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NSR database version of May 1, 2024.

Search: Author = J.E.Purcell

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2017KE05      Nucl.Phys. A968, 71 (2017)

J.H.Kelley, J.E.Purcell, C.G.Sheu

Energy levels of light nuclei A = 12

COMPILATION ¹²He, ¹²Li, ¹²Be, ¹²B, ¹²C, ¹²N, ¹²O; compiled data on energy levels, J, π, γ transitions, other structure data.

doi: 10.1016/j.nuclphysa.2017.07.015
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This article is in the ENSDF database. For more information, click here.

2015PU04      Nucl.Data Sheets 130, 1 (2015)

J.E.Purcell, C.G.Sheu

Nuclear Data Sheets for A = 3

COMPILATION ³H, ³He, ³Li; compiled, evaluated nuclear structure data.

doi: 10.1016/j.nds.2015.11.001
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This article is in the ENSDF database. For more information, click here.

2012KE01      Nucl.Phys. A880, 88 (2012)

J.H.Kelley, E.Kwan, J.E.Purcell, C.G.Sheu, H.R.Weller

Energy levels of light nuclei A=11

COMPILATION ¹¹He, ¹¹Li, ¹¹Be, ¹¹B, ¹¹C, ¹¹N; compiled, evaluated levels, J, π, mass, resonances, resonance T_1/2, decay modes, γ transitions, Q, quadrupole moment, μ. Comparison with older evaluations.

doi: 10.1016/j.nuclphysa.2012.01.010
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This article is in the ENSDF database. For more information, click here.

2010PU04      Nucl.Phys. A848, 1 (2010)

J.E.Purcell, J.H.Kelley, E.Kwan, C.G.Sheu, H.R.Weller

Energy levels of light nuclei A=3

COMPILATION ³n, ³H, ³He, ³Li; compiled evaluated nuclear structure data.

doi: 10.1016/j.nuclphysa.2010.08.012
Citations: PlumX Metrics

2004TI06      Nucl.Phys. A745, 155 (2004)

D.R.Tilley, J.H.Kelley, J.L.Godwin, D.J.Millener, J.E.Purcell, C.G.Sheu, H.R.Weller

Energy levels of light nuclei A = 8, 9, 10

COMPILATION ^8,10n, ^8,9,10He, ^8,9,10Li, ^8,9,10Be, ^8,9,10B, ^8,9,10C, ^9,10N, ¹⁰O, ¹⁰F, ¹⁰Ne; compiled, evaluated structure data.

doi: 10.1016/j.nuclphysa.2004.09.059
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This article is in the ENSDF database. For more information, select a mass: 9 , 10 .

1993SY03      Phys.Rev. C48, 2252 (1993)

G.N.Sylvan, J.E.Purcell, J.Doring, J.W.Holcomb, G.D.Johns, T.D.Johnson, M.A.Riley, P.C.Womble, V.A.Wood, S.L.Tabor

Shape Coexistence and Signature Splitting in ⁷⁷Br

NUCLEAR REACTIONS ⁶⁵Cu(¹⁸O, 2nα), E=65 MeV; measured γγ-coin, DCO ratios. ⁷⁷Br deduced levels, J, π, band structure. Model comparison.

doi: 10.1103/PhysRevC.48.2252
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1990CH06      Phys.Lett. 235B, 225 (1990)

P.C.Chiang, M.R.Meder, J.E.Purcell

A Systematic Study of the D-State Probability of ⁴He Using Eight Different Realistic N-N Interactions

NUCLEAR STRUCTURE ⁴He; calculated binding energy, D-state probability. Several interactions.

doi: 10.1016/0370-2693(90)91954-A
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1983ME06      Phys.Rev. C27, 1790 (1983)

M.R.Meder, J.E.Purcell

Shell Model Calculations using Modified Sussex Matrix Elements for A ≤ 4

NUCLEAR STRUCTURE ³H, ^3,4He; calculated binding energies, negative parity states. Shell model, Sussex matrix elements.

doi: 10.1103/PhysRevC.27.1790
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1978PH01      Nucl.Phys. A294, 6 (1978)

R.J.Philpott, D.Mukhopadhyay, J.E.Purcell

Application of the v-w Formalism to the Continuum Shell Model

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca(p, p), E=40-50 MeV; calculated σ.

doi: 10.1016/0375-9474(78)90391-3
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1977PU02      Phys.Rev. C16, 76 (1977)

J.E.Purcell, M.R.Meder

Application of the Unified Weak-Coupling Model to Neutron Scattering by ¹²C

NUCLEAR REACTIONS ¹²C(n, n), E=0-5 MeV; calculated total σ(E), phase shifts. Unified model.

doi: 10.1103/PhysRevC.16.76
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1975ME24      Phys.Rev. C12, 2056 (1975)

M.R.Meder, J.E.Purcell

Unified Weak-Coupling Model of Mass 13 Nuclei, Including Exchange Effects

NUCLEAR STRUCTURE ¹³C, ¹³N; calculated levels, log ft, μ, B(λ).

doi: 10.1103/PhysRevC.12.2056
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1974ME19      Phys.Rev. C10, 84 (1974)

M.R.Meder, J.E.Purcell

Structure of Low-Lying Negative Parity States of ¹¹B and ¹¹C

NUCLEAR STRUCTURE ¹¹B, ¹¹C; calculated μ, log ft, quadrupole moment. ¹¹B calculated B(M1), B(E2).

doi: 10.1103/PhysRevC.10.84
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1974PU02      Phys.Rev. C10, 89 (1974)

J.E.Purcell, M.R.Meder

Multiplet Structure of Highly Excited States in ¹⁵N and ¹⁵O

NUCLEAR STRUCTURE ¹⁵O, ¹⁵N; calculated levels, J, π.

doi: 10.1103/PhysRevC.10.89
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1969PU05      Phys.Rev. 185, 1279 (1969)

J.E.Purcell

Nuclear-Structure Calculations in the Continuum-Application to Neutron-Carbon Scattering

NUCLEAR REACTIONS ¹²C(n, n), (n, X), E= 0-5 MeV; calculated σ(E), σ(T)(E). Weak-coupling particle-rotator model for ¹³C.

doi: 10.1103/PhysRev.185.1279
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