NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.Zumbro Found 71 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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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