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NSR database version of April 11, 2024.

Search: Author = D.J.Millener

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2013GA33      Nucl.Phys. A914, 34c (2013)

F.Garibaldi, P.Bydzovsky, E.Cisbani, F.Cusanno, R.De Leo, S.Frullani, M.Iodice, J.J.LeRose, P.Markowitz, D.J.Millener, G.M.Urciuoli, for the Hall A Collaboration

High resolution hypernuclear spectroscopy at Jefferson Lab Hall A

NUCLEAR REACTIONS 12C(e, e'K+), E at 1.56 GeV/c; calculated hypernucleus σ(Ea, E*). Compared to published data.

doi: 10.1016/j.nuclphysa.2013.02.054
Citations: PlumX Metrics


2013GA51      Phys.Lett. B 725, 445 (2013)

A.Gal, D.J.Millener

Neutron-rich hypernuclei: 6ΛH and beyond

NUCLEAR STRUCTURE 6H, 9He, 10Li, 12Be, 14B; calculated hypernuclei binding energies; analyzed particle stability of 6H.

doi: 10.1016/j.physletb.2013.07.027
Citations: PlumX Metrics


2013MI18      Nucl.Phys. A914, 109c (2013)

D.J.Millener

Shell-model calculations applied to the γ-ray spectroscopy of light Λ hypernuclei

NUCLEAR STRUCTURE 7,8,9Li, 9,10Be, 11B, 12C, 15N, 16O; calculated Λ hypernuclei levels, J, π, double-spacings; deduced (some) parameters. 18F; calculated levels, J, π, matrix elements. Shell model calculations with Λ- and Σ-hypernuclear states and used data on hypernuclei γ transitions.

doi: 10.1016/j.nuclphysa.2013.01.023
Citations: PlumX Metrics


2012MI11      Nucl.Phys. A881, 298 (2012)

D.J.Millener

Shell-model calculations for p-shell hypernuclei

NUCLEAR STRUCTURE 7,8,9He, 7,8,9,10Li, 9,11,12Be, 10,11,12,13,14B, 13,14,15C, 15,16N; calculated Λ hypernuclei ground state binding energy, levels, J, π, γ transitions, branching ratios, T1/2 using shell model.

doi: 10.1016/j.nuclphysa.2012.01.019
Citations: PlumX Metrics


2010GA29      Int.J.Mod.Phys. E19, 2487 (2010)

F.Garibaldi, E.Cisbani, F.Cusanno, S.Frullani, M.Iodice, G.M.Urciuoli, R.De Leo, L.Lagamba, S.Marrone, J.J.LeRose, C.W.de Jager, R.J.Feuerbach, D.W.Higinbotham, B.Reitz, A.Acha, P.Markowitz, P.Bydzovsky, M.Sotona, C.C.Chang, J.Millener

High-resolution hypernuclear spectroscopy electron scattering at JLab, HALL A

NUCLEAR REACTIONS 9B, 12C, 16O(E, EK+)9Li/12B/16N, E=4 GeV; measured reaction products; deduced σ(θ, E), hypernuclear levels and relative strengths. Comparison with theoretical calculations.

doi: 10.1142/S0218301310016995
Citations: PlumX Metrics


2010MI25      Nucl.Phys. A835, 11c (2010)

D.J.Millener

Shell-model structure of light hypernuclei

NUCLEAR STRUCTURE 11B; calculated hypernucleus ground state, J, π, levels using shell model; deduced model parameters.

doi: 10.1016/j.nuclphysa.2010.01.169
Citations: PlumX Metrics


2009MI26      Nucl.Phys. A827, 297c (2009)

D.J.Millener

Structure of p-shell hypernuclei and the spin-dependence of YN interactions from γ-ray spectroscopy

NUCLEAR STRUCTURE 7Li, 9Be, 10,11B, 12C, 15N, 16O; calculated hypernuclei levels, J, π including Λ-Σ coupling. Comparison with data.

doi: 10.1016/j.nuclphysa.2009.05.060
Citations: PlumX Metrics


2008MI08      Nucl.Phys. A804, 84 (2008)

D.J.Millener

Shell-model interpretation of γ-ray transitions in p-shell hypernuclei

NUCLEAR STRUCTURE 7Li, 9Be, 10,11B, 12C, 15N, 16O; calculated hypernuclei levels, J, π including Λ-Σ coupling. Comparison with data.

doi: 10.1016/j.nuclphysa.2008.02.252
Citations: PlumX Metrics


2008MO06      Nucl.Phys. A804, 99 (2008)

T.Motoba, D.E.Lanskoy, D.J.Millener, Y.Yamamoto

Λ spin-orbit splitting in heavy hypernuclei as deduced from DWIA analyses of the 89Y(π+, K+)89ΛY reaction

NUCLEAR REACTIONS 89Y(π+, K+), E at 1.05 GeV/c; calculated hypernuclei production σ(θ) and excitation spectra using DWIA. 89Y deduced hypernuclei levels, J, π.

doi: 10.1016/j.nuclphysa.2008.01.026
Citations: PlumX Metrics


2008UK01      Phys.Rev. C 77, 054315 (2008)

M.Ukai, S.Ajimura, H.Akikawa, D.E.Alburger, A.Banu, R.E.Chrien, G.B.Franklin, J.Franz, O.Hashimoto, T.Hayakawa, H.Hotchi, K.Imai, T.Kishimoto, M.May, D.J.Millener, S.Minami, Y.Miura, T.Miyoshi, K.Mizunuma, T.Nagae, S.N.Nakamura, K.Nakazawa, Y.Okayasu, P.Pile, B.P.Quinn, A.Rusek, Y.Sato, R.Sutter, H.Takahashi, L.Tang, H.Tamura, K.Tanida, S.H.Zhou, for the E930('01) Collaboration

γ-ray spectroscopy of 16ΛO and 15ΛN hypernuclei via the 16O(K-, π-γ) reaction

NUCLEAR REACTIONS 16O(K-, π-γ), (K-, π-p), E=900 MeV/c; measured Eγ, Iγ, γγ-coin, angular distributions, B(M1), missing mass spectra. 16O, 15N; deduced levels, J, π of hypernuclei. Comparison with shell model calculations.

doi: 10.1103/PhysRevC.77.054315
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2007UK01      Eur.Phys.J. A 33, 247 (2007)

M.Ukai, S.Ajimura, H.Akikawa, D.E.Alburger, A.Banu, R.E.Chrien, G.B.Franklin, J.Franz, O.Hashimoto, T.Hayakawa, H.Hotchi, K.Imai, T.Kishimoto, M.May, D.J.Millener, S.Minami, Y.Miura, T.Miyoshi, K.Mizunuma, T.Nagae, S.N.Nakamura, K.Nakazawa, Y.Okayasu, P.Pile, B.P.Quinn, A.Rusek, Y.Sato, R.Sutter, H.Takahashi, L.Tang, H.Tamura, K.Tanida, L.Yuan, S.H.Zhou

Observation of the 7 MeV excited spin-flip and non-spin-flip partners in 16ΛO by γ-ray spectroscopy

NUCLEAR REACTIONS 16O(K-, π-), E at 0.93 GeV/c; measured Eγ, Iγ from decaying hypernucleus. 16O deduced hypernucleus levels, J, π. Hyperball array.

doi: 10.1140/epja/i2007-10473-7
Citations: PlumX Metrics


2006UK01      Phys.Rev. C 73, 012501 (2006)

M.Ukai, S.Ajimura, H.Akikawa, D.E.Alburger, A.Banu, R.E.Chrien, G.B.Franklin, J.Franz, O.Hashimoto, T.Hayakawa, H.Hotchi, K.Imai, T.Kishimoto, M.May, D.J.Millener, S.Minami, Y.Miura, T.Miyoshi, K.Mizunuma, T.Nagae, S.N.Nakamura, K.Nakazawa, Y.Okayasu, P.Pile, B.P.Quinn, A.Rusek, Y.Sato, R.Sutter, H.Takahashi, L.Tang, H.Tamura, K.Tanida, L.Yuan, S.H.Zhou, and the E930('01) Collaboration

Cascade γ decay in the 7ΛLi hypernucleus

NUCLEAR REACTIONS 10B(K-, π-), E at 0.93 GeV/c; measured Eγ, Iγ, γγ-, (particle)γ-coin following hypernucleus creation and decay. 7Li deduced hypernucleus levels, J, π. Hyperball array.

doi: 10.1103/PhysRevC.73.012501
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2005AS04      Phys.Rev. C 72, 024314 (2005)

N.I.Ashwood, M.Freer, D.J.Millener, N.A.Orr, F.Carstoiu, S.Ahmed, J.C.Angelique, V.Bouchat, W.N.Catford, N.M.Clarke, N.Curtis, F.Hanappe, M.Horoi, Y.Kerckx, J.L.Lecouey, F.M.Marques, T.Materna, G.Normand, S.Pain, N.Soic, C.Timis, A.Unshakova, V.A.Ziman

High-energy two-neutron removal from 10Be

NUCLEAR REACTIONS 12C(10Be, 2α), (10Be, n2α), E=30 MeV/nucleon; measured En, Eα, relative energy spectra, σ(E). 8,9Be deduced levels, J, π. Kinematically complete measurement.

doi: 10.1103/PhysRevC.72.024314
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1402.


2005MI18      Nucl.Phys. A754, 48c (2005)

D.J.Millener

Hypernuclear structure from γ-ray spectroscopy

NUCLEAR STRUCTURE 7Li, 9Be, 10,11B, 15N, 16O; analyzed hypernucleus levels, J, π, T1/2; deduced constraints on hyperon-nucleon interaction.

doi: 10.1016/j.nuclphysa.2004.12.068
Citations: PlumX Metrics


2005MI30      Eur.Phys.J. A 25, Supplement 1, 97 (2005)

D.J.Millener

Beta decays of 8He, 9Li, and 9C

RADIOACTIVITY 8He, 9Li(β-); 9C(β+); analyzed transitions B(GT), symmetry effects.

NUCLEAR STRUCTURE 8Li; calculated triton and neutron decay widths for 1+ level.

doi: 10.1140/epjad/i2005-06-049-5
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 .


2004UK01      Phys.Rev.Lett. 93, 232501 (2004)

M.Ukai, S.Ajimura, H.Akikawa, D.E.Alburger, A.Banu, R.E.Chrien, G.B.Franklin, J.Franz, O.Hashimoto, T.Hayakawa, H.Hotchi, K.Imai, T.Kishimoto, M.May, D.J.Millener, S.Minami, Y.Miura, T.Miyoshi, K.Mizunuma, T.Nagae, S.N.Nakamura, K.Nakazawa, Y.Okayasu, P.Pile, B.P.Quinn, A.Rusek, Y.Sato, R.Sutter, H.Takahashi, L.Tang, H.Tamura, K.Tanida, L.Yuan, S.H.Zhou, and the E930('01) Collaboration

Hypernuclear Fine Structure in 16ΛO and the ΛN Tensor Interaction

NUCLEAR REACTIONS 16O(K-, π-), E at 0.93 GeV/c; measured Eγ, Iγ, (particle)γ-coin. 16O deduced hypernucleus level energies, transitions. Hyperball array.

doi: 10.1103/PhysRevLett.93.232501
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2003KA46      Phys.Rev. C 68, 037302 (2003)

D.E.Kahana, S.H.Kahana, D.J.Millener

Resonant state in 4ΛHe

NUCLEAR STRUCTURE 4He; analyzed data; deduced hypernucleus resonant state features.

doi: 10.1103/PhysRevC.68.037302
Citations: PlumX Metrics


2002BR22      Phys.Rev. C65, 051309 (2002)

B.A.Brown, F.C.Barker, D.J.Millener

Di-Proton Decay of the 6.15 MeV 1- State in 18Ne

NUCLEAR STRUCTURE 18Ne; calculated one- and two-proton decay widths, spectroscopic factors for 1- state. Sequential and direct two-proton decay considered. Comparison with data.

doi: 10.1103/PhysRevC.65.051309
Citations: PlumX Metrics


2001MI29      Nucl.Phys. A693, 394 (2001)

D.J.Millener

Structure of Unstable Light Nuclei

doi: 10.1016/S0375-9474(01)00589-9
Citations: PlumX Metrics


2001MI32      Nucl.Phys. A691, 93 (2001)

D.J.Millener

Shell-Model Description of Λ Hypernuclei

NUCLEAR STRUCTURE 7Li, 9Be, 12,13C, 16O; analyzed hypernucleus levels J, π; deduced shell-model parameters.

doi: 10.1016/S0375-9474(01)01013-2
Citations: PlumX Metrics


1998AZ01      Phys.Rev. C57, 628 (1998)

A.Azhari, T.Baumann, J.A.Brown, M.Hellstrom, J.H.Kelley, R.A.Kryger, D.J.Millener, H.Madani, E.Ramakrishnan, D.E.Russ, T.Suomijarvi, M.Thoennessen, S.Yokoyama

Proton Decay of States in 11N

NUCLEAR REACTIONS 9Be(12N, 11N), E=40 MeV/nucleon; measured projectile-like fragment decay p(10C)-coin. 11N deduced levels J, π, Γ, proton decay branching ratios.

doi: 10.1103/PhysRevC.57.628
Citations: PlumX Metrics


1997FR22      Phys.Lett. 414B, 7 (1997)

N.Frazier, B.A.Brown, D.J.Millener, V.Zelevinsky

Gamow-Teller Strength as a Function of Excitation Energy

NUCLEAR STRUCTURE 24Mg; calculated total Gamow-Teller strength vs excitation energy; deduced spatial symmetry energy dependence. Shell model.

doi: 10.1016/S0370-2693(97)01144-1
Citations: PlumX Metrics


1997MI08      Phys.Rev. C55, R1633 (1997)

D.J.Millener

First-Forbidden β Decay of 17N and 17Ne

RADIOACTIVITY 17N(β-); 17Ne(β+); analyzed β-decay rates via f values; deduced charge-dependent effects role. Shell model.

NUCLEAR STRUCTURE 18O, 18Ne; calculated binding energy. Shell model.

doi: 10.1103/PhysRevC.55.R1633
Citations: PlumX Metrics


1997TE14      Phys.Lett. 413B, 253 (1997)

J.A.Templon, B.A.Raue, K.Murphy, D.J.Millener, D.S.Carman, G.M.Huber, B.C.Markham, D.W.Miller, P.Schwandt, L.C.Bland

Study of Continuum Nuclear Structure of 12C Via (p, p'X) at Intermediate Energies

NUCLEAR REACTIONS 12C(p, p'), (p, 2p), (p, pα), E=156 MeV; measured Ep, Ip, σ(θ, Ep). 12C deduced small continuum nonresonant contribution.

doi: 10.1016/S0370-2693(97)01149-0
Citations: PlumX Metrics


1996AN08      Phys.Rev. C54, 237 (1996)

B.D.Anderson, L.A.C.Garcia, D.J.Millener, D.M.Manley, A.R.Baldwin, A.Fazely, R.Madey, N.Tamimi, J.W.Watson, C.C.Foster

12C(p, n)12N Reaction at 135 MeV

NUCLEAR REACTIONS 12C(p, n), E=135 MeV; measured σ(θ) vs excitation energy. 12N deduced levels, Γ, J, π. DWBA analysis.

NUCLEAR STRUCTURE 12N; calculated levels, one-body density matrices, Coulomb energy shifts. 12N levels deduced J, π. Shell model.

doi: 10.1103/PhysRevC.54.237
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0441.


1994DO09      Nucl.Phys. A572, 85 (1994)

C.B.Dover, A.Gal, D.J.Millener

On the Production and Decay of Strangeness S = -2 Hypernuclei

doi: 10.1016/0375-9474(94)90423-5
Citations: PlumX Metrics


1994MI37      Prog.Theor.Phys.(Kyoto), Suppl. 117, 307 (1994)

D.J.Millener, C.B.Dover, A.Gal

Widths of Ξ Hypernuclear States

NUCLEAR STRUCTURE A=12; calculated Λ-, neutron decay widths in hypernuclei. Shell model approach.

doi: 10.1143/PTPS.117.307
Citations: PlumX Metrics


1994RA17      Phys.Rev. C50, 682 (1994)

S.Raman, E.T.Jurney, J.W.Starner, A.Kuronen, J.Keinonen, K.Nordlund, D.J.Millener

Lifetimes in 15N from Gamma-Ray Line Shapes Produced in the 2H(14N, pγ) and 14N(thermal n, γ) Reactions

NUCLEAR REACTIONS 2H(14N, p), E=10 MeV; 14N(n, γ), E=thermal; measured Eγ, Iγ, DSA; deduced 15N, 15O mirror symmetry features. 15N levels deduced T1/2.

doi: 10.1103/PhysRevC.50.682
Citations: PlumX Metrics


1993HA27      Phys.Rev.Lett. 71, 1498 (1993)

J.Hao, T.T.S.Kuo, A.Reuber, K.Holinde, J.Speth, D.J.Millener

Hypernucleus 16O(Lambda) and Accurate Hyperon-Nucleon G-Matrix Interactions

NUCLEAR STRUCTURE A=16; calculated hypernucleus spectrum. G-matrix approach.

doi: 10.1103/PhysRevLett.71.1498
Citations: PlumX Metrics


1993OL03      Nucl.Phys. A559, 368 (1993)

N.Olsson, H.Conde, E.Ramstrom, T.Ronnqvist, R.Zorro, J.Blomgren, A.Hakansson, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, A.Brockstedt, P.Ekstrom, M.Osterlund, S.Y.van der Werf, D.J.Millener, G.Szeflinska, Z.Szeflinski

The 12C(n, p)12B Reaction at E(n) = 98 MeV

NUCLEAR REACTIONS 12C(n, p), E=98 MeV; measured σ(Ep, θ), θ=0°-33°. 12B deduced ΔL=0-3 multipole strength distributions. DWBA calculations, multipole decomposition.

doi: 10.1016/0375-9474(93)90159-U
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22243.


1992MI01      Phys.Rev. C45, 473 (1992)

D.J.Millener, A.C.Hayes, D.Strottman

Comment on ' p-Shell Nuclei in a (0+2)(h-bar x Omega) Model Space. I. Method ' and on ' p-Shell nuclei in a (0+2)(h-bar x Omega) Model Space. II. Results '

NUCLEAR STRUCTURE 16O; analyzed other model calculation results; deduced effective interaction inconsistencies.

doi: 10.1103/PhysRevC.45.473
Citations: PlumX Metrics


1992WA25      Phys.Lett. 293B, 7 (1992)

E.K.Warburton, B.A.Brown, D.J.Millener

Large-Basis Shell-Model Treatment of A = 16

NUCLEAR STRUCTURE 16O; calculated levels. Large basis shell model.

RADIOACTIVITY 16N(β-); calculated unique first forbidden β-decay matrix element. Large basis shell model.

doi: 10.1016/0370-2693(92)91472-L
Citations: PlumX Metrics


1991BR10      Phys.Rev. C43, 2284 (1991)

F.P.Brady, T.D.Ford, G.A.Needham, J.L.Romero, D.S.Sorenson, C.M.Castaneda, J.L.Drummond, E.L.Hjort, B.McEachern, N.S.P.King, D.J.Millener

12C(n, p)12B Reaction at 56, 60, and 65 MeV

NUCLEAR REACTIONS 12C(n, p), E=56, 60, 65 MeV; measured σ(E, θ). 12C(p, p), E=65 MeV; 12C(n, p), E=62, 65 MeV; calculated σ(θ). Microscopic DWBA, shell model analyses.

NUCLEAR STRUCTURE 12C, 12B; calculated levels, wave functions, one-body density-matrix elements. Shell model.

doi: 10.1103/PhysRevC.43.2284
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset12911.


1991DI03      Phys.Rev. C43, 1758 (1991)

S.Dixit, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, C.E.Hyde-Wright, M.V.Hynes, M.A.Kovash, B.E.Norum, J.J.Kelly, A.D.Bacher, G.T.Emery, C.C.Foster, W.P.Jones, D.W.Miller, B.L.Berman, D.J.Millener

Structure of 9Be from Proton Scattering at 180 MeV

NUCLEAR REACTIONS 9Be(polarized p, p')E=180 MeV; measured proton spectra, σ(θ), analyzing power vs θ. 9Be deduced levels, possible J, π. Other data input. Shell model.

doi: 10.1103/PhysRevC.43.1758
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0147.


1991DO07      Phys.Rev. C44, 1905 (1991)

C.B.Dover, D.J.Millener, A.Gal, D.H.Davis

Interpretation of a Double Hypernucleus Event

NUCLEAR STRUCTURE A=13; analyzed data; deduced double hypernucleus event features.

doi: 10.1103/PhysRevC.44.1905
Citations: PlumX Metrics


1991GL02      Phys.Rev. C43, 1740 (1991)

J.P.Glickman, W.Bertozzi, T.N.Buti, S.Dixit, F.W.Hersman, C.E.Hyde-Wright, M.V.Hynes, R.W.Lourie, B.E.Norum, J.J.Kelly, B.L.Berman, D.J.Millener

Electron Scattering from 9Be

NUCLEAR REACTIONS 9Be(e, e'), E=100-360 MeV; measured electron spectra, form factors. 9Be deduced levels, J, π. Shell model.

doi: 10.1103/PhysRevC.43.1740
Citations: PlumX Metrics


1991MA14      Phys.Rev. C43, 2147 (1991)

D.M.Manley, B.L.Berman, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, C.E.Hyde-Wright, M.V.Hynes, J.J.Kelly, M.A.Kovash, S.Kowalski, R.W.Lourie, B.Murdock, B.E.Norum, B.Pugh, C.Sargent, D.J.Millener

Electroexcitation of Negative-Parity States in 18O

NUCLEAR REACTIONS 18O(e, e'), E=119.4, 268.8 MeV; measured spectra, form factors. 18O levels deduced transition charge densities, reduced transition probabilities. Shell model calculations.

doi: 10.1103/PhysRevC.43.2147
Citations: PlumX Metrics


1991MI10      Nucl.Phys. A527, 471c (1991)

D.J.Millener

Progress and Open Problems in Hypernuclear Structure

NUCLEAR REACTIONS 89Y, 90Zr(π+, K+), E at 1.05 GeV/c; calculated σ(θ).

doi: 10.1016/0375-9474(91)90141-R
Citations: PlumX Metrics


1991PI07      Phys.Rev.Lett. 66, 2585 (1991)

P.H.Pile, S.Bart, R.E.Chrien, D.J.Millener, R.J.Sutter, N.Tsoupas, J.-C.Peng, C.S.Mishra, E.V.Hungerford, T.Kishimoto, L.-G.Tang, W.von Witsch, Z.Xu, K.Maeda, D.Gill, R.McCrady, B.Quinn, J.Seydoux, J.W.Sleight, R.L.Stearns, H.Plendl, A.Rafatian, J.Reidy

Study of Hypernuclei by Associated Production

NUCLEAR REACTIONS 9Be, 12C, 16O, 28Si, 40Ca, 51V, 89Y(π+, K+), E at 1048 MeV/c; measured σ(θ); deduced hypernuclei production σ, binding energies.

doi: 10.1103/PhysRevLett.66.2585
Citations: PlumX Metrics


1990CH19      Z.Phys. C46, S157 (1990)

R.E.Chrien, D.J.Millener

Hypernuclear Physics with the (π+, K+) Reaction

NUCLEAR REACTIONS 56Fe(K-, π-), E at 720 MeV/c, at rest; 56Fe(K+, π+), E at 1040 MeV/c; 9Be(K-, π-), E at 0.72 GeV/c; 9Be(K+, π+), E at 1.04 GeV/c; 89Y(K+, π+), E not given; analyzed data; deduced hypernuclear properties.


1990MA06      Phys.Rev. C41, 448 (1990)

D.M.Manley, D.J.Millener, B.L.Berman, W.Bertozzi, T.N.Buti, J.M.Finn, F.W.Hersman, C.E.Hyde-Wright, M.V.Hynes, J.J.Kelly, M.A.Kovash, S.Kowalski, R.W.Lourie, B.Murdock, B.E.Norum, B.Pugh, C.P.Sargent

Electroexcitation of Rotational Bands in 18O

NUCLEAR REACTIONS 18O(e, e'), E=194.3 MeV; measured longitudinal, Coulomb form factors. 18O levels deduced transition matrix elements, configurations. Shell model.

doi: 10.1103/PhysRevC.41.448
Citations: PlumX Metrics


1989MI01      Phys.Rev. C39, 14 (1989)

D.J.Millener, D.I.Sober, H.Crannell, J.T.O'Brien, L.W.Fagg, S.Kowalski, C.F.Williamson, L.Lapikas

Inelastic Electron Scattering from 13C

NUCLEAR REACTIONS 13C(e, e'), E=45-340 MeV; measured σ(E, θ). 13C levels deduced longitudinal, transverse form factors, multipole matrix elements. Shell model.

doi: 10.1103/PhysRevC.39.14
Citations: PlumX Metrics


1989WA06      Phys.Rev. C39, 1120 (1989)

E.K.Warburton, D.J.Millener

Structure of 17C and 17N

NUCLEAR STRUCTURE 17C; calculated levels, β-decay observables. 17N; calculated levels, B(λ). Shell model.

NUCLEAR REACTIONS 18O(3He, d), E not given; calculated spectroscopic factors. Shell model.

doi: 10.1103/PhysRevC.39.1120
Citations: PlumX Metrics


1988WA30      Ann.Phys.(New York) 187, 471 (1988)

E.K.Warburton, J.A.Becker, B.A.Brown, D.J.Millener

First-Forbidden Beta Decay Near A = 40

NUCLEAR STRUCTURE A=34-44; calculated first forbidden β-decay transition strengths. Shell model.

doi: 10.1016/0003-4916(88)90156-X
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1987CH14      Phys.Rev. C35, 2197 (1987)

S.Chakravarti, D.Dehnhard, M.A.Franey, S.J.Seestrom-Morris, D.B.Holtkamp, C.L.Blilie, A.C.Hayes, C.L.Morris, D.J.Millener

Distorted-Wave Impulse Approximation and Coupled-Channels Analysis of Inelastic Pion Scattering from 18O

NUCLEAR REACTIONS 18O(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; calculated σ(θ). 18O levels deduced transition densities. DWIA, coupled-channels calculations.

doi: 10.1103/PhysRevC.35.2197
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1987MI25      Phys.Rev. C36, 1643 (1987)

D.J.Millener

Comment on ' Electroexcitation of M4 Transitions in 17O and 18O '

NUCLEAR REACTIONS 17,18O(e, e'), E not given; calculated M4 level excitations strengths. 17,18O levels deduced possible J.

NUCLEAR STRUCTURE 17,18O; calculated levels.

doi: 10.1103/PhysRevC.36.1643
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1986DO01      Phys.Rev.Lett. 56, 119 (1986)

C.B.Dover, A.Gal, L.Klieb, D.J.Millener

Definitive Tests of the Σ-Nuclear Spin-Orbit Splitting

NUCLEAR REACTIONS 7Li, 13C(K-, π+), 13C(K-, π-), E at rest; calculated relative hypernuclei production yields.

doi: 10.1103/PhysRevLett.56.119
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1986HI06      Phys.Rev. C34, 1161 (1986)

R.S.Hicks, R.A.Lindgren, M.A.Plum, G.A.Peterson, H.Crannell, D.I.Sober, H.A.Thiessen, D.J.Millener

M4 Excitations in 13C

NUCLEAR REACTIONS 13C(e, e'), E=78-338 MeV; measured σ(E, θ). 13C levels deduced from factors, isoscalar, isovector transition amplitudes. Shell model.

doi: 10.1103/PhysRevC.34.1161
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1985SE06      Phys.Rev. C31, 923 (1985)

S.J.Seestrom-Morris, D.Dehnhard, C.L.Morris, L.C.Bland, R.Gilman, H.T.Fortune, D.J.Millener, D.P.Saunders, P.A.Seidl, R.R.Kiziah, C.F.Moore

M4 Transitions Observed in Pion Inelastic Scattering on 15N

NUCLEAR REACTIONS 15N(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=164 MeV; measured σ(θ(π), E(π)), σ(θ). 15N levels deduced M4 transition strength, form factors.

doi: 10.1103/PhysRevC.31.923
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1984BL17      Phys.Rev. C30, 1989 (1984)

C.L.Blilie, D.Dehnhard, M.A.Franey, D.H.Gay, D.B.Holtkamp, S.J.Seestrom-Morris, P.J.Ellis, C.L.Morris, D.J.Millener

Isospin Structure of Transitions in 17O from Inelastic Pion Scattering at 164 MeV

NUCLEAR REACTIONS 16,17O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 17O deduced M4, E2 transition strength distribution. Microscopic DWIA calculations.

doi: 10.1103/PhysRevC.30.1989
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1984DO04      Phys.Lett. 138B, 337 (1984)

C.B.Dover, A.Gal, D.J.Millener

Is Isospin a Good Quantum Number for Σ Hypernuclei ( Question )

NUCLEAR REACTIONS 12C(K-, π+), (K-, π-), E=400, 450 MeV/c; analyzed data; deduced isospin mixing in hypernucleus 12C.

doi: 10.1016/0370-2693(84)91911-7
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1984HI06      Phys.Rev. C30, 1 (1984)

R.S.Hicks, J.B.Flanz, R.A.Lindgren, G.A.Peterson, L.W.Fagg, D.J.Millener

Magnetic Multipole Excitations in 12C by Inelastic Electron Scattering

NUCLEAR REACTIONS 12C(e, e'), E=50.7-338 MeV; measured σ(E(e')), θ=180°, form factors. 12C deduced resonances, J, π, Γ. Shell model comparison.

doi: 10.1103/PhysRevC.30.1
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1984WA07      Phys.Rev. C29, 2281 (1984)

E.K.Warburton, D.E.Alburger, D.J.Millener

Shapes of the 16N and 15C Beta Spectra and Extraction of Matrix Elements for 15C(β-)15N(g.s.)

NUCLEAR STRUCTURE 15N; calculated partial muon capture rates.

RADIOACTIVITY 16N, 15C(β-); analyzed β-spectra shapes; deduced matrix elements, β-branching ratios, meson exchange effect. Shell model.

doi: 10.1103/PhysRevC.29.2281
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1983CA03      Phys.Rev. C27, 1175 (1983)

F.P.Calaprice, D.J.Millener

Heavy Neutrinos and the Beta Spectra of 35S, 18F, and 19Ne

RADIOACTIVITY 18F(β+), (EC); 19Ne(β+), (EC); 35S(β-); calculated β-decay matrix elements, shape factors. Shell model, effective interactions.

doi: 10.1103/PhysRevC.27.1175
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1983KO01      Phys.Rev. C27, 158 (1983)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, J.W.Olness, E.K.Warburton

Lifetimes of Levels in 20,21F, 22Ne, and 16N

NUCLEAR REACTIONS 7Li(18O, α), (18O, nα), (18O, t), E=10-60 MeV; 7Li(11B, np), E=7-35 MeV; measured Eγ, Iγ, recoil. 21F, 22Ne levels deduced T1/2. 16N, 20F levels deduced T1/2, B(λ). Shell model.

doi: 10.1103/PhysRevC.27.158
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1983KO03      Nucl.Phys. A394, 221 (1983)

P.E.Koehler, H.D.Knox, D.A.Resler, R.O.Lane, D.J.Millener

Structure of 12B from Measurement and R-Matrix Analysis of σ(θ) for 11B(n, n)11B and 11B(n, n')11B*(2.12 MeV), and Shell-Model Calculations

NUCLEAR STRUCTURE 12B; calculated levels, spectroscopic amplitudes. Shell model.

NUCLEAR REACTIONS 11B(n, n), (n, n'), E=4.8-7.6 MeV; measured σ(θ). 12B deduced levels, J, π, reduced widths. R-matrix analysis.

doi: 10.1016/0375-9474(83)90170-7
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1983MI08      Phys.Rev. C28, 497 (1983)

D.J.Millener, J.W.Olness, E.K.Warburton, S.S.Hanna

Strong E1 Transitions in 9Be, 11Be, and 13C

NUCLEAR STRUCTURE 9,11Be, 13C; calculated B(λ). Shell model.

NUCLEAR REACTIONS 9Be(t, pγ), E=1.5-3.3 MeV; 3H(9Be, pγ), E=10-16 MeV; measured DSA. 11Be level deduced T1/2.

doi: 10.1103/PhysRevC.28.497
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1982MI08      Phys.Rev. C26, 1167 (1982)

D.J.Millener, D.E.Alburger, E.K.Warburton, D.H.Wilkinson

Decay Scheme of 11Be

RADIOACTIVITY 11Be [from 9Be(t, p)]; measured Eγ, Iγ, γγ-coin; deduced log ft. 11B levels deduced β-, γ-branching, B(λ). Shell model.

doi: 10.1103/PhysRevC.26.1167
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1982OL01      Nucl.Phys. A373, 13 (1982)

J.W.Olness, E.K.Warburton, D.E.Alburger, C.J.Lister, D.J.Millener

The Beta Decay of 18N and T = 2 States of Mass 18

RADIOACTIVITY 18N; measured Eγ, Iγ, T1/2; deduced log ft. 18O deduced levels, β-branches. He transport, Ge(Li) detectors. Shell model.

doi: 10.1016/0375-9474(82)90179-8
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1981AL03      Phys.Rev. C23, 473 (1981)

D.E.Alburger, D.J.Millener, D.H.Wilkinson

Delayed Particles from the β-decay of 11Be

RADIOACTIVITY 11Be [from 9Be(t, p), E=3.4 MeV]; measured β-delayed Eα, β-delayed E(7Li), αγ-, 7Liγ-coin; deduced log ft, β-branching. 11B level deduced α-branching. Helium jet system, Si, Na(Tl) detectors.

doi: 10.1103/PhysRevC.23.473
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1981AL07      Phys.Rev. C23, 2217 (1981)

D.E.Alburger, C.J.Lister, J.W.Olness, D.J.Millener

Beta Decay of 21O

RADIOACTIVITY 21O [from 9Be(18O, 2pα), E=80-110 MeV]; measured Eγ, Iγ, Eβ, Iβ, γγ-, βγ-coin, T1/2; deduced Qβ, mass excess, log ft. 21F deduced levels, γ-branching ratios, J, π.

NUCLEAR REACTIONS 19F(t, p), E=2, 2.5, 3 MeV; measured Eγ, Iγ. 21F deduced levels.

NUCLEAR STRUCTURE 21F; calculated levels, J, π, B(λ), T1/2, δ. Shell model.

doi: 10.1103/PhysRevC.23.2217
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1981AU05      Phys.Rev.Lett. 47, 1110 (1981)

E.H.Auerbach, A.J.Baltz, C.B.Dover, A.Gal, S.H.Kahana, L.Ludeking, D.J.Millener

Lambda-Nuclear Properties from the Spectroscopy of 13C Hypernucleus

NUCLEAR REACTIONS 13C(K-, π-), E at 800 MeV/c; analyzed σ(θ). Shell model, DWBA calculations.

doi: 10.1103/PhysRevLett.47.1110
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1981KO08      Phys.Rev. C23, 1571 (1981)

R.L.Kozub, J.Lin, J.F.Mateja, C.J.Lister, D.J.Millener, E.K.Warburton

Electromagnetic Transitions in 14C and 14N

NUCLEAR REACTIONS 7Li(9Be, pn), E=5.5 MeV; 9Be(7Li, pn), (7Li, 2n), E=3.8-7.8 MeV; measured Eγ, Iγ, recoil. 14C, 14N levels deduced T1/2. Shell model, SU(3) basis.

NUCLEAR STRUCTURE 14C, 14N; calculated levels, B(λ), δ, Γγ, T1/2, γ-branching. Shell model, SU(3) basis.

doi: 10.1103/PhysRevC.23.1571
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1981SA07      Phys.Rev.Lett. 46, 884 (1981)

A.M.Sandorfi, M.T.Collins, D.J.Millener, A.M.Nathan, S.F.LeBrun

Evidence for Giant E2 Transitions in High-Energy α-Particle Capture

NUCLEAR REACTIONS 12C(α, γ), E=35-42.25 MeV; measured σ(E, θγ); deduced reaction mechanism. 16O deduced possible giant quadrupole excitations. Shell model calculations.

doi: 10.1103/PhysRevLett.46.884
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1980WA24      Phys.Rev. C22, 2330 (1980)

E.K.Warburton, D.E.Alburger, D.J.Millener

Energies and Branching Ratios of γ transitions in 13C

NUCLEAR REACTIONS 10B(α, p), E=1.66 MeV; 12C(d, p) E=2.51 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 13C level deduced T1/2. 13C deduced levels, γ-branching, B(λ). Shell model.

doi: 10.1103/PhysRevC.22.2330
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1979AL23      Phys.Rev. C20, 1891 (1979)

D.E.Alburger, D.J.Millener

Beta Decay of 15C

RADIOACTIVITY 15C [from 13C(t, p), E=3 MeV]; measured Eγ, Iγ, T1/2; deduced log ft. 15N deduced levels, β-branching ratios. Shell-model interpretation.

doi: 10.1103/PhysRevC.20.1891
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1979FA12      Nucl.Phys. A330, 333 (1979)

A.Faessler, D.J.Millener, P.Paul, D.Strottman

Alpha and Proton Decay of the Isoscalar E2 Resonance in 16O and 40Ca

NUCLEAR STRUCTURE 16O, 40Ca; calculated Γα/Γp for T=0, GQR. SU(3) framework, 1p-1h excitations.

doi: 10.1016/0375-9474(79)90058-7
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1978MI10      Phys.Rev. C18, 1878 (1978)

D.J.Millener, E.K.Warburton, K.A.Snover, R.von Lintig, P.G.Ikossi

Electromagnetic Transitions between the Low-Lying Levels of 21Ne and their Relation to Parity Mixing of the 2.80-MeV 1/2± Doublet

NUCLEAR STRUCTURE 21Ne; calculated γ CP. 21Ne, 21Na; calculated nuclear wave functions, electromagnetic, parity-mixing matrix elements.

NUCLEAR REACTIONS 18O(α, n), E=5.1 MeV; measured γγ(θ). 21Ne deduced δ E3/M2.

doi: 10.1103/PhysRevC.18.1878
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1976PI16      Nucl.Phys. A273, 189 (1976)

A.A.Pilt, D.J.Millener, H.Bradlow, O.Dietzsch, P.S.Fisher, W.J.Naude, W.D.M.Rae, D.Sinclair

Study of States in 19F and 20Ne via the (13C, 9Be) α-Transfer Reaction

NUCLEAR REACTIONS 15N, 16O(13C, 9Be), E=105 MeV; measured σ(E, θ). 19F, 20Ne deduced levels, relative spectroscopic amplitudes, suggested J, π values. Enriched gas targets. Shell-model calculation.

doi: 10.1016/0375-9474(76)90307-9
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1975KU01      Nucl.Phys. A238, 269 (1975)

D.Kurath, D.J.Millener

Three-Nucleon Transfer for the 1p Shell

NUCLEAR STRUCTURE 16O, 15,14N, 14,13,12C, 11,10B, 10,9Be, 7,6Li, 4He; calculated three-nucleon transfer properties.

doi: 10.1016/0375-9474(75)90353-X
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1975MI12      Nucl.Phys. A255, 315 (1975)

D.J.Millener, D.Kurath

The Particle-Hole Interaction and the Beta Decay of 14B

RADIOACTIVITY 14B; calculated log ft.

NUCLEAR STRUCTURE 11Be, 12,14B, 13C, 14N, 16O; calculated levels.

doi: 10.1016/0375-9474(75)90683-1
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1974AN36      Phys.Rep. 12, 201 (1974)

N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland

Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions

NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 11B), (12C, 11C), (12C, 10B), (12C, 10Be), (12C, 10C), (12C, 9Be), E=114 MeV; 12,13C(11B, 9Li), E=114 MeV; 13C(11B, 10B), E=114 MeV; measured particle spectra, σ(E, θ). 13,14C, 13,14,15N, 14,15O deduced levels, J, π, spectroscopic amplitudes.

doi: 10.1016/0370-1573(74)90045-3
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1973MI06      Nucl.Phys. A209, 59 (1973)

D.J.Millener, P.E.Hodgson

The Systematics of Nuclear Single-Particle States (I). The Region 35 < A < 65

NUCLEAR STRUCTURE 36,38,40Ar, 40,42,44,46,48Ca, 45Sc, 46,47,48,49,50Ti, 51V, 48,50,52,54Cr, 55Mn, 52,54,56,58Fe, 57,59Co, 56,58,60,62,64Ni, 63,65Cu; calculated binding energies.

doi: 10.1016/0375-9474(73)90051-1
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