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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
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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
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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
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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
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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
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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
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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
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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
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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
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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 T1/2 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
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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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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
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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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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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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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