WO04 Phys.Rev. C27, 1745 (1983) J.M.Wouters, H.M.Thierens, J.Aysto, M.D.Cable, P.E.Haustein, R.F.Parry, J.Cerny Beta-decay Energies and Masses of 103-105In RADIOACTIVITY 103In(β+), (EC) [from 92Mo(14N, 3n), E=80 MeV, 92Mo(16O, 4np), E=115 MeV]; 104In(β+), (EC) [from 92Mo(16O, 3np), E=95 MeV]; 105In(β+), (EC) [from Mo(14N, xn), E=100 MeV, 92Mo(16O, 2np), E=75 MeV]; measured βγ-coin, Eβ+; deduced Q(EC), mass excesses. On-line mass separated sources, enriched Mo targets, Ge(Li), scintillation telescope detectors.
doi: 10.1103/PhysRevC.27.1745
1982CA16 Phys.Rev. C26, 1778 (1982) M.D.Cable, J.Honkanen, R.F.Parry, H.M.Thierens, J.M.Wouters, Z.Y.Zhou, J.Cerny Beta-Delayed Proton Decay of an Odd-Odd T(z) = (-2) Isotope, 22Al RADIOACTIVITY 22Al(β+), (p) [from 24Mg(3He, 4np), E=110 MeV]; measured β-delayed Ep, Ip, T1/2. 22Mg level deduced mass excess, Iβ.
doi: 10.1103/PhysRevC.26.1778
1982TO01 Phys.Rev. C25, 667 (1982) K.S.Toth, D.M.Moltz, Y.A.Ellis-Akovali, C.R.Bingham, M.D.Cable, R.F.Parry, J.M.Wouters Single-Proton States in 147Tb RADIOACTIVITY 147Dy; measured Eγ, Iγ, γγ-coin. 147Tb deduced levels, J, π.
doi: 10.1103/PhysRevC.25.667
1981AY01 Phys.Rev. C23, 879 (1981) J.Aysto, M.D.Cable, R.F.Parry, J.M.Wouters, D.M.Moltz, J.Cerny Decays of the T(z) = -2 Nuclei 20Mg, 24Si, and 36Ca RADIOACTIVITY 20Mg, 24Si, 36Ca [from Ne, Mg, Ca(3He, 3n), (3He, 3nα), E=40-100 MeV, mass separation]; measured β-delayed Ep, Ip; deduced T1/2, proton-branching; deduced coefficients of isobaric multiplet mass equation. 20Na, 24Al, 36K level deduced mass excess.
doi: 10.1103/PhysRevC.23.879
1979AY01 Phys.Lett. 82B, 43 (1979) J.Aysto, D.M.Moltz, M.D.Cable, R.D.Von Dincklage, R.F.Parry, J.M.Wouters, J.Cerny Decay of a New Isotope, 24Si: A Test of the Isobaric Multiplet Mass Equation RADIOACTIVITY 24Si [from 24Mg(3He, 3n), E=70 MeV]; measured σ(Ep) of β-delayed protons; deduced T1/2. 24Al level deduced mass excess, fit to quadratic isobaric multiplet mass equation.
doi: 10.1016/0370-2693(79)90421-0
1979MO02 Phys.Rev.Lett. 42, 43 (1979) D.M.Moltz, J.Aysto, M.D.Cable, R.D.von Dincklage, R.F.Parry, J.M.Wouters, J.Cerny Completion of the Mass-20 Isospin Quintet by Employing a Helium-Jet-Fed on-Line Mass Separator RADIOACTIVITY 20Mg [from 20Ne(3He, n)]; measured β-delayed protons. 20Na deduced mass excess. Recoil-atom analyzer. Evidence for quadratic form of isobaric multiplet mass equation.
doi: 10.1103/PhysRevLett.42.43
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