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NSR database version of April 27, 2024.

Search: Author = D.Oakley

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1996OA01      Phys.Rev. C53, 689 (1996)

D.S.Oakley, R.J.Peterson, C.L.Morris, H.T.Fortune

Anomalous Angular Distributions in Pion and α Particle Scattering to the 2⁺₂ State of ⁵²Cr

NUCLEAR REACTIONS ⁵²Cr(π⁺, π⁺'), (π^-, π^-'), E=180 MeV; measured σ(θ). ⁵²Cr(α, α'), E=42 MeV; analyzed σ(θ). ⁵²Cr level deduced no definitive configurational based reason for anomaly. DWBA analysis.

doi: 10.1103/PhysRevC.53.689
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1993KO17      Phys.Rev. C48, 250 (1993)

C.M.Kormanyos, R.J.Peterson, J.Applegate, J.Beck, T.D.Averett, B.G.Ritchie, C.L.Morris, J.McGill, D.S.Oakley

Low-Energy Pion Scattering to 1^- States in ¹²C

NUCLEAR REACTIONS ¹²C(π⁺, π⁺'), (π^-, π^-'), E=40, 50, 65 MeV; measured σ(θ). ¹²C deduced level energies, Γ, sum rule strengths. DWIA analysis.

doi: 10.1103/PhysRevC.48.250
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1992HI01      Phys.Rev. C45, 601 (1992)

N.M.Hintz, X.H.Yang, M.Gazzaly, S.J.Seestrom-Morris, C.L.Morris, D.C.Cook, A.M.Mack, J.W.McDonald, S.Mordechai, D.S.Oakley, C.F.Moore, M.Lynker, J.D.Zumbro

Determination of Neutron and Proton Multipole Matrix Elements in ²⁰⁸Pb from π^- and π⁺ Scattering at 180 MeV

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-'), (π^-, π^-), E=180 MeV; measured σ(θ). ²⁰⁸Pb levels deduced neutron, proton multipole matrix elements.

doi: 10.1103/PhysRevC.45.601
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1992JO03      Phys.Rev. C46, 52 (1992)

M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.H.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore

⁴He(π, π'p)³H Reaction Near the P₃₃ π-Nucleon Resonance

NUCLEAR REACTIONS ⁴He(π⁺, π⁺'p), (π^-, π^-'p), E=140, 180 MeV; measured σ(θ(π'), σ(p)) vs excitation energy; deduced reaction mechanisms.

doi: 10.1103/PhysRevC.46.52
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1992OA01      Phys.Rev. C45, 2254 (1992)

D.S.Oakley, J.R.Shepard, N.Auerbach

Nuclear Compressibility and the Isoscalar Monopole Resonance in a Relativistic Continuum Random Phase Approximation

NUCLEAR STRUCTURE ¹⁶O, ⁴⁰Ca; calculated isoscalar monopole strength distribution, transition density. Dirac-Hartree RPA, continuum.

doi: 10.1103/PhysRevC.45.2254
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1992PE14      Phys.Lett. 297B, 238 (1992)

R.J.Peterson, S.Hoibraten, J.Ouyang, M.R.Braunstein, X.Y.Chen, M.D.Kohler, B.J.Kriss, D.J.Mercer, D.S.Oakley, D.L.Prout, W.Fong

Quasifree Pion Single Charge Exchange at 500 MeV

NUCLEAR REACTIONS Zr, C(π^-, π⁰), (π⁺, π⁰), E=500 MeV; measured σ(θ); deduced quasifree peak shift features. Pauli-blocked Fermi-gas model.

doi: 10.1016/0370-2693(92)91255-8
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1991OA01      Phys.Rev. C44, 2058 (1991)

D.S.Oakley, R.J.Peterson, S.J.Seestrom, C.L.Morris, M.A.Plum, J.D.Zumbro, A.L.Williams, M.A.Bryan, J.W.McDonald, C.F.Moore

Energy Dependence of Pion Inelastic Scattering from ²⁰⁸Pb

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=120, 250 MeV; calculated σ(θ). ²⁰⁸Pb levels deduced proton, neutron matrix elements ratio. Different structure models.

doi: 10.1103/PhysRevC.44.2058
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1991WI03      Phys.Rev. C43, 766 (1991)

A.L.Williams, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, D.S.Oakley, M.Burlein, H.T.Fortune, J.M.O'Donnell, G.P.Kahrimanis, C.F.Moore

Pion Double Charge Exchange on ^42,44,48Ca for 300 ≤ T(π) ≤ 550 MeV

NUCLEAR REACTIONS ^42,44,48Ca(π⁺, π^-), E=300-550 MeV; measured σ(θ), σ(E(π)); deduced two-amplitude model parameters.

doi: 10.1103/PhysRevC.43.766
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1991WI13      Phys.Rev. C44, 2025 (1991)

A.L.Williams, K.W.Johnson, G.P.Kahrimanis, H.Ward, C.F.Moore, J.A.McGill, C.L.Morris, G.R.Burleson, J.A.Faucett, M.Rawool-Sullivan, D.S.Oakley, M.Burlein, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith

Mass Dependence of High-Energy Pion Double Charge Exchange

NUCLEAR REACTIONS ²⁶Mg, ^46,50Ti, ^54,56Fe, ⁵²Cr, ⁸⁰Se, ⁹⁰Zr, ¹⁹⁷Au, ²⁰⁸Pb(π⁺, π^-), E=450, 500 MeV; measured σ(θ), θ=5°; deduced mass dependence, two-amplitude model parameters. Double isobaric analog state excitation.

doi: 10.1103/PhysRevC.44.2025
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1990JO04      Phys.Rev. C42, R807 (1990)

M.K.Jones, D.Dehnhard, S.K.Nanda, S.M.Sterbenz, C.L.Morris, M.Plum, J.D.Zumbro, A.Hussein, D.S.Oakley, M.J.Smithson, A.L.Williams, J.McDonald, M.A.Bryan, A.H.Fuentes, M.Lynker, D.Crockett, M.A.Machuca, S.Mordechai, C.F.Moore

⁴He(π, π'p)³H Reaction: Quasifree and resonance scattering

NUCLEAR REACTIONS ⁴He(π⁺, π⁺'p), (π^-, π^-'p), E=180 MeV; measured σ(θ(π), θp); deduced σ(π⁺)/σ(π^-). DWIA calculation.

doi: 10.1103/PhysRevC.42.R807
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1990OA01      Phys.Rev. C41, 1081 (1990)

D.S.Oakley, P.D.Kunz, C.L.Morris

Coulomb-Nuclear Interference in Pion Inelastic Scattering

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π⁺'), (π^-, π^-'), E=120-250 MeV; analyzed σ(θ); deduced Coulomb-nuclear interference role. ²⁰⁸Pb levels deduced neutron, proton matrix element ratio.

doi: 10.1103/PhysRevC.41.1081
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1990SE11      Phys.Rev. C42, 1929 (1990)

P.A.Seidl, M.A.Bryan, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, R.Gilman, S.J.Greene, M.A.Machuca, C.F.Moore, S.Mordechai, C.L.Morris, D.S.Oakley, M.A.Plum, G.Rai, M.J.Smithson, Z.F.Wang, D.L.Watson, J.D.Zumbro

Pion Double Charge Exchange on T = 2 Nuclei in the Δ(3/2, 3/2) Resonance Region

NUCLEAR REACTIONS ¹²C, ¹⁶O, ⁴⁴Ca, ⁵⁶Fe(π⁺, π^-), E=100-300 MeV; measured σ(θ) vs E.

doi: 10.1103/PhysRevC.42.1929
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1990YO02      J.Phys.(London) G16, L89 (1990)

S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom, M.Jones, S.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely

²⁰⁸Pb(π±, π±'n) Reaction in the Giant-Resonance Region

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π⁺'n), (π^-, π^-'n), E=180 MeV; measured σ(θn, θπ), missing mass spectra. ²⁰⁸Pb deduced giant resonance neutron decay features.

doi: 10.1088/0954-3899/16/5/002
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1989OA01      Phys.Rev. C40, 859 (1989)

D.S.Oakley, M.R.Braunstein, J.J.Kraushaar, R.A.Loveman, R.J.Peterson, D.J.Rilett, R.L.Boudrie

Isospin Asymmetries in Pion Scattering to Isoscalar Giant Quadrupole States in Ni Isotopes

NUCLEAR REACTIONS ^58,60,62,64Ni(π⁺, π⁺'), (π^-, π^-'), E=180 MeV; measured σ(θ), σ(E(π')). ^58,60,62,64Ni deduced giant quadrupole resonance neutron, proton matrix elements, B(λ).

doi: 10.1103/PhysRevC.40.859
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1989SE12      Phys.Rev. C40, 2780 (1989)

M.E.Sevior, A.Feltham, P.Weber, G.R.Smith, D.R.Gill, D.Healey, D.Ottewell, G.D.Wait, J.T.Brack, M.Kohler, J.J.Kraushaar, D.Oakley, R.J.Peterson, R.A.Ristinen, E.L.Mathie, N.R.Stevenson, R.B.Schubank, E.Gibson, R.Arndt

Analyzing Power in π±p(pol) Elastic Scattering from T(π) = 98 to 263 MeV

NUCLEAR REACTIONS ¹H(π⁺, π⁺), (π^-, π^-), E=98-263 MeV; measured analyzing power vs θ; deduced πp phase shifts. Polarized target.

doi: 10.1103/PhysRevC.40.2780
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1989SH25      Phys.Rev. C40, 2195 (1989)

J.R.Shepard, D.S.Oakley, R.J.Peterson

Giant Resonances at Complex Excitation Energies

NUCLEAR STRUCTURE ⁴⁰Ca; calculated GQR strengths, Γ, continuum response functions. Nonspectral RPA.

doi: 10.1103/PhysRevC.40.2195
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1989YO06      Phys.Rev.Lett. 63, 738 (1989)

S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom-Morris, M.K.Jones, S.M.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely

¹²C(π±, π±'p)¹¹B Reaction Near the Giant Dipole Region

NUCLEAR REACTIONS ¹²C(π⁺, π⁺'p), (π^-, π^-'p), E=180 MeV; measured σ(θ(π), θ(p), E(π)); deduced σ(π⁺, π⁺p)/σ(π^-, π^-p) near GDR. DWIA analysis.

doi: 10.1103/PhysRevLett.63.738
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1988MO01      Phys.Rev.Lett. 60, 408 (1988)

S.Mordechai, N.Auerbach, G.R.Burleson, K.S.Dhuga, M.Dwyer, J.A.Faucett, H.T.Fortune, R.Gilman, S.J.Greene, C.Laymon, C.F.Moore, C.L.Morris, D.S.Oakley, M.A.Plum, S.J.Seestrom-Morris, P.A.Seidl, M.J.Smithson, Z.F.Wang, J.D.Zumbro

Giant Dipole Resonances Built on Isobaric Analog States in Pion Double Charge Exchange

NUCLEAR REACTIONS ⁵⁶Fe, ⁸⁰Se, ²⁰⁸Pb(π⁺, π^-), E at 292 MeV/c; measured σ(E(π^-), θ(π^-)), σ(θ(π^-)). ⁵⁶Ni, ⁸⁰Kr, ²⁰⁸Po deduced giant dipole resonance parameters. Coupled-channel impulse approximation calculations.

doi: 10.1103/PhysRevLett.60.408
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1988OA01      Phys.Rev. C37, 866 (1988)

D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, S.J.Seestrom-Morris, R.Gilman, J.D.Zumbro, H.T.Fortune, K.S.Dhuga

Pion Inelastic Scattering from ^48,50Ti, ⁵²Cr, and ^54,56Fe: Higher-lying states

NUCLEAR REACTIONS ^48,50Ti, ⁵²Cr, ^54,56Fe(π⁺, π⁺), (π⁺, π⁺'), E=180 MeV; measured σ(θ). ^48,50Ti, ⁵²Cr, ^54,56Fe levels deduced neutron, proton matrix elements.

doi: 10.1103/PhysRevC.37.866
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1988OA02      Phys.Rev. C37, 1126 (1988)

D.S.Oakley, H.T.Fortune

Configuration Dependence in Calculations for Pion Inelastic Scattering near N = 28

NUCLEAR REACTIONS ⁴⁸Ti, ⁵²Cr, ^54,56Fe(π, π'), E=180 MeV; analyzed data. ⁴⁸Ti levels deduced neutron, proton matrix element ratio. ^54,56Fe, ⁵²Cr levels deduced B(E2), neutron, proton matrix element ratio.

doi: 10.1103/PhysRevC.37.1126
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1988OA03      Phys.Rev. C38, 2978 (1988)

D.S.Oakley, R.J.Peterson, D.J.Rilett, C.L.Morris, S.J.Greene, B.Boyer, K.Johnson, A.H.Fuentes, J.W.McDonald, M.J.Smithson, A.L.Williams, S.H.Yoo, C.F.Moore

Energy Dependence of Pion Inelastic Scattering to the 1⁺ States in ¹²C

NUCLEAR REACTIONS ¹²C(π^-, π^-'), (π⁺, π⁺'), E=80-295 MeV; measured σ(θ); deduced isobar excitation role. ¹²C levels deduced σ ratio.

doi: 10.1103/PhysRevC.38.2978
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1987MO18      Phys.Rev. C36, 710 (1987)

S.Mordechai, M.J.Smithson, M.Lynker, D.S.Oakley, C.F.Moore, D.L.Watson, R.Gilman, J.D.Zumbro, P.Kutt, H.T.Fortune, C.L.Morris, K.S.Dhuga

Neutron and Proton Matrix Elements for Transitions in ³⁹K from Pion Inelastic Scattering

NUCLEAR REACTIONS ³⁹K(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured missing mass spectra, σ(θ); deduced neutron, proton octupole matrix elements. ³⁹K level deduced E2 transition probe sensitivity. DWIA analyses.

doi: 10.1103/PhysRevC.36.710
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1987OA01      Phys.Rev. C35, 1392 (1987)

D.S.Oakley, M.J.Smithson, S.Mordechai, C.F.Moore, C.L.Morris, G.C.Idzorek, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson

Pion Elastic and Inelastic Scattering from ^48,50Ti, ⁵²Cr, and ^54,56Fe at 180 MeV: Determination of neutron and proton multipole matrix elements

NUCLEAR REACTIONS ^48,50Ti, ⁵²Cr, ^54,56Fe(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured σ(E(π)), σ(θ). ^48,50Ti, ⁵²Cr, ^54,56Fe deduced levels, neutron, proton multipole matrix elements, ground state density distribution parameters.

doi: 10.1103/PhysRevC.35.1392
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1987OA02      Phys.Rev. C36, 1074 (1987)

D.S.Oakley, M.A.Machuca, M.J.Smithson, S.Mordechai, C.F.Moore, P.A.Seidl, C.L.Morris, Z.F.Wang, R.Gilman, J.D.Zumbro, H.T.Fortune, S.J.Seestrom-Morris, K.S.Dhuga, D.L.Watson

Pion Elastic and Inelastic Scattering from ⁵¹V at 180 MeV

NUCLEAR REACTIONS ⁵¹V(π⁺, π⁺), (π⁺, π⁺'), E=180 MeV; measured σ(θ). ⁵¹V deduced levels, J, π, B(λ), proton, neutron matrix elements.

doi: 10.1103/PhysRevC.36.1074
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1987ZU03      Phys.Rev. C36, 1479 (1987)

J.D.Zumbro, H.T.Fortune, M.Burlein, C.L.Morris, Z.-F.Wang, R.Gilman, K.S.Dhuga, G.R.Burleson, M.W.Rawool, R.W.Garnett, M.J.Smithson, D.S.Oakley, S.Mordechai, C.F.Moore, M.A.Machuca, D.L.Watson, N.Auerbach

Double Charge Exchange to the Double Isobaric Analog State at T(π) ≈ 292 MeV

NUCLEAR REACTIONS ³⁰Si, ³⁴S, ⁴⁴Ca, ⁵⁰Ti, ⁵¹V, ⁵²Cr, ⁵⁸Ni(π⁺, π^-), E ≈ 292 MeV; measured σ(θ), σ(π). ⁴⁴Ti, ⁵¹Mn, ⁵²Fe, ⁵⁰Cr levels deduced ground state, double IAS excitation σ.

doi: 10.1103/PhysRevC.36.1479
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1986BU13      Nucl.Instrum.Methods Phys.Res. A247, 327 (1986)

G.R.Burleson, W.B.Cottingame, K.S.Dhuga, J.A.Faucett, C.P.Fontenla, J.F.Amann, R.L.Boudrie, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, D.Yusnukis, M.Brown, R.R.Kiziah, E.C.Milner, C.F.Moore, S.Mordechai, D.Oakley, P.A.Seidl, C.L.Blilie, D.Dehnhard, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro, K.Maeda

A Large-Angle Pion-Nucleus Scattering Facility for EPICS at LAMPF

NUCLEAR REACTIONS ¹²C(π⁺, π⁺), E=162 MeV; ¹⁶O(π^-, π^-), E=114 MeV; measured σ(θ), θ=115°-180°. Energetic pion channel, spectrometer.

doi: 10.1016/0168-9002(86)91314-8
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1984KI16      Phys.Rev. C30, 1643 (1984)

R.R.Kiziah, M.D.Brown, C.J.Harvey, D.S.Oakley, D.P.Saunders, P.A.Seidl, C.F.Moore, W.B.Cottingame, R.W.Garnett, S.J.Greene, G.A.Luna, G.R.Burleson, D.B.Holtkamp

Pion Inelastic Scattering to the Low-Lying Excited States of ⁶Li

NUCLEAR REACTIONS ⁶Li(π⁺, π⁺), (π⁺, π⁺'), E=100-260 MeV; measured σ(θ); deduced reaction mechanism. ⁶Li levels deduced form factors. DWIA analysis.

doi: 10.1103/PhysRevC.30.1643
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Note: The following list of authors and aliases matches the search parameter D.Oakley: , D.A.OAKLEY, D.S.OAKLEY