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Search: Author = K.S.Dhuga

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2002BR49      Phys.Rev. C 66, 054006 (2002)

W.J.Briscoe, B.L.Berman, R.W.C.Carter, K.S.Dhuga, S.K.Matthews, N.-J.Nicholas, S.J.Greene, B.M.K.Nefkens, J.W.Price, L.D.Isenhower, M.E.Sadler, I.Slaus, I.Supek

Elastic scattering of charged pions from ³H and ³He

NUCLEAR REACTIONS ³H, ³He(π⁺, π⁺), (π^-, π^-), E=142, 180, 220, 256 MeV; measured σ(θ) ratios; deduced reaction mechanism features.

doi: 10.1103/PhysRevC.66.054006
Citations: PlumX Metrics

2002KU36      Phys.Rev. C 66, 054007 (2002)

A.E.Kudryavtsev, V.E.Tarasov, B.L.Berman, W.J.Briscoe, K.S.Dhuga, I.I.Strakovsky

Charge-symmetry violation in pion scattering from three-body nuclei

NUCLEAR REACTIONS ³H, ³He(π⁺, π⁺), (π^-, π^-), E=142, 180, 220, 256 MeV; calculated, analyzed σ(θ), ratios; deduced charge-symmetry violation features.

doi: 10.1103/PhysRevC.66.054007
Citations: PlumX Metrics

2000BA88      Phys.Rev. C62, 044003 (2000)

V.V.Baru, A.E.Kudryavtsev, V.E.Tarasov, W.J.Briscoe, K.S.Dhuga, I.I.Strakovsky

Charge Symmetry Violation Effects in Pion Scattering Off the Deuteron

NUCLEAR REACTIONS ²H(π⁺, π⁺), (π^-, π^-), E=143, 180, 220, 256 MeV; calculated charge asymmetry vs angle; deduced possible charge symmetry violation mechanism. Comparisons with data.

doi: 10.1103/PhysRevC.62.044003
Citations: PlumX Metrics

1998CO06      Phys.Rev. C57, 1569 (1998)

J.P.Connelly, B.L.Berman, W.J.Briscoe, K.S.Dhuga, A.Mokhtari, D.Zubanov, H.P.Blok, R.Ent, J.H.Mitchell, L.Lapikas

Trinucleon Cluster Knockout from ⁶Li

NUCLEAR REACTIONS ⁶Li(e, e'³He), E=484.5 MeV; ⁶Li(e, e't), E=456, 524 MeV; measured σ(E, θ) momentum transfer dependence; deduced two-step processes.

doi: 10.1103/PhysRevC.57.1569
Citations: PlumX Metrics

1996DH01      Phys.Rev. C54, 2823 (1996)

K.S.Dhuga, B.L.Berman, W.J.Briscoe, R.W.Caress, S.K.Matthews, D.B.Barlow, B.M.K.Nefkens, C.Pillai, J.W.Price, S.J.Greene, I.Slaus, I.Supek

Investigation of Nuclear Charge Symmetry by Pion Elastic Scattering from ³H and ³He

NUCLEAR REACTIONS ³H, ³He(π⁺, π⁺), (π^-, π^-), E=180-295 MeV; measured σ(E, θ); deduced role of charge symmetry breaking in the pion-nucleus system.

doi: 10.1103/PhysRevC.54.2823
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1996LA04      Phys.Rev. C53, 1167 (1996)

C.M.Laymon, W.Amos, M.G.Burlein, H.T.Fortune, T.Ekenberg, A.Kotwal, J.M.O'Donnell, J.D.Silk, J.D.Zumbro, C.L.Morris, S.J.Seestrom, K.S.Dhuga, R.Garnett, M.W.Rawool-Sullivan, C.F.Moore, S.L.Morris, D.L.Watson

Pion Elastic and Inelastic 2⁺₁ Scattering on ^58,60,62,64Ni at T(π) = 180 MeV

NUCLEAR REACTIONS ^58,60,62,64Ni(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=180 MeV; measured σ(θ); deduced nucleon radii, deformation parameters. ^58,60,62,64Ni levels deduced neutron, proton matrix elements.

doi: 10.1103/PhysRevC.53.1167
Citations: PlumX Metrics

1995BU01      Phys.Rev. C51, 88 (1995)

M.Burlein, H.T.Fortune, W.M.Amos, T.L.Ekenberg, A.Kotwal, P.H.Kutt, J.M.O'Donnell, J.D.Silk, B.Boyer, A.Fuentes, K.Johnson, C.F.Moore, S.H.Yoo, S.Mordechai, C.L.Morris, J.D.Zumbro, D.L.Watson, K.S.Dhuga

Pion Inelastic Scattering to Low-Lying Positive-Parity States in ²⁰Ne

NUCLEAR REACTIONS ²⁰Ne(π⁺, π⁺'), E=120, 180 MeV; ²⁰Ne(π^-, π^-'), E=180 MeV; measured σ(θ). Coupled-channels analysis.

doi: 10.1103/PhysRevC.51.88
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1995MA32      Phys.Rev. C51, 2534 (1995)

S.K.Matthews, W.J.Briscoe, C.Bennhold, B.L.Berman, R.W.Caress, K.S.Dhuga, S.N.Dragic, S.S.Kamalov, N.J.Nicholas, M.F.Taragin, L.Tiator, S.J.Greene, D.B.Barlow, B.M.K.Nefkens, C.Pillai, J.W.Price, L.D.Isenhower, M.E.Sadler, I.Slaus, I.Supek

Elastic Scattering of Pions from ³H and ³He into the Backward Hemisphere

NUCLEAR REACTIONS ³He, ³H(π⁺, π⁺), E=142-256 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.51.2534
Citations: PlumX Metrics

1993BR03      Nucl.Phys. A553, 585c (1993)

W.J.Briscoe, D.B.Barlow, B.L.Berman, R.W.Caress, K.S.Dhuga, S.N.Dragic, S.J.Greene, L.D.Isenhower, D.Knowles, D.Macek, S.K.Matthews, A.Mokhtari, B.M.K.Nefkens, N.J.Nicholas, C.Pillai, J.W.Price, M.E.Sadler, I.Slaus, I.Supek, M.F.Taragin

π± Elastic and Inelastic Scattering from ³H and ³He

NUCLEAR REACTIONS ³H, ³He(π⁺, π⁺), (π⁺, π⁺'), (π^-, π^-), (π^-, π^-'), E=142-256 MeV; measured σ(θ). ³H, ³He deduced matter form factors differences.

doi: 10.1016/0375-9474(93)90663-I
Citations: PlumX Metrics

1991BR21      Phys.Rev. C44, 2031 (1991)

B.Brinkmoller, C.L.Blilie, D.Dehnhard, M.K.Jones, G.M.Martinez, S.K.Nanda, S.M.Sterbenz, Y.-F.Yen, L.G.Atencio, S.J.Greene, C.L.Morris, S.J.Seestrom, G.R.Burleson, K.S.Dhuga, J.A.Faucett, R.W.Garnett, K.Maeda, C.F.Moore, S.Mordechai, A.Williams, S.H.Yoo, L.C.Bland

Elastic Scattering of π⁺ and π^- from ⁴He between 90 and 240 MeV

NUCLEAR REACTIONS ⁴He(π⁺, π⁺), (π^-, π^-), E=90-240 MeV; measured σ(θ); deduced phase shifts. Optical model analysis.

doi: 10.1103/PhysRevC.44.2031
Citations: PlumX Metrics

1990CL03      Phys.Rev.Lett. 65, 547 (1990)

B.L.Clausen, R.A.Lindgren, M.Farkhondeh, L.W.Fagg, D.I.Sober, C.W.de Jager, H.de Vries, N.Kalantar-Nayestanaki, B.L.Berman, K.S.Dhuga, J.A.Carr, F.Petrovich, P.E.Burt

Electroexcitation of 6^- States in ³²S

NUCLEAR REACTIONS ³²S(e, e'), E=207 MeV; measured σ(E(e')), form factors; deduced spectator nucleons role. ³²S levels deduced extreme single particle model strengths. Stretched state transitions.

doi: 10.1103/PhysRevLett.65.547
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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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1989BU14      Phys.Rev. C40, 785 (1989)

M.Burlein, H.T.Fortune, W.M.Amos, T.L.Ekenberg, A.Kotwal, P.H.Kutt, J.M.O'Donnell, J.D.Silk, B.Boyer, A.Fuentes, K.Johnson, C.F.Moore, S.H.Yoo, S.Mordechai, J.D.Zumbro, D.L.Watson, K.S.Dhuga

Pion Inelastic Scattering to the Low-Lying Broad 2⁺ in ²⁰Ne

NUCLEAR REACTIONS ²⁰Ne(π⁺, π⁺'), E=120, 180 MeV; ²⁰Ne(π^-, π^-'), E=180 MeV; measured σ(θ), σ(E(π')). ²⁰Ne deduced resonances, J, π, Γ.

doi: 10.1103/PhysRevC.40.785
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1989WI02      Phys.Lett. 216B, 11 (1989)

A.L.Williams, L.Agnew, L.G.Atencio, H.W.Baer, M.Burlein, G.R.Burleson, K.S.Dhuga, H.T.Fortune, G.S.Kyle, J.A.McGill, C.F.Moore, C.L.Morris, S.Mordechai, J.M.O'Donnell, M.W.Rawool, S.Schilling, J.D.Silk, J.D.Zumbro

Pion Double Charge Exchange Above the Δ(1232) Resonance

NUCLEAR REACTIONS ¹⁴C, ¹⁸O(π⁺, π^-), E=300, 400, 500 MeV; measured σ(E(π), θ(π)). ¹⁴N, ¹⁸Ne deduced double IAS excitation.

doi: 10.1016/0370-2693(89)91360-9
Citations: PlumX Metrics

1988ER04      Phys.Rev. C37, 2651 (1988)

D.J.Ernst, K.S.Dhuga

Delta-Hole Model in the Local-Density Approximation

NUCLEAR REACTIONS ¹²C, ⁴⁰Ca, ¹⁶O(π⁺, π⁺), E=162 MeV; calculated σ(θ). Isobar-hole model.

doi: 10.1103/PhysRevC.37.2651
Citations: PlumX Metrics

1988FA05      Phys.Lett. 208B, 361 (1988)

A.Fazely, R.J.Estep, S.J.Greene, F.Irom, L.C.Liu, J.E.Warren, D.L.Watson, K.S.Dhuga, R.W.Garnett, M.Burlein, J.D.Zumbro, S.H.Rokni

Nonanalog 0⁺(g.s.) → 0⁺(g.s.) Transitions in Pion Double Charge Exchange Reactions on ¹²⁸Te and ¹³⁰Te

NUCLEAR REACTIONS ^128,130Te(π⁺, π^-), E=164 MeV; measured missing mass spectra; deduced σ ratio, ββ-decay T_1/2 ratio geochemical interpretation.

doi: 10.1016/0370-2693(88)90629-6
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1987DH01      Phys.Rev. C35, 1148 (1987)

K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, Z.F.Wang, J.W.McDonald, C.F.Moore, S.Mordechai, A.L.Williams, P.A.Seidl, M.A.Bryan, S.Nanda, S.J.Seestrom-Morris, J.D.Zumbro

Sensitivity of Large-Angle Pion Elastic Scattering to Medium Modifications

NUCLEAR REACTIONS ¹²C, ¹⁶O(π⁺, π⁺), E=100-240 MeV; measured σ(θ); deduced model parameter modifications. Optical model.

doi: 10.1103/PhysRevC.35.1148
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1987FA05      Phys.Rev. C35, 1570 (1987)

J.A.Faucett, M.W.Rawool, K.S.Dhuga, J.D.Zumbro, R.Gilman, H.T.Fortune, C.L.Morris, M.A.Plum

Pion Double Charge Exchange on ¹²C at Low Energies

NUCLEAR REACTIONS ¹²C(π⁺, π^-), E=50-120 MeV; measured σ(θ), σ(θ) vs E, σ(E(π^-)); deduced σ energy dependence.

doi: 10.1103/PhysRevC.35.1570
Citations: PlumX Metrics

1987GI04      Phys.Rev. C35, 1334 (1987)

R.Gilman, H.T.Fortune, J.D.Zumbro, C.M.Laymon, G.R.Burleson, J.A.Faucett, W.B.Cottingame, C.L.Morris, P.A.Seidl, C.F.Moore, L.C.Bland, R.R.Kiziah, S.Mordechai, K.S.Dhuga

Mass Dependence of Pion Double Charge Exchange

NUCLEAR REACTIONS ^40,44Ca(π⁺, π^-), E=163, 210 MeV; ⁵⁶Fe, ⁵⁸Ni(π^-, π⁺), E=164 MeV; ⁵⁶Fe(π⁺, π^-), E=100-292 MeV; ⁸⁰Se(π⁺, π^-), E=100-190 MeV; ⁹⁰Zr(π⁺, π^-), E=164, 211 MeV; ¹¹⁸Sn(π⁺, π^-), E=165, 212 MeV; measured σ(θ=5°); deduced reaction mechanism. ⁴⁴Ti, ⁵⁶Ni, ⁵⁶Cr, ⁵⁸Fe, ⁸⁰Kr, ⁹⁰Mo, ¹¹⁸Te deduced nonanalog, double analog transition differences.

doi: 10.1103/PhysRevC.35.1334
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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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1986DH01      Phys.Rev. C33, 1294 (1986)

K.S.Dhuga, H.T.Fortune, M.Burlein, M.Carchidi, M.Dwyer, G.Gilfoyle, J.W.Sweet

Direct and Compound Components of the ²⁷Al(⁶Li, α)²⁹Si Reaction at 32 MeV

NUCLEAR REACTIONS, ICPND ²⁷Al(⁶Li, α), E=32 MeV; measured σ(Eα), σ(θ); deduced σ, direct, compound components, potential, level density prameters. ²⁹Si levels deduced spectroscopic factors. DWBA, statistical model analyses.

doi: 10.1103/PhysRevC.33.1294
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0027.

1986GI06      Phys.Rev. C33, 1082 (1986)

R.Gilman, H.T.Fortune, J.D.Zumbro, P.A.Seidl, C.F.Moore, C.L.Morris, J.A.Faucett, G.R.Burleson, S.Mordechai, K.S.Dhuga

Angular Distributions for ¹⁴C, ²⁶Mg(π⁺, π^-)

NUCLEAR REACTIONS ¹⁴C, ²⁶Mg(π⁺, π^-), E=80-292 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.33.1082
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1985DH01      Phys.Rev. C32, 2208 (1985)

K.S.Dhuga, G.R.Burleson, J.A.Faucett, R.L.Boudrie, W.B.Cottingame, S.J.Greene, C.L.Morris, N.Tanaka, Z.F.Wang, S.Nanda, D.Dehnhard, J.D.Zumbro, S.Mordechai, C.F.Moore, D.J.Ernst

Large-Angle Elastic Scattering of π⁺ and π^- from ¹⁶O at 114 MeV

NUCLEAR REACTIONS ¹⁶O(π⁺, π⁺), (π^-, π^-), E=114 MeV; measured σ(θ); deduced large σ(π⁺)/σ(π^-) differences. First-, second-order optical model calculations.

doi: 10.1103/PhysRevC.32.2208
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1985GI07      Phys.Rev. C32, 861 (1985)

G.P.Gilfoyle, L.C.Bland, R.Gilman, M.Carchidi, K.S.Dhuga, J.W.Sweet, A.H.Wuosmaa, G.S.F.Stephans, R.W.Zurmuhle, H.T.Fortune

Resonances in ¹³C(¹³C, α)²²Ne

NUCLEAR REACTIONS, ICPND ¹³C(¹³C, α), E(cm)=6.25-13.38 MeV; measured σ(E), σ(θ). Legendre polynomial, grid search analyses.

doi: 10.1103/PhysRevC.32.861
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1391.

1985MO03      Phys.Rev.Lett. 54, 775 (1985)

C.L.Morris, S.J.Greene, R.Gilman, H.T.Fortune, J.D.Zumbro, J.A.Faucett, G.R.Burleson, K.S.Dhuga, P.A.Seidl, S.Mordechai, C.F.Moore

Properties of the ²⁰⁸Po(0⁺, T=22) Double Isobaric Analog State

NUCLEAR REACTIONS ²⁰⁸Pb(π⁺, π^-), E=295 MeV; measured σ(E(π^-)); deduced isobaric multiplet mass equation linear, quadratic terms. ²⁰⁸Po deduced double analog, Γ.

doi: 10.1103/PhysRevLett.54.775
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1985MO18      Phys.Rev. C32, 999 (1985)

S.Mordechai, P.A.Seidl, C.F.Moore, L.C.Bland, R.Gilman, K.S.Dhuga, H.T.Fortune, C.L.Morris, S.J.Greene

Systematics of Continuum Pion Double Charge Exchange on T = 0 Nuclei

NUCLEAR REACTIONS ¹²C, ²⁴Mg, ²⁸Si, ³²S, ⁴⁰Ca(π⁺, π^-), E=120-210 MeV; measured σ(θ, E(π)). ¹²C, ⁴⁰Ca(π⁺, π^-), E=164 MeV; measured σ(θ); deduced target mass, E(π), excitation energy dependences. ¹²O, ⁴⁰Ti deduced nonanalog transition excitation.

doi: 10.1103/PhysRevC.32.999
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1985SE08      Phys.Lett. 154B, 255 (1985)

P.A.Seidl, C.F.Moore, S.Mordechai, R.Gilman, K.S.Dhuga, H.T.Fortune, J.D.Zumbro, C.L.Morris, J.A.Faucett, G.R.Burleson

The Energy Dependence of ¹⁸O(π⁺, π^-)¹⁸Ne(gs)

NUCLEAR REACTIONS ¹⁸O(π⁺, π^-), E=100-292 MeV; measured σ(θ) vs E; deduced reaction energy dependence, mechanism.

doi: 10.1016/0370-2693(85)90358-2
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1984BU13      Phys.Rev. C29, 2013 (1984)

M.Burlein, K.S.Dhuga, H.T.Fortune

Spectroscopic Factors in ²⁵Mg(d, p)²⁶Mg

NUCLEAR REACTIONS ²⁵Mg(d, p), E=12 MeV; measured σ(θ), σ(Ep). ²⁶Mg deduced levels, J, π, spectroscopic factors. DWBA analysis, shell model comparison.

doi: 10.1103/PhysRevC.29.2013
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1197.

1984DH02      Phys.Rev. C29, 1566 (1984)

K.S.Dhuga, H.T.Fortune, M.Carchidi, G.P.Gilfoyle, R.Gilman, J.W.Sweet, A.Wuosmaa

Dominance of l = 10 in ¹²C(¹²C, α)²⁰Ne(g.s.) at E(c.m.) = 13-15 MeV

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, α), E(cm)=13-15 MeV; measured σ(E), σ(θ) vs E; deduced L=10 partial wave dominance. Legendre polynomial analysis.

doi: 10.1103/PhysRevC.29.1566
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1984GI05      Phys.Rev. C29, 2395 (1984)

R.Gilman, H.T.Fortune, K.S.Dhuga, P.H.Kutt, L.C.Bland, R.R.Kiziah, C.F.Moore, P.A.Seidl, C.L.Morris, W.B.Cottingame

Energy Dependence of Angular Distributions in the Nonanalog Pion Double-Charge-Exchange Reaction ¹⁶O(π⁺, π^-)¹⁶Ne(g.s.)

NUCLEAR REACTIONS ¹⁶O(π⁺, π^-), E=164 MeV; measured σ(θ); deduced nonanalog double charge exchange reaction mechanism characteristics. Damped Bessel function fit, other data input.

doi: 10.1103/PhysRevC.29.2395
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1984SW02      Phys.Rev. C30, 556 (1984)

J.W.Sweet, H.T.Fortune, R.W.Zurmuhle, L.C.Bland, M.Carchidi, K.S.Dhuga, G.P.Gilfoyle, R.Gilman, G.S.Stephans, A.Wuosmaa

Resonances in ¹²C(¹⁸O, α)²⁶Mg

NUCLEAR REACTIONS ¹²C(¹⁸O, α), E(cm)=10-15 MeV; measured σ(θ) vs E. ³⁰Si deduced resonance structure, J, π. Legendre polynomial analysis.

doi: 10.1103/PhysRevC.30.556
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1983EN02      Nucl.Phys. A405, 69 (1983)

F.Entezami, J.D.Brown, K.S.Dhuga, O.Karban, J.M.Nelson, S.Roman

Tensor Analysing Power of (d, ³He) and (d, t) Reactions and the D-State of the Tri-Nucleon System

NUCLEAR REACTIONS ¹⁹F, ⁴⁵Sc, ⁶³Cu, ⁶⁴Zn(polarized d, ³He), ⁶³Cu, ⁶⁴Zn(polarized d, t), E=12.4 MeV; measured σ(θ), iT₁₁, T₂₀, T₂₂; deduced tri-nucleon wave function D-state parameter. Natural ¹⁹F, ⁴⁵Sc, enriched ⁶³Cu, ⁶⁴Zn targets.

doi: 10.1016/0375-9474(83)90324-X
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