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Search: Author = J.Zumbro

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2001PA47      Phys.Lett. 523B, 1 (2001)

E.A.Pasyuk, R.L.Boudrie, P.A.M.Gram, C.L.Morris, J.D.Zumbro, J.L.Matthews, Y.Tan, V.V.Zelevinsky, G.Glass, B.J.Kriss

A Study of the Δ--Component of the Wave Function in Light Nuclei

NUCLEAR REACTIONS 3H, 4He, 6,7Li(π+, π+pX), (π+, π-pX), E=500 MeV; measured pion and proton spectra, σ. 3H, 4He, 6,7Li deduced Δ resonance component of wave function.

doi: 10.1016/S0370-2693(01)01329-6
Citations: PlumX Metrics


1998MO09      Phys.Lett. 419B, 25 (1998)

C.L.Morris, J.D.Zumbro, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Reidel, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, J.Ouyang, R.J.Peterson, J.E.Wise

Evidence for Δ+ Components in Nuclei

NUCLEAR REACTIONS 12,13C, 90Zr, 208Pb(π+, π+p), (π+, π-p), E=500 MeV; measured σ(DCX)/σ(NCX); deduced nuclear wave function Δ+ components.

doi: 10.1016/S0370-2693(97)01453-6
Citations: PlumX Metrics


1998PA31      Acta Phys.Pol. B29, 2335 (1998)

E.A.Pasyuk, C.L.Morris, J.L.Ullman, J.D.Zumbro, L.W.Kwok, J.L.Matthews, Y.Tan

A Search for Δ- and Δ++ Wave-Function Components in Light Nuclei using the (π+, π-p) and (n, 2p) Reactions

NUCLEAR REACTIONS 3H, 4He, 6,7Li(π+, π-p), (π+, π+p), E=500 MeV; 3He(n, 2p), E=200-500 MeV; measured pion, proton spectra. 3H, 4He, 6,7Li deduced Δ wavefunction components.


1997SC23      Phys.Rev. C56, 1687 (1997)

W.M.Schmitt, W.Turchinetz, C.F.Williamson, T.C.Yates, J.D.Zumbro, K.S.Lee, H.Baghaei, S.Churchwell, R.S.Hicks, R.Miskimen, G.A.Peterson, K.Wang, P.E.Bosted, M.Spengos, B.Frois, J.Martino, S.Platchkov, A.Hotta

Deuteron Threshold Electrodisintegration at High Momentum Transfer

NUCLEAR REACTIONS 2H(e, e'), E=347, 576, 754, 820, 913 MeV; measured electron spectra; deduced electrodisintegration absolute σ(E, θ), meson exchange current role. Several models compared.

doi: 10.1103/PhysRevC.56.1687
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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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1995SI01      Phys.Rev. C51, 665 (1995)

J.D.Silk, M.Burlein, H.T.Fortune, E.Insko, M.Kagarlis, P.H.Kutt, J.M.O'Donnell, J.D.Zumbro, J.A.Faucett, R.Garnett, M.W.Rawool-Sullivan, C.L.Morris, S.Saini

Nonanalog 40,44Ca(π+, π-)40,44Ti(g.s.) Reactions at Low Energy

NUCLEAR REACTIONS 40,44Ca(π+, π-), E=32-79.26 MeV; measured σ(θ); deduced core polarization, cross shell transitions role.

doi: 10.1103/PhysRevC.51.665
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1994GI09      Nucl.Phys. A577, 227c (1994)

R.Gilman, E.Brash, G.Edwards, C.Glashausser, M.K.Jones, F.T.Baker, S.Bastea, D.P.Beatty, L.Bimbot, J.Brusoe, J.Chiba, D.Cooper, G.Kumbartzki, C.Mauger, T.Nagae, B.Park, D.Prout, R.D.Ransome, M.Rawool-Sullivan, P.Rutt, B.Storm, E.Sugarbaker, T.Taddeucci, J.Zumbro

Coherent Pion Production in 12C(p, nπ) at 800 MeV

NUCLEAR REACTIONS 12C(p, nπ+), E=800 MeV; measured neutron, pion spectra.

doi: 10.1016/0375-9474(94)90860-5
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1994HU02      Phys.Rev. C49, 83 (1994)

P.Hui, H.T.Fortune, R.Gilman, C.M.Laymon, J.D.Zumbro, P.A.Seidl, J.A.Faucett

Pion Double Charge Exchange on (nat)Se

NUCLEAR REACTIONS Se(π+, π-), E=132-294 MeV; measured spectra, σ(θ) vs E; deduced double IAS excitation evidence.

doi: 10.1103/PhysRevC.49.83
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1993JO01      Phys.Rev. C47, 110 (1993)

C.E.Jones, E.J.Beise, J.E.Belz, R.W.Carr, B.W.Filippone, W.Lorenzon, R.D.McKeown, B.A.Mueller, T.G.O'Neill, G.W.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.F.van den Brand, A.Young, X.Yu, J.D.Zumbro

3He(pol)(e(pol), e') Quasielastic Asymmetry

NUCLEAR REACTIONS 3He(polarized e, e'), E=574 MeV; measured spin-dependent asymmetry. Model comparison. Longitudinal beam polarization, polarized target.

doi: 10.1103/PhysRevC.47.110
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1993JO11      Phys.Rev. C48, 2800 (1993)

M.K.Jones, R.D.Ransome, V.R.Cupps, R.W.Fergerson, C.L.Morris, J.A.McGill, J.D.Zumbro, J.R.Comfort, B.G.Ritchie, J.R.Tinsley, P.C.Gugelot, C.F.Moore

Pion Absorption Above the Δ(1232) Resonance

NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 118Sn, 208Pb(π+, xp), E=250-500 MeV; measured σ vs missing energy for x=2, 3; deduced total absorption σ.

doi: 10.1103/PhysRevC.48.2800
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1993MO27      Acta Phys.Pol. B24, 1659 (1993)

C.L.Morris, J.M.O'Donnell, J.D.Zumbro

Pion Scattering at Energies Above the Δ Resonance

NUCLEAR REACTIONS 12C(π+, π+), (π-, π-), E=180-673 MeV; analyzed σ(θ). 12C, 208Pb(π+, π+X), (π-, π-X), E=500 MeV; compiled, reviewed data, analyses; deduced virtual Δ-components measuring possibility.


1993WI15      Phys.Rev. C48, 1840 (1993)

J.E.Wise, M.R.Braunstein, S.Hoibraten, M.D.Kohler, B.J.Kriss, J.Ouyang, R.J.Peterson, J.A.McGill, C.L.Morris, S.J.Seestrom, R.M.Whitton, J.D.Zumbro, C.M.Edwards, A.L.Williams

Quasifree Pion Scattering at 500 MeV

NUCLEAR REACTIONS C(π+, π+), (π-, π-), E=500 MeV; measured σ(θ) vs energy loss, σ(θ). Ca, Zr, Pb(π+, π+), (π-, π-), E=500 MeV; measured σ(θ); deduced surface single nucleon knockout evidence.

doi: 10.1103/PhysRevC.48.1840
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1993ZU01      Phys.Rev.Lett. 71, 1796 (1993)

J.D.Zumbro, C.L.Morris, J.A.McGill, S.J.Seestrom, R.M.Whitton, C.M.Edwards, A.L.Williams, M.R.Braunstein, M.D.Kohler, B.J.Kriss, S.Hoibraten, R.J.Peterson, J.Ouyang, J.E.Wise, W.R.Gibbs

Inclusive Scattering of 500-MeV Pions from Carbon

NUCLEAR REACTIONS C(π+, π+X), (π-, π-X), E=500 MeV; measured inclusive σ(θ, E(π)); deduced comparison with (e, e'X).

doi: 10.1103/PhysRevLett.71.1796
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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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1992HO08      Phys.Rev. C46, 499 (1992)

D.J.Horen, C.L.Morris, S.J.Seestrom, F.W.Hersman, J.R.Calarco, M.Holtrop, M.Leuschner, M.Rawool-Sullivan, R.W.Garnett, S.J.Greene, M.A.Plum, J.D.Zumbro

Isospin Character of the Transition to the 0.803-MeV State in 206Pb from π± Scattering at 180 MeV

NUCLEAR REACTIONS 206Pb(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured missing mass spectra, σ(θ). 206Pb deduced neutron, proton matrix elements ratio for quadrupole, octupole transitions. Deformed optical model, DWIA analyses.

doi: 10.1103/PhysRevC.46.499
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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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1992OD01      Phys.Rev. C46, 2259 (1992)

J.M.O'Donnell, H.T.Fortune, J.D.Silk, S.Mordechai, C.L.Morris, J.D.Zumbro, S.H.Yoo, C.F.Moore

T = 13 Double Isobaric Analog State in 138Ce via Pion-Induced Double Charge Exchange

NUCLEAR REACTIONS 138Ba(π+, π-), E=292 MeV; measured pion spectra, σ(θ); deduced Q. 138Ce deduced double IAS excitation. Systematics, isobaric multiplet mass equation comparisons.

doi: 10.1103/PhysRevC.46.2259
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1992RA01      Phys.Rev. C45, R509 (1992)

R.D.Ransome, C.L.Morris, V.R.Cupps, R.W.Fergerson, J.A.McGill, D.L.Watson, J.D.Zumbro, B.G.Ritchie, J.R.Comfort, J.R.Tinsley, R.A.Loveman, S.Dawson, A.Green, P.C.Gugelot, C.F.Moore

Pion Absorption in Heavy Nuclei

NUCLEAR REACTIONS 6Li, 12C, 27Al, 58Ni, 118Sn, 208Pb, 238U(π+, xp), (π+, d), E=50-200 MeV; measured σ vs missing energy; deduced pion absorption mechanism. Large solid angle bismuth germanate detector array.

doi: 10.1103/PhysRevC.45.R509
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1992TH03      Phys.Rev.Lett. 68, 2901 (1992); Erratum Phys.Rev.Lett. 69, 391 (1992)

A.K.Thompson, A.M.Bernstein, T.E.Chupp, D.J.De Angelis, G.E.Dodge, G.Dodson, K.A.Dow, M.Farkhondeh, W.Fong, J.Y.Kim, R.A.Loveman, J.M.Richardson, H.Schmieden, D.R.Tieger, T.C.Yates, M.E.Wagshul, J.D.Zumbro

Quasielastic Scattering of Polarized Electrons from Polarized 3He and Measurement of the Neutron's Form Factors

NUCLEAR REACTIONS 3He(polarized e, e'), E=578 MeV; measured quasielastic scattering asymmetry; deduced 1n electric form factor implications. Polarized target.

doi: 10.1103/PhysRevLett.68.2901
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1991JO06      Phys.Rev. C44, R571 (1991)

C.E.Jones-Woodward, E.J.Beise, J.E.Belz, R.W.Carr, B.W.Filippone, W.Lorenzon, R.D.McKeown, B.A.Mueller, T.G.O'Neill, G.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.F.J.van den Brand, A.Young, X.Yu, J.D.Zumbro

Determination of the Neutron Electric Form Factor in Quasielastic Scattering of Polarized Electrons from Polarized 3He

NUCLEAR REACTIONS 3He(polarized e, e'), E=574 MeV; measured spin dependent asymmetry. 1n deduced electric form factor. Polarized target.

doi: 10.1103/PhysRevC.44.R571
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1991MI13      Phys.Rev. C44, 1679 (1991)

R.A.Miskimen, H.Baghaei, P.E.Bosted, K.A.Dow, M.Frodyma, B.Frois, R.S.Hicks, A.Hotta, R.L.Huffman, K.S.Lee, J.Martino, G.A.Peterson, S.Platchkov, S.E.Rock, S.H.Rokni, W.Turchinetz, J.D.Zumbro

Elastic Magnetic Electron Scattering from 13C at Q2 = 1 (GeV)2/c2

NUCLEAR REACTIONS 13C(e, e), E not given; measured elastic σ upper limit. 13C deduced M1 form factor high-q enhancement. Shell model.

doi: 10.1103/PhysRevC.44.1679
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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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1991WA04      Phys.Rev. C43, 1318 (1991)

D.L.Watson, R.Gilman, C.L.Morris, J.D.Zumbro, S.Mordechai, M.Burlein, J.M.O'Donnell, H.T.Fortune, A.Kotwal, J.Puttz, J.D.Silk, J.S.McDonald, C.F.Moore, A.L.Williams, S.Y.Yoo

Pion-Induced Double Charge Exchange on 12C, 24Mg, 32S, and 40Ca

NUCLEAR REACTIONS 12C, 24Mg, 32S, 40Ca(π+, π-), E=164 MeV; measured σ(θ). Isobar-nucleon interaction mechanism.

doi: 10.1103/PhysRevC.43.1318
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1991WO02      Nucl.Phys. A527, 367c (1991)

C.Woodward, E.Beise, J.E.Belz, R.Carr, B.Filippone, W.Lorenzon, R.McKeown, B.Mueller, T.O'Neill, G.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.van den Brand, A.Young, X.Yu, J.Zumbro

Measurement of Inclusive Quasielastic Scattering of Polarized Electrons from Polarized 3He

NUCLEAR REACTIONS 3He(polarized e, e), E=574 MeV; measured asymmetry, quasielastic scattering. Polarized target, longitudinal beam polarization.

doi: 10.1016/0375-9474(91)90126-Q
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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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1990KU08      Nucl.Phys. A514, 589 (1990)

R.Kunselman, J.D.Zumbro, E.B.Shera, M.V.Hoehn

Pionic-Atom 3d2p X-Ray Measurements in 54,56Fe, 59Co, and 58,60,61,62,64Ni

ATOMIC PHYSICS, Mesic-Atoms 54,56Fe, 59Co, 58,60,61,62,64Ni; measured 3d-2p pionic X-rays, isotope shifts, strong-interaction shifts, widths.

NUCLEAR MOMENTS 54,56Fe, 59Co, 58,60,61,62,64Ni; measured 3d-2p pionic X-rays, isotope shifts, strong-interaction shifts, widths.

doi: 10.1016/0375-9474(90)90011-A
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1990RA05      Phys.Rev.Lett. 64, 372 (1990)

R.D.Ransome, V.R.Cupps, S.Dawson, R.W.Fergerson, A.Green, C.L.Morris, J.A.McGill, J.R.Comfort, B.G.Ritchie, J.Tinsley, J.D.Zumbro, R.A.Loveman, P.C.Gugelot, D.L.Watson, C.F.Moore

Charged-Particle Multiplicities following Pion Absorption on 6Li

NUCLEAR REACTIONS 6Li(π+, X), E=150 MeV; measured charged particle spectra following pion absorption; deduced multi-proton emission σ.

doi: 10.1103/PhysRevLett.64.372
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1990RA20      Phys.Rev. C42, 1500 (1990)

R.D.Ransome, V.R.Cupps, S.Dawson, R.W.Fergerson, A.Green, C.L.Morris, J.A.McGill, J.R.Comfort, B.G.Ritchie, J.R.Tinsley, J.D.Zumbro, R.A.Loveman, P.C.Gugelot, D.L.Watson, C.F.Moore

Systematics of Pion Absorption on 6Li

NUCLEAR REACTIONS 6Li(π+, 2pX), E=50-200 MeV; measured missing energy distributions, σ(θ) for 2p, 2pn, 3p, 2pd final states; deduced pion absorption mechanism.

doi: 10.1103/PhysRevC.42.1500
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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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1990WO06      Phys.Rev.Lett. 65, 698 (1990)

C.E.Woodward, E.J.Beise, J.E.Belz, R.W.Carr, B.W.Filippone, W.B.Lorenzon, R.D.McKeown, B.Mueller, T.G.O'Neill, G.Dodson, K.Dow, M.Farkhondeh, S.Kowalski, K.Lee, N.Makins, R.Milner, A.Thompson, D.Tieger, J.van den Brand, A.Young, X.Xu, J.D.Zumbro

Measurement of Inclusive Quasielastic Scattering of Polarized Electrons from Polarized 3He

NUCLEAR REACTIONS 3He(polarized e, e'X), E at 462 MeV/c; measured asymmetry. Faddeev calculations, polarized target.

doi: 10.1103/PhysRevLett.65.698
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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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1988AS04      Phys.Lett. 215B, 41 (1988)

D.Ashery, J.Lichtenstadt, E.Piasetzky, C.L.Morris, J.D.Zumbro, R.Gilman, M.W.Rawool, S.Mordechai, B.Boyer, A.Fuentes, K.Johnson, J.W.McDonald, M.J.Smithson, A.Williams, S.H.Yoo, C.F.Moore

A Search for πNN Bound Systems

NUCLEAR REACTIONS 2H(π+, π-), (π-, π+), E=260 MeV; measured possible (πNN) system mass; deduced σ upper limit.

doi: 10.1016/0370-2693(88)91066-0
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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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1988HU09      Phys.Rev. C37, 2334 (1988)

J.R.Hurd, H.T.Fortune, J.D.Zumbro, C.P.Browne

114Cd from 112Cd(t, p)

NUCLEAR REACTIONS 112Cd(t, p), E=15 MeV; measured σ(Ep), σ(θ). 114Cd deduced levels, J, π, L.

doi: 10.1103/PhysRevC.37.2334
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1262.


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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1988MO15      Phys.Rev.Lett. 61, 531 (1988)

S.Mordechai, N.Auerbach, M.Burlein, H.T.Fortune, S.J.Greene, C.F.Moore, C.L.Morris, J.M.O'Donnell, M.W.Rawool, J.D.Silk, D.L.Watson, S.H.Yoo, J.D.Zumbro

Pion Double Charge Exchange to the Double Dipole Resonance

NUCLEAR REACTIONS 32S(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 32Ar deduced resonances, Γ.

doi: 10.1103/PhysRevLett.61.531
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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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1988SE04      Phys.Rev. C37, 2057 (1988)

S.J.Seestrom-Morris, D.Dehnhard, M.A.Franey, D.B.Holtkamp, C.L.Blilie, C.L.Morris, J.D.Zumbro, H.T.Fortune

Pion Inelastic Scattering to the Three Lowest 2+ States of 18O

NUCLEAR REACTIONS 18O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ). 18O levels deduced matrix elements, transition densities. Gas Target. DWIA analysis.

doi: 10.1103/PhysRevC.37.2057
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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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1987FO04      Phys.Rev. C35, 1151 (1987)

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

Double Charge Exchange on 56Fe

NUCLEAR REACTIONS 56Fe(π+, π-), E=80, 100, 120, 180, 230, 292 MeV; measured σ(E, θ), θ=5°. Natural target. Model calculations.

doi: 10.1103/PhysRevC.35.1151
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1987FO06      Phys.Rev. C35, 1603 (1987)

H.T.Fortune, C.Ogilvie, R.Gilman, J.D.Zumbro, D.L.Watson, M.J.Smithson, M.D.Cohler, A.Ghazarian, R.Wadsworth, J.O'Donnell

No Two-Proton Strength to 72Ge (02+)

NUCLEAR REACTIONS 70Zn(16O, 14C), E=110 MeV; measured σ(E(14C)). 72Ge level deduced no two-proton strength.

doi: 10.1103/PhysRevC.35.1603
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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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1987ME19      Phys.Rev. C36, 1785 (1987)

L.R.Medsker, H.T.Fortune, J.D.Zumbro, C.P.Browne, J.F.Mateja

112Cd from 110Cd(t, p)

NUCLEAR REACTIONS, MECPD 110Cd(t, p), E=15 MeV; measured σ(θ), σ(Et); deduced model parameters. 112Cd deduced levels, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.36.1785
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1987MO07      Phys.Rev. C35, 1388 (1987)

C.L.Morris, S.J.Seestrom-Morris, D.Dehnhard, C.L.Blilie, R.Gilman, G.P.Gilfoyle, J.D.Zumbro, M.G.Burlein, S.Mordechai, H.T.Fortune, L.C.Bland, M.Brown, D.P.Saunders, P.A.Seidl, C.F.Moore, K.Maeda, G.S.Blanpied, B.A.Brown

Neutron and Proton Matrix Elements for 2+1 Transitions in T = 1 Nuclei from Pion Inelastic Scattering

NUCLEAR REACTIONS 18O, 22Ne, 26Mg, 30Si, 34S(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ). 18O, 22Ne, 26Mg, 30Si, 34S transitions deduced neutron, proton quadrupole matrix elements. DWIA analysis.

doi: 10.1103/PhysRevC.35.1388
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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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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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1986ZU01      Phys.Lett. 167B, 383 (1986)

J.D.Zumbro, R.A.Naumann, M.V.Hoehn, W.Reuter, E.B.Shera, C.E.Bemis, Jr., Y.Tanaka

E2 and E4 Deformations in 232Th and 239,240,242Pu

NUCLEAR MOMENTS 232Th, 239,240,242Pu; measured muonic X-ray data; deduced quadrupole, hexadecapole moments, charge parameters, rms radii. 239Pu deduced E2 martix elements. Adiabatic rotation model.

ATOMIC PHYSICS, Mesic-Atoms 232Th, 239,240,242Pu; measured muonic X-ray data.

doi: 10.1016/0370-2693(86)91285-2
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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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1985JO04      Phys.Lett. 161B, 75 (1985)

M.W.Johnson, E.B.Shera, M.V.Hoehn, R.A.Naumann, J.D.Zumbro, C.E.Bemis, Jr.

241Am and 243Am Charge Distributions from Muonic X-Ray Spectroscopy and the Quadrupole Moment of the 240Am Fission Isomer

NUCLEAR REACTIONS 241,243Am(μ-, X), E at rest; measured muonic E X-ray, I X-ray. 241,243Am deduced intrinsic quadrupole moment, Barrett radii. 240Am deduced fission isomer quadrupole moment. Optical isotope shift data input.

ATOMIC PHYSICS, Mesic-Atoms 241,243Am(μ, X), E at rest; measured muonic X-rays.

doi: 10.1016/0370-2693(85)90612-4
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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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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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1984TA04      Phys.Rev. C29, 1830 (1984)

Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro

Systematics of Ground-State Quadrupole Moments of Odd-A Deformed Nuclei Determined with Muonic M X Rays

NUCLEAR MOMENTS 151,153Eu, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic hfs, E(M X-ray), I(M X-ray); deduced ground state quadrupole moments, β2. 151,153Eu deduced large deformation change.

ATOMIC PHYSICS, Mesic-Atoms 151,153Eu, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic hfs, E(M X-ray), I(M X-ray); deduced implication on Steinheimer correction factors.

doi: 10.1103/PhysRevC.29.1830
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1984TA05      Phys.Rev. C29, 1897 (1984)

Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro

Measurement and Analysis of the Muonic X Rays of 151Eu and 153Eu

ATOMIC PHYSICS, Mesic-Atoms 151,153Eu; measured muonic E(K X-ray), I(K X-ray), E(L X-ray), I(L X-ray); deduced isotope, isomer shifts, monopole, quadrupole charge parameters.

NUCLEAR MOMENTS 151,153Eu; measured muonic X-rays; deduced isotope, isomer shifts, monopole, quadrupole charge parameters. 151,153Eu levels deduced quadrupole moments, B(E2).

doi: 10.1103/PhysRevC.29.1897
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1984TA10      Phys.Rev. C30, 350 (1984)

T.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro

Measurement and Analysis of Muonic X Rays of 176,177,178,179,180Hf

ATOMIC PHYSICS, Mesic-Atoms 176,177,178,179,180Hf; measured muonic X-rays.

NUCLEAR MOMENTS 176,177,178,179,180Hf; measured muonic E X-ray, I X-ray; deduced monopole, quadrupole charge distributions, isotope shifts, rms radii. 176,177,178,179,180Hf level deduced isomer shift, quadrupole moment, B(E2). Axially symmetric rotor model comparison.

doi: 10.1103/PhysRevC.30.350
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1984TA16      Phys.Lett. 143B, 347 (1984)

Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro

Pionic M X-Rays of 166,168Er and 176Hf

NUCLEAR REACTIONS 166,168Er, 176Hf(π, X), E at rest; measured M X-rays.

ATOMIC PHYSICS, Mesic-Atoms 166,168Er, 176Hf; measured pionic X-rays; deduced strong interaction shifts, widths.

doi: 10.1016/0370-2693(84)91480-1
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1984ZU02      Phys.Rev.Lett. 53, 1888 (1984)

J.D.Zumbro, E.B.Shera, Y.Tanaka, C.E.Bemis, Jr., R.A.Naumann, M.V.Hoehn, W.Reuter, R.M.Steffen

E2 and E4 Deformations in 233,234,235,238U

NUCLEAR MOMENTS 233,234,235,238U; measured muonic X-rays. 234,238U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, rms radii. 233,235U deduced intrinsic quadrupole, hexadecapole moments, charge distribution parameters, B(E2).

ATOMIC PHYSICS, Mesic-Atoms 233,234,235,238U; measured muonic X-rays.

doi: 10.1103/PhysRevLett.53.1888
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1983TA14      Phys.Rev.Lett. 51, 1633 (1983)

Y.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro

Precision Muonic-Atom Measurements of Nuclear Quadrupole Moments and the Sternheimer Effect in Rare-Earth Atoms

ATOMIC PHYSICS, Mesic-Atoms 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic X-rays, hfs; deduced 4f, 5d, 6p electronic state Sternheimer shielding factors.

NUCLEAR MOMENTS 151,153Eu, 155,157Gd, 159Tb, 163Dy, 167Er, 177,179Hf, 191,193Ir; measured muonic X-rays, hfs; deduced quadrupole moments.

doi: 10.1103/PhysRevLett.51.1633
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1983ZU01      Nucl.Phys. A393, 15 (1983)

J.D.Zumbro, R.W.Tarara, C.P.Browne

Study of the Levels of 77,79,81,83Br with the 76,78,80,82Se(3He, d) Reaction

NUCLEAR REACTIONS 76,78,80Se(3He, d), E=24 MeV; measured σ(Ed, θ). 82Se(3He, d), E=24 MeV; measured σ(Ed, θ), Q. 77,79,81,83Br levels deduced L, J, π, S. Enriched targets, magnetic spectrograph.

doi: 10.1016/0375-9474(83)90062-3
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1982ZU02      Phys.Rev. C26, 965 (1982)

J.D.Zumbro, C.P.Browne, J.F.Mateja, H.T.Fortune, R.Middleton

176Yb(t, p)178Yb Reaction

NUCLEAR REACTIONS 176Yb(t, p), E=15 MeV; measured σ(Ep), σ(θ); deduced Q. 178Yb deduced levels, L, J, π, band structure. Magnetic spectrograph. DWBA analysis.

doi: 10.1103/PhysRevC.26.965
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1982ZU04      Phys.Rev. C26, 2668 (1982)

J.D.Zumbro, A.A.Rollefson, R.W.Tarara, C.P.Browne

Q Values for Proton- and Deuteron-Induced Reactions on Selenium Targets

NUCLEAR REACTIONS 78,80,82Se(p, d), (p, t), 78,80Se(p, α), 80Se(d, p), E=15-16 MeV; measured Q. 82,83Se, 83Br deduced mass decrease. Comparison with mass table evaluation.

doi: 10.1103/PhysRevC.26.2668
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1981MA12      Phys.Rev. C23, 2435 (1981)

J.F.Mateja, L.R.Medsker, C.P.Browne, J.D.Zumbro, H.T.Fortune, R.Middleton, J.B.McGrory

(t, p) Studies of 52Ti, 53V, and 57Mn and Tests of Mixed-Configuration Shell-Model Calculations

NUCLEAR REACTIONS 50Ti, 51V(t, p), E=15 MeV; measured σ(θ, Ep). 52Ti, 53V levels deduced L, J, π, enhancement factors. 55Mn(t, p), E not given; analyzed data. 57Mn levels deduced L, J, π, enhancement factors. Mixed-configuration shell model, DWBA analysis.

doi: 10.1103/PhysRevC.23.2435
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1978MA21      Phys.Rev. C17, 2047 (1978)

J.F.Mateja, L.R.Medsker, H.T.Fortune, R.Middleton, G.E.Moore, M.E.Cobern, S.Mordechai, J.D.Zumbro, C.P.Browne

76Ge(t, p)78Ge Reaction

NUCLEAR REACTIONS 76Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). 78Ge deduced levels, L, J, π. DWBA analysis.

doi: 10.1103/PhysRevC.17.2047
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1978MO12      Nucl.Phys. A305, 29 (1978)

L.A.Montestruque, M.C.Cobian-Rozak, G.Szaloky, J.D.Zumbro, S.E.Darden

Study of the 77,79,81,83Se Level Structure with the 76,78,80,82Se(d, p) Reaction

NUCLEAR REACTIONS 76,78,80,82Se(d, p), E=12.5 MeV; measured σ(Ep, θ), A(Ep, θ); deduced Q. 77,79,81,83Se levels deduced L, J, π, S. Enriched targets.

doi: 10.1016/0375-9474(78)90163-X
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1978TA10      Phys.Rev. C18, 1064 (1978)

R.W.Tarara, J.D.Zumbro, C.P.Browne

Levels in 173Tm via the 176Yb(p, α)173Tm Reaction

NUCLEAR REACTIONS 176Yb(p, α), E=16 MeV; measured σ(Eα, θ); deduced Q. 173Tm deduced levels, L, J, π. Enriched targets, DWBA analysis.

doi: 10.1103/PhysRevC.18.1064
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