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Search: Author = N.A.Jelley

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2004BL02      Nucl.Instrum.Methods Phys.Res. A517, 139 (2004)

I.Blevis, J.Boger, E.Bonvin, B.T.Cleveland, X.Dai, F.Dalnoki-Veress, G.Doucas, J.Farine, H.Fergani, D.Grant, R.L.Hahn, A.S.Hamer, C.K.Hargrove, H.Heron, P.Jagam, N.A.Jelley, C.Jillings, A.B.Knox, H.W.Lee, I.Levine, M.Liu, S.Majerus, A.McDonald, K.McFarlane, C.Mifflin, A.J.Noble, S.Noel, V.M.Novikov, J.K.Rowley, M.Shatkay, J.J.Simpson, D.Sinclair, B.Sur, J.-X.Wang, M.Yeh, X.Zhu

Measurement of 222Rn dissolved in water at the Sudbury Neutrino Observatory

RADIOACTIVITY 222Rn(α); measured Eα, Iα, contribution to detector background.

doi: 10.1016/j.nima.2003.10.103
Citations: PlumX Metrics

1995BO43      Z.Phys. C68, 391 (1995)

M.G.Bowler, N.A.Jelley

Investigations into the Origin of the Spurious 17 keV Neutrino Signal Observed in 35S Beta Decay

RADIOACTIVITY 35S(β-); measured β spectrum; deduced β-endpoint energy, 17 keV neutrino admixture upper limit.

doi: 10.1007/BF01620714
Citations: PlumX Metrics

1994BO33      Phys.Lett. 331B, 193 (1994)

M.G.Bowler, N.A.Jelley

The Origin of the Spurious 17 keV Neutrino Signal Observed in 35S Beta-Decay

RADIOACTIVITY 35S(β-); measured β-spectra; deduced spurious 17 keV ν signal origin. Different geometries, collimation, source thickness, clumping associated energy loss effects.

doi: 10.1016/0370-2693(94)90963-6
Citations: PlumX Metrics

1991HI06      Phys.Lett. 257B, 441 (1991)

A.Hime, N.A.Jelley

New Evidence for the 17 keV Neutrino

RADIOACTIVITY 32S; measured β-spectrum; deduced 17 keV neutrino mass component, mixing probability. High statistics measurements.

doi: 10.1016/0370-2693(91)91922-I
Citations: PlumX Metrics

1985WI18      Nucl.Phys. A437, 65 (1985)

J.S.Winfield, N.A.Jelley, W.D.M.Rae, C.L.Woods

Spectroscopic-Factor Discrepancies in (9Be, 10B) For Different Ejectile Excitations

NUCLEAR REACTIONS 63Cu, 54Fe, 26,24Mg, 16O(9Be, 10B), 26Mg, 16O(9Be, 9Be), E=43 MeV; 40Ca(9Be, 10B), (9Be, 9Be), E=30, 45 MeV; measured σ(θ). 62Ni, 53Mn, 25,23Na, 15N, 39K levels deduced spectroscopic factors. Magnetic spectrometer, ΔE counter telescope.

doi: 10.1016/0375-9474(85)90227-1
Citations: PlumX Metrics

1984BI03      Nucl.Phys. A413, 503 (1984)

J.Billowes, E.G.Adelberger, O.Avila, N.A.Jelley, W.R.Kolbl

The g-Factor and Lifetime of the 3- (298 keV) States in 16N

NUCLEAR REACTIONS 2H(15N, p), E=25 MeV; measured γ(θ), DSA, γ(θ, t). 16N levels deduced g, T1/2, μ, B(M1). Ge(Li) detector, deuterium target. Shell model calculations.

doi: 10.1016/0375-9474(84)90424-X
Citations: PlumX Metrics

1982WO09      J.Phys.(London) G8, 1699 (1982)

C.L.Woods, B.A.Brown, N.A.Jelley

A Comparison of Woods-Saxon and Doubled-Folding Potentials for Lithium Scattering from Light Target Nuclei

NUCLEAR REACTIONS 12C, 16O, 26Mg(6Li, 6Li), E=36 MeV; 15N(7Li, 7Li), E=28.8 MeV; 25Mg(7Li, 7Li), E=27 MeV; 12C(6Li, 6Li'), E=36 MeV; calculated σ(θ); deduced potential dependence. Woods-Saxon, double folding potentials, optical model, DWBA analyses.

doi: 10.1088/0305-4616/8/12/012
Citations: PlumX Metrics

1980WO05      J.Phys.(London) G6, L187 (1980)

C.L.Woods, N.A.Jelley, A.A.Pilt, J.S.Winfield

Is the (6Li, 7Be)Reaction a Useful Spectroscopic Tool (Question)

NUCLEAR REACTIONS 26Mg(6Li, 7Be), (6Li, 6Li), (6Li, 6Li'), E=36 MeV; measured σ(θ). 26Mg level deduced β2. 25Na level deduced C2S; DWBA.

doi: 10.1088/0305-4616/6/11/002
Citations: PlumX Metrics

1977RO03      Can.J.Phys. 55, 206 (1977)

D.W.O.Rogers, N.Anyas-Weiss, S.P.Dolan, N.A.Jelley, T.K.Alexander

Gamma Decay of the T = 3/2 States in 25Al

NUCLEAR REACTIONS 24Mg(p, γ), E ≈ 6 MeV; measured σ(E, Eγ, θ). 25Al resonances deduced J, π, Γγ.

doi: 10.1139/p77-029
Citations: PlumX Metrics

1977WE03      Nucl.Phys. A280, 217 (1977)

R.B.Weisenmiller, N.A.Jelley, D.Ashery, K.H.Wilcox, G.J.Wozniak, M.S.Zisman, J.Cerny

Very Light Neutron-Rich Nuclei Studied with the (6Li, 8B) Reaction

NUCLEAR REACTIONS 6Li(6Li, 8B), 7Li(6Li, 8B), 9Be(6Li, 8B), 11B(6Li, 8B), E=80.0, 93.3 MeV; measured σ(θ). 4H, 7He, 9Li deduced structure parameters.

doi: 10.1016/0375-9474(77)90305-0
Citations: PlumX Metrics

1976BH03      Nucl.Phys. A269, 327 (1976)

K.Bharuth-Ram, K.P.Jackson, P.G.Lawson, N.A.Jelley, K.W.Allen

Electromagnetic Transitions in 19F

NUCLEAR REACTIONS 19F(p, p'γ), E=5-9 MeV; measured Eγ, Iγ, p'γ-coin, γ(θ), DSA. 19F deduced levels, J, π, T1/2, Γ, Γγ, γ-branching. Ge(Li) detectors.

doi: 10.1016/0375-9474(76)90684-9
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1976WE09      Phys.Rev. C13, 1330 (1976)

R.B.Weisenmiller, N.A.Jelley, K.H.Wilcox, G.J.Wozniak, J.Cerny

Spectroscopic Utility of the Two-Proton Pickup (6Li, 8β) Reaction

NUCLEAR REACTIONS 10B, 12,13C, 16O(6Li, 8B), E=80, 93 MeV; measured σ(E(8B), θ) to levels in 8Li, 10,11Be, 14C.

doi: 10.1103/PhysRevC.13.1330
Citations: PlumX Metrics

1976WO11      Phys.Rev. C14, 815 (1976)

G.J.Wozniak, D.P.Stahel, J.Cerny, N.A.Jelley

(α, 8Be) Reaction in the 1p Shell

NUCLEAR REACTIONS 9Be, 10,11B, 12,13C, 14,15N, 16O(α, 8Be), E=65-72.5 MeV; measured σ(E(8Be), θ). 5He, 6,7Li, 8,9Be, 10,11B, 12C levels deduced absolute, relative S α, L. DWBA analysis.

doi: 10.1103/PhysRevC.14.815
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2760.

1975JE02      Phys.Rev. C11, 2049 (1975)

N.A.Jelley, J.Cerny, D.P.Stahel, K.H.Wilcox

Predictions of the Masses of Highly Neutron-Righ Light Nuclei

ATOMIC MASSES A=8-43; calculated mass excess, p-, n-binding energy, Q.

doi: 10.1103/PhysRevC.11.2049
Citations: PlumX Metrics

1975PA14      Nucl.Phys. A252, 173 (1975)

I.Paschopoulos, P.S.Fisher, N.A.Jelley, S.Kahana, A.A.Pilt, W.D.M.Rae, D.Sinclair

DWBA Analysis for Single-Particle Transfers Induced by 11B on 26Mg at 114 MeV

NUCLEAR REACTIONS 26Mg(11B, 10B), (11B, 10Be), (11B, 12B), (11B, 12C), E=114 MeV; measured σ(θ). 27Mg, 27Al, 25Mg, 25Na levels deduced S. Optical model, DWBA analyses. Enriched target. ΔE counter telescope.

doi: 10.1016/0375-9474(75)90611-9
Citations: PlumX Metrics

1975WI26      Phys. Lett. 59B, 142 (1975)

K.H.Wilcox, R.B.Weisenmiller, G.J.Wozniak, N.A.Jelley, D.Ashery, J.Cerny

The (9Be, 8B) Reaction and the Unbound Nuclide 10Li

NUCLEAR REACTIONS 9Be(9Be, 8B), E=121 MeV; measured σ(E(8B), θ); deduced Q. 10Li deduced mass excess.

doi: 10.1016/0370-2693(75)90687-5
Citations: PlumX Metrics

1974CE05      Phys.Rev. C10, 2654 (1974)

J.Cerny, N.A.Jelley, D.L.Hendrie, C.F.Maguire, J.Mahoney, D.K.Scott, R.B.Weisenmiller

A More Accurate Mass for 8He

NUCLEAR REACTIONS 26Mg(α, 8He), E=110.6 MeV; measured σ(E(8He)). 8He deduced mass excess. 8C, 20Mg; calculated mass excess.

doi: 10.1103/PhysRevC.10.2654
Citations: PlumX Metrics

1974CE06      Phys.Lett. 53B, 247 (1974)

J.Cerny, R.B.Weisenmiller, N.A.Jelley, K.H.Wilcox, G.J.Wozniak

7Li + 7Li Reaction Studies Leading to Multi-Neutron Final States

NUCLEAR REACTIONS 7Li(7Li, X), (16O, X), (7Li, 11C), (7Li, 11B), (7Li, 12B), (7Li, 10C), E=79.6 MeV; measured σ.

doi: 10.1016/0370-2693(74)90471-7
Citations: PlumX Metrics

1974JE01      Phys.Rev. C9, 2067 (1974)

N.A.Jelley, K.H.Wilcox, R.B.Weisenmiller, G.J.Wozniak, J.Cerny

Masses for 43Ar and the New Isotopes 45Ar and 46Ar

NUCLEAR REACTIONS 48Ca(α, 9Be), (α, 7Be), (6Li, 8B), Eα=78 MeV, E(6Li)=80 MeV; measured σ(E(9Be), E(7Be), E(8B)), Q. 43,45,46Ar deduced levels.

doi: 10.1103/PhysRevC.9.2067
Citations: PlumX Metrics

1974RO27      Nucl.Phys. A226, 424 (1974)

D.W.O.Rogers, J.A.Becker, T.K.Alexander, N.Anyas-Weiss, T.A.Belote, S.P.Dolan, N.A.Jelley, W.L.Randolph

The Electromagnetic Decay of 17N

NUCLEAR REACTIONS 11B(7Li, pγ), E=6.0 MeV; measured Eγ, I(θ), γp-coin. 17N deduced E(X), γ-branching ratios, T1/2, J, π.

doi: 10.1016/0375-9474(74)90493-X
Citations: PlumX Metrics

1974UN01      Nucl.Phys. A225, 253 (1974)

B.Y.Underwood, M.R.Wormald, N.Anyas-Weiss, N.A.Jelley, K.W.Allen

High Spin States in the Kπ = 1/2- Band of 19F

NUCLEAR REACTIONS 15N(α, γ), E=4.00, 5.41, 6.26 MeV; measured Eγ, Iγ(θ), DSA, (α-width)(γ-width)/total width. 19F resonances deduced T1/2, γ-width, J, π.

doi: 10.1016/0375-9474(74)90541-7
Citations: PlumX Metrics

1973AN01      Nucl.Phys. A201, 513 (1973)

N.Anyas-Weiss, R.Griffiths, N.A.Jelley, W.Randolph, J.Szucs, T.K.Alexander

Lifetimes in 22Ne, 22Na, 30Si, 30P and 35Cl Using the Recoil-Distance Method

NUCLEAR REACTIONS 19F(α, p), 19F(α, n), 27Al(α, p), 27Al(α, n), 32S(α, p), E=5.5, 8.6 MeV; measured recoil distance. 22Ne, 22Na, 30Si, 30P, 35Cl levels deduced T1/2. Natural targets.

doi: 10.1016/0375-9474(73)90317-5
Citations: PlumX Metrics

1973MA47      Phys.Lett. 47B, 237 (1973)

J.A.MacDonald, N.A.Jelley, J.Cerny

Analyzing Powers in 208Pb(p, t)206Pb Transitions

NUCLEAR REACTIONS 208Pb(polarized p, t), E=40 MeV; measured σ(Et, θ), A(θ). 206Pb deduced transitions.

doi: 10.1016/0370-2693(73)90719-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0293.

1973ST08      Nucl.Phys. A206, 207 (1973)

D.F.H.Start, N.A.Jelley, J.Burde, D.A.Hutcheon, W.L.Randolph, B.Y.Underwood, R.E.Warner

Gamma-Ray Transitions from the Lowest T = 2 States of 24Na and 28Al

NUCLEAR REACTIONS 22Ne(3He, pγ), E=9.0 MeV; 26Mg(3He, pγ), E=8.0 MeV; measured σ(E;Eγ, θ(pγ)). 24Na, 28Al deduced levels, branching ratios, T. Enriched targets.

doi: 10.1016/0375-9474(73)90617-9
Citations: PlumX Metrics

1973WI06      Phys.Rev.Lett. 30, 866 (1973)

K.H.Wilcox, N.A.Jelley, G.J.Wozniak, R.B.Weisenmiller, H.L.Harney, J.Cerny

New Spectroscopic Measurements via Exotic Nuclear Rearrangement; the Reaction 26Mg(7Li, 8B)25Ne

NUCLEAR REACTIONS 26Mg(7Li, 8B), E=79 MeV; measured σ(E(8B)), Q. 25Ne deduced levels.

doi: 10.1103/PhysRevLett.30.866
Citations: PlumX Metrics

1973WO06      Phys.Rev.Lett. 31, 607 (1973)

G.J.Wozniak, N.A.Jelley, J.Cerny

Feasibility of α-Transfer Studies via the (α, 8Be) Reaction at High Energies

NUCLEAR REACTIONS 11B, 12C, 16O(α, 8Be), 11B(α, 7Li), E=65 MeV; measured σ(E(8Be)), σ(θ), σ(E(7Li)).

doi: 10.1103/PhysRevLett.31.607
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2758.

1972AL32      Nucl.Phys. A197, 1 (1972)

T.K.Alexander, B.Y.Underwood, N.Anyas-Weiss, N.A.Jelley, J.Szucs, S.P.Dolan, M.R.Wormald, K.W.Allen

16O(α, γ)20Ne Capture γ-Ray Measurements on the Excited Kπ = 0+ Bands in 20Ne Near 7 MeV

NUCLEAR REACTIONS 16O(α, γ), E approx 3 to 7.6 MeV; measured omegaγ, σ(E;Eγ, θ(γ)). 20Ne deduced level energies, γ-width, γ-ray branching, γ-mixing.

doi: 10.1016/0375-9474(72)90741-5
Citations: PlumX Metrics

1972JE04      Phys.Lett. 40B, 200 (1972)

N.A.Jelley, N.Anyas-Weiss, M.R.Wormald, B.Y.Underwood, K.W.Allen

Decay of the 15.22 Mev, T=2 State in 28Si

NUCLEAR REACTIONS 24Mg(α, γ), E approx 6.1 MeV; measured γγ-coin, σ(E;Eγ). 28Si deduced resonances, levels, level-width, γ-branching, isobaric analogs.

doi: 10.1016/0370-2693(72)90409-1
Citations: PlumX Metrics

1971RO33      Phys.Lett. 37B, 65 (1971)

D.W.O.Rogers, K.W.Allen, H.C.Evans, N.A.Jelley, A.E.Litherland, B.Y.Underwood

The 5- Resonance in the 16O(α, γ)20Ne Reaction at E = 4.65 MeV

NUCLEAR REACTIONS 16O(α, γ), E approx 4.6 MeV; measured σ(E;Eγ). 20Ne deduced resonance, level-width, J, π, γ-branching.

doi: 10.1016/0370-2693(71)90572-7
Citations: PlumX Metrics

1970CE02      Phys.Rev.Lett. 24, 1128 (1970)

J.Cerny, C.U.Cardinal, H.C.Evans, K.P.Jackson, N.A.Jelley

49Fe: A New T(z) = -3/2 Delayed-Proton Emitter

RADIOACTIVITY 49Fe[from 40Ca(12C, 3n)]; measured T1/2, delayed proton spectrum. 33Ar; measured delayed proton spectrum.

NUCLEAR REACTIONS 24Mg, 28Si(12C, 3n), 40Ca(12C, 3n), E=65 MeV; measured delayed proton spectrum.

doi: 10.1103/PhysRevLett.24.1128
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1970JA22      Phys.Lett. 33B, 281 (1970)

K.P.Jackson, C.U.Cardinal, H.C.Evans, N.A.Jelley, J.Cerny

53Co-m: A Proton-Unstable Isomer

NUCLEAR REACTIONS Ca(16O, 2np), E < 81 MeV; measured σ(E), delayed-p spectrum, (16O)(γ)-delay. 53mCo deduced T1/2.

doi: 10.1016/0370-2693(70)90269-8
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