NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.J.Greene Found 56 matches. 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
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
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
1994YE06 Phys.Rev. C50, 897 (1994) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, M.A.Franey, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.I.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=130-180 MeV; 13C(π+, π+), E=223 MeV; 13C(π-, π-), E=226 MeV; measured analyzing power A(y)(θ), σ(θ); deduced spin-flip transition quadrupole component role. Polarized, unpolarized target. DWIA calculations, optical, Δ-hole models.
doi: 10.1103/PhysRevC.50.897
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
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
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
1991YE01 Phys.Rev.Lett. 66, 1959 (1991) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.J.Gorgen, B.G.Ritchie, J.R.Tinsley, M.Barlett, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, M.A.Khandaker, S.Chakravarti Asymmetry Measurement of Pion Elastic Scattering from Polarized 13C in the Energy Region of the P33 Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=132-226 MeV; measured analyzing power vs θ. Polarized target.
doi: 10.1103/PhysRevLett.66.1959
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
1990YE06 J.Phys.(Paris), Colloq.C-6, 587 (1990) Y.-F.Yen, B.Brinkmoller, D.Dehnhard, S.M.Sterbenz, Y.-J.Yu, B.Berman, G.R.Burleson, K.Cranston, A.Klein, G.S.Kyle, R.Alarcon, T.Averett, J.R.Comfort, J.Gorgen, B.Ritchie, J.R.Tinsley, G.W.Hoffmann, K.Johnson, C.F.Moore, M.Purcell, H.Ward, A.Williams, J.A.Faucett, S.J.Greene, J.Jarmer, J.A.McGill, C.L.Morris, S.Penttila, N.Tanaka, H.T.Fortune, E.Insko, R.Ivie, J.M.O'Donnell, D.Smith, S.Hoibraten, M.Khandaker, S.Chakravarti Pion Elastic Scattering from Polarized 13C in the Energy Region of the [3, 3] Resonance NUCLEAR REACTIONS 13C(π+, π+), (π-, π-), E=114-226 MeV; measured analyzing power vs θ. Polarized target. DWIA analyses.
1988AD02 Nucl.Phys. A480, 530 (1988) D.L.Adams, B.Aas, E.Bleszynski, M.Bleszynski, G.Igo, C.Newsom, Y.Ohashi, G.Pauletta, F.Sperisen, C.A.Whitten, Jr., H.Fujisawa, M.Gazzaly, S.J.Greene, K.Jones, J.B.McClelland, N.Tanaka, H.Hasai, K.Iwatani, S.Ishimoto, S.Isagawa, A.Masaike, A.Okihana, S.Okumi Spin Observables in Small-Angle Elastic p(pol)d(pol) → p(pol)d Scattering with an L-Type Deuteron Target at 800 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=800 MeV; measured analyzing powers, spin transfer coefficients. Polarized target.
doi: 10.1016/0375-9474(88)90462-9
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
1988HA14 Phys.Rev. C37, 1554 (1988) A.C.Hayes, S.Chakravarti, D.Dehnhard, P.J.Ellis, D.B.Holtkamp, L.-P.Lung, S.J.Seestrom-Morris, H.Baer, C.L.Morris, S.J.Greene, C.J.Harvey Structure of the Low-Lying 2+ States in 14C from Inelastic Pion Scattering NUCLEAR STRUCTURE 14C, 14N, 14O; calculated levels, B(λ). Shell model. NUCLEAR REACTIONS 14C(π, π'), E=164 MeV; analyzed σ(θ). 14C level deduced isovector component quenching.
doi: 10.1103/PhysRevC.37.1554
1988IG02 Phys.Rev. C38, 2777 (1988) G.Igo, A.Masaike, B.Aas, D.Adams, E.Bleszynski, M.Bleszynski, M.Gazzaly, S.J.Greene, H.Hasai, S.Ishimoto, S.Isagawa, K.Jones, D.Lopiano, J.B.McClelland, F.Nishiyama, Y.Ohashi, A.Okihana, G.Pauletta, F.Sperisen, T.-H.Sun, N.Tanaka, G.S.Weston, C.A.Whitten, Jr. Spin Observables in Small-Angle Elastic p(pol)d(pol) → p(pol)d with an N-Type Polarized Target at 800 MeV NUCLEAR REACTIONS 2H(polarized p, p), E=800 MeV; measured polarization observables; deduced nucleon-nucleon amplitude ambiguities. N-type polarized, fully deuterated propanediol target.
doi: 10.1103/PhysRevC.38.2777
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
1988OA03 Phys.Rev. C38, 2978 (1988) D.S.Oakley, R.J.Peterson, D.J.Rilett, C.L.Morris, S.J.Greene, B.Boyer, K.Johnson, A.H.Fuentes, J.W.McDonald, M.J.Smithson, A.L.Williams, S.H.Yoo, C.F.Moore Energy Dependence of Pion Inelastic Scattering to the 1+ States in 12C NUCLEAR REACTIONS 12C(π-, π-'), (π+, π+'), E=80-295 MeV; measured σ(θ); deduced isobar excitation role. 12C levels deduced σ ratio.
doi: 10.1103/PhysRevC.38.2978
1988ZE01 Phys.Rev. C38, 2251 (1988) B.Zeidman, D.F.Geesaman, P.Zupranski, R.E.Segel, G.C.Morrison, C.Olmer, G.R.Burleson, S.J.Greene, R.L.Boudrie, C.L.Morris, L.W.Swenson, G.S.Blanpied, B.G.Ritchie, C.L.H.Johnstone Inelastic Scattering of Pions by 10B NUCLEAR REACTIONS 10B(π+, π+), (π+, π+'), E=162 MeV; measured σ(θ). 10B deduced levels, J, π, stretched configurations, B(λ).
doi: 10.1103/PhysRevC.38.2251
1987CO17 Phys.Rev. C36, 230 (1987) W.B.Cottingame, K.G.Boyer, W.J.Braithwaite, S.J.Greene, C.J.Harvey, R.J.Joseph, D.B.Holtkamp, C.F.Moore, J.J.Kraushaar, R.J.Peterson, R.A.Ristinen, J.R.Shepard, G.R.Smith, R.L.Boudrie, N.S.P.King, C.L.Morris, J.Piffaretti, H.A.Thiessen Inelastic Pion Scattering from 12C NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=100-291 MeV; measured σ(θ); deduced σ. 12C levels deduced isospin mixing effects. DWIA analysis.
doi: 10.1103/PhysRevC.36.230
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
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
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
1985GI01 Nucl.Phys. A432, 610 (1985) R.Gilman, L.C.Bland, P.A.Seidl, C.F.Moore, C.L.Morris, S.J.Greene, H.T.Fortune Two-Amplitude Model of Pion DCX Applied to the 18O Angular Distribution and Excitation Function NUCLEAR REACTIONS 16O(π+, π-), E=164 MeV; analyzed σ(θ). Two-amplitude model fit.
doi: 10.1016/0375-9474(85)90003-X
1985HO07 Phys.Rev. C31, 957 (1985); Erratum Phys.Rev. C41, 1319 (1990) D.B.Holtkamp, S.J.Seestrom-Morris, D.Dehnhard, H.W.Baer, C.L.Morris, S.J.Greene, C.J.Harvey, D.Kurath, J.A.Carr Pion Scattering to 4- States in 14C NUCLEAR REACTIONS 14C(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ), σ(E(π)). 14C deduced levels, J, π, neutron, proton amplitudes, ratios. DWIA, shell model wave functions.
doi: 10.1103/PhysRevC.31.957
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
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
1984AU04 Phys.Rev. D29, 2435 (1984) I.P.Auer, W.R.Ditzler, D.Hill, K.Imai, H.Spinka, R.Stanek, K.Toshioka, D.Underwood, R.Wagner, A.Yokosawa, E.W.Hoffman, J.J.Jarmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, S.Stuart Measurement of Δσ(L) and C(LL)=(L, L;0, 0) in Proton-Proton Scattering between 300 and 800 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=300-800 MeV; measured total σ dependence on spin correlation parameter; deduced resonance structure in 1D2, 3F3 partial waves.
doi: 10.1103/PhysRevD.29.2435
1984BL12 Phys.Lett. 144B, 328 (1984) L.C.Bland, R.Gilman, G.S.Stephans, G.P.Gilfoyle, H.T.Fortune, C.L.Morris, S.J.Seestrom-Morris, S.J.Greene, P.A.Seidl, R.R.Kiziah, C.F.Moore Forward-Peaked Angular Distributions Observed in (π, π') on Light Nuclei NUCLEAR REACTIONS 12C(π+, π+'), E=170 MeV; 28Si(π+, π+'), E=162 MeV; calculated σ(θ, E(π)). 12C, 28Si deduced resonances, Γ, possible multipole character.
doi: 10.1016/0370-2693(84)91271-1
1984BO02 Phys.Rev. C29, 182 (1984) K.G.Boyer, W.J.Braithwaite, W.B.Cottingame, S.J.Greene, L.E.Smith, C.F.Moore, C.L.Morris, H.A.Thiessen, G.S.Blanpied, G.R.Burleson, J.F.Davis, J.S.McCarthy, R.C.Minehart, C.A.Goulding Pion Elastic and Inelastic Scattering from 40,42,44,48Ca and 54Fe NUCLEAR REACTIONS 40,42,44,48Ca, 54Fe(π+, π+'), (π-, π-'), E=116, 118, 292.5 MeV; measured σ(E(π)), σ(θ). 40,42,44,48Ca, 54Fe level deduced neutron density rms radii. DWIA analysis.
doi: 10.1103/PhysRevC.29.182
1984GE06 Phys.Rev. C30, 952 (1984) D.F.Geesaman, R.D.Lawson, B.Zeidman, G.C.Morrison, A.D.Bacher, C.Olmer, G.R.Burleson, W.B.Cottingame, S.J.Greene, R.L.Boudrie, C.L.Morris, R.A.Lindgren, W.H.Kelly, R.E.Segel, L.W.Swenson Quenching of Isoscalar Spin-Flip Strength in 54Fe NUCLEAR REACTIONS 54Fe(π+, π+'), (π-, π-'), E=162 MeV; measured σ(θ), σ(E(π)). 54Fe levels deduced isoscalar, isovector strengths.
doi: 10.1103/PhysRevC.30.952
1984GR27 Phys.Rev. C30, 2003 (1984) S.J.Greene, C.J.Harvey, P.A.Seidl, R.Gilman, E.R.Siciliano, M.B.Johnson Unified Analysis of Pion Single- and Double-Charge-Exchange Scattering in the Resonance Region NUCLEAR REACTIONS 16O, 28Si, 40Ca, 14,12C(π+, π+), (π-, π-), E=164 MeV; 14C, 18O, 24Mg(π+, π0), E=164 MeV; 13C, 15N(π+, π-), E=165 MeV; calculated σ(θ). 7Li, 13,14C, 15N, 18O, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π-), E=165 MeV; 14C, 18O, 26Mg, 42,48Ca, 56Fe, 90Zr(π+, π0), E=164 MeV; calculated σ(θ, A); deduced second-order optical model parameters. Phenomenological analysis.
doi: 10.1103/PhysRevC.30.2003
1984KI16 Phys.Rev. C30, 1643 (1984) R.R.Kiziah, M.D.Brown, C.J.Harvey, D.S.Oakley, D.P.Saunders, P.A.Seidl, C.F.Moore, W.B.Cottingame, R.W.Garnett, S.J.Greene, G.A.Luna, G.R.Burleson, D.B.Holtkamp Pion Inelastic Scattering to the Low-Lying Excited States of 6Li NUCLEAR REACTIONS 6Li(π+, π+), (π+, π+'), E=100-260 MeV; measured σ(θ); deduced reaction mechanism. 6Li levels deduced form factors. DWIA analysis.
doi: 10.1103/PhysRevC.30.1643
1984SE14 Phys.Rev. C30, 973 (1984) P.A.Seidl, M.D.Brown, R.R.Kiziah, C.F.Moore, H.Baer, C.L.Morris, G.R.Burleson, W.B.Cottingame, S.J.Greene, L.C.Bland, R.Gilman, H.T.Fortune Pion Double Charge Exchange on T = 1 Nuclei NUCLEAR REACTIONS 26Mg(π+, π-), E=164 MeV; 14C(π+, π-), E=164, 292 MeV; measured missing mass spectra, σ(θ); deduced double charge exchange mass dependence. Other data input.
doi: 10.1103/PhysRevC.30.973
1984SE15 Phys.Rev. C30, 1076 (1984) P.A.Seidl, M.D.Brown, R.R.Kiziah, C.F.Moore, H.Baer, C.L.Morris, G.R.Burleson, W.B.Cottingame, S.J.Greene, L.C.Bland, R.Gilman, H.T.Fortune 13C(π+, π-)13O near the Δ33 Resonance NUCLEAR REACTIONS 13C(π+, π-), E=164, 292 MeV; measured σ(E(π), θ), missing mass spectra.
doi: 10.1103/PhysRevC.30.1076
1983BL08 Phys.Lett. 128B, 157 (1983) L.C.Bland, R.Gilman, M.Carchidi, K.Dhuga, C.L.Morris, H.T.Fortune, S.J.Greene, P.A.Seidl, C.F.Moore Systematics of Pion Double-Charge-Exchange Reactions on T = 0 Nuclei NUCLEAR REACTIONS 12C, 24Mg, 28Si, 32S, 40Ca(π+, π-), E=120-210 MeV; measured σ(θ=5°) vs E; deduced charge exchange reaction systematics.
doi: 10.1016/0370-2693(83)90380-5
1983BU05 Nucl.Phys. B213, 365 (1983) G.R.Burleson, W.B.Cottingame, S.J.Greene, S.Stuart, E.W.Hoffman, J.J.Jarmer, I.P.Auer, W.R.Ditzler, D.Hill, K.Imai, H.Spinka, R.Stanek, K.Toshioka, D.Underwood, R.Wagner, A.Yokosawa C(LL) = (L, L;0, 0) Measurements and a Structure due to a P Partial Wave in the pp System NUCLEAR REACTIONS 1H(polarized p, p), E=300-800 MeV; measured σ(θ), spin correlation parameter vs θ, E; deduced amplitudes.
doi: 10.1016/0550-3213(83)90226-2
1983DI02 Phys.Rev. D27, 680 (1983) W.R.Ditzler, D.Hill, K.Imai, H.Shimizu, H.Spinka, R.Stanek, K.Toshioka, D.Underwood, R.Wagner, A.Yokosawa, G.R.Burleson, W.B.Cottingame, S.J.Greene, J.J.Jarmer, R.H.Jeppesen Measurement of the Difference in pp Total Cross Sections for Pure Parallel and Antiparallel Transverse-Spin State (Δσ(T)) at T(p) = 487, 639, and 791 MeV NUCLEAR REACTIONS 1H(polarized p, p), E=487, 639, 791 MeV; measured transverse spin state σ(total) difference. Polarized frozen spin target.
doi: 10.1103/PhysRevD.27.680
1983GR07 Phys.Rev. C27, 2375 (1983) S.J.Greene, W.B.Cottingame, G.R.Burleson, L.C.Bland, R.Gilman, H.T.Fortune, C.L.Morris, D.B.Holtkamp, C.F.Moore Diffractive Angular Distribution for 16O(π+, π-)16Ne(g.s.) NUCLEAR REACTIONS 16O(π+, π-), E=164 MeV; measured σ(θ). 16Ne deduced nonanalog transition characteristics. Eikonal fit.
doi: 10.1103/PhysRevC.27.2375
1983MO18 Phys.Rev. C28, 2165 (1983) C.L.Morris, S.J.Seestrom-Morris, P.A.Seidl, R.R.Kiziah, S.J.Greene Pion Elastic and Inelastic Scattering from 152Sm NUCLEAR REACTIONS 152Sm(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ). 152Sm level deduced deformation parameters β2(p), β2(n) equality. DWIA, coupled-channels.
doi: 10.1103/PhysRevC.28.2165
1983SE06 Phys.Rev.Lett. 50, 1106 (1983) P.A.Seidl, R.R.Kiziah, M.K.Brown, C.F.Moore, C.L.Morris, H.Baer, S.J.Greene, G.R.Burleson, W.B.Cottingame, L.C.Bland, R.Gilman, H.T.Fortune Observation of Analog and Nonanalog Transitions in the Reaction 56Fe(π+, π-)56Ni NUCLEAR REACTIONS 56Fe(π+, π-), E=140-290 MeV; measured σ(E(π-)), σ(θ) vs E; deduced analog, nonanalog transition mass dependence. 56Ni deduced double analog, nonanalog transition relative strengths.
doi: 10.1103/PhysRevLett.50.1106
1982BL20 J.Phys.(London) G8, L173 (1982) L.C.Bland, H.T.Fortune, S.J.Greene, C.F.Moore, C.L.Morris Energy Dependence of Pion-Induced Isotensor Double Charge Exchange NUCLEAR REACTIONS 16O, 24Mg(π+, π-), E=100-292 MeV; measured σ(E). 16Ne, 24Si deduced nonanalog transition, isobar component width. Breit-Wigner analysis, two amplitude model.
doi: 10.1088/0305-4616/8/11/001
1982FO05 Phys.Rev. C25, 2142 (1982); Erratum Phys.Rev. C26, 2337 (1982) H.T.Fortune, S.J.Greene, C.F.Moore, C.L.Morris Pion Double Charge Exchange on Ca Isotopes NUCLEAR REACTIONS 42,44,48Ca(π+, π-), E=164, 292 MeV; calculated σ(θ), σ(total). Two-amplitude model.
doi: 10.1103/PhysRevC.25.2142
1982GR02 Phys.Rev. C25, 924 (1982) S.J.Greene, D.B.Holtkamp, W.B.Cottingame, C.F.Moore, G.R.Burleson, C.L.Morris, H.A.Thiessen, H.T.Fortune Interference Effects in Pion Double Charge Exchange NUCLEAR REACTIONS 16,18O(π+, π-), E=80-292 MeV; measured σ(θ) vs E; deduced direct double analog, two-step nonanalog amplitude interference.
doi: 10.1103/PhysRevC.25.924
1982GR28 Phys.Rev. C 25, 927 (1982) S.J.Greene, W.J.Braithwaite, D.B.Holtkamp, W.B.Cottingame, C.F.Moore, G.R.Burleson, G.S.Blanpied, A.J.Viescas, G.H.Daw, C.L.Morris, H.A.Thiessen Systematics in pion double charge exchange NUCLEAR REACTIONS 9Be, 12,13C, 16,18O, 24,26Mg, 32S, 209Bi(π+, π-), E=100-300 MeV; measured reaction products; deduced σ(θ), systematics. LAMPF meson facility.
doi: 10.1103/PhysRevC.25.927
1982MO01 Phys.Lett. 108B, 172 (1982) C.L.Morris, W.B.Cottingame, S.J.Greene, C.J.Harvey, C.F.Moore, D.B.Holtkamp, S.J.Seestrom-Morris, H.T.Fortune Indication of Δ-Hole Configurations in 12C(15.11 MeV) NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=100, 180, 230 MeV; measured σ(θ, E(π)). 12C level deduced isobar-hole configuration component. DWIA, Cohen-Kurath transition densities, Fermi momentum corrections.
doi: 10.1016/0370-2693(82)91168-6
1982MO12 Phys.Rev. C25, 3218 (1982) C.L.Morris, H.T.Fortune, L.C.Bland, R.Gilman, S.J.Greene, W.B.Cottingame, D.B.Holtkamp, G.R.Burleson, C.F.Moore Target Mass Dependence of Isotensor Double Charge Exchange: Evidence for deltas in nuclei NUCLEAR REACTIONS 16O, 28Si, 40Ca(π+, π-), E=164 MeV; measured σ(E(π-)) at θ=5°; deduced mass dependence of σ, isobar components in wave function. 28S, 40Ti deduced mass excess.
doi: 10.1103/PhysRevC.25.3218
1982MO25 Phys.Rev. C26, 2561 (1982) C.F.Moore, C.J.Harvey, C.L.Morris, W.B.Cottingame, S.J.Greene, D.B.Holtkamp, H.T.Fortune 12C(π, π') to Giant Dipole Resonance Region NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ, E(π)). 12C deduced dominant GDR, spin-flip giant resonance excitation.
doi: 10.1103/PhysRevC.26.2561
1981BL07 Phys.Rev. C23, 2599 (1981) G.S.Blanpied, G.W.Hoffmann, M.L.Barlett, J.A.McGill, S.J.Greene, L.Ray, O.B.Van Dyck, J.Amann, H.A.Thiessen Large Angle Scattering of 0.8 GeV Protons from 12C NUCLEAR REACTIONS 12C(p, p'), E=800 MeV; measured σ(θ). 12C deduced charge density multipole moments M(E2), M(E4). Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.23.2599
1981BO26 Phys.Rev. C24, 598 (1981) K.G.Boyer, W.B.Cottingame, L.E.Smith, S.J.Greene, C.F.Moore, J.S.McCarthy, R.C.Minehart, J.F.Davis, G.R.Burleson, G.Blanpied, C.A.Goulding, H.A.Thiessen, C.L.Morris Pion Inelastic Scattering to the Low-Lying States in 42,44,48Ca: Determination of the neutron and proton multipole matrix elements NUCLEAR REACTIONS 42,44,48Ca(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ). 40,42,48Ca levels deduced neutron, proton multipole matrix elements, M(E2), M(E3). DWIA analysis, collective, microscopic model from factors.
doi: 10.1103/PhysRevC.24.598
1981HO14 Phys.Rev.Lett. 47, 216 (1981) D.B.Holtkamp, S.J.Seestrom-Morris, S.Chakravarti, D.Dehnhard, H.W.Baer, C.L.Morris, S.J.Greene, C.J.Harvey Strong Cancellations of Neutron and Proton Transition Amplitudes Observed in Pion Inelastic Scattering NUCLEAR REACTIONS 14C(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ, E(π)); deduced neutron, proton transition amplitude cancellations. 14C deduced levels, J, π, configuration.
doi: 10.1103/PhysRevLett.47.216
1981MO07 Phys.Lett. 99B, 387 (1981) C.L.Morris, R.L.Boudrie, J.Piffaretti, W.B.Cottingame, W.J.Braithwaite, S.J.Greene, C.J.Harvey, D.B.Holtkamp, C.F.Moore, S.J.Seestrom-Morris Measurements of Isospin Mixing Between the 1+ Doublet in 12C using Pion Inelastic Scattering NUCLEAR REACTIONS 12C(π+, π+'), (π-, π-'), E=100, 116, 130 MeV; measured σ(E(π)); deduced charge dependent matrix element. 12C levels deduced isospin mixing. Model independent method.
doi: 10.1016/0370-2693(81)90554-2
1981MO17 Phys.Rev. C24, 231 (1981) C.L.Morris, K.G.Boyer, C.F.Moore, C.J.Harvey, K.J.Kallianpur, I.B.Moore, P.A.Seidl, S.J.Seestrom-Morris, D.B.Holtkamp, S.J.Greene, W.B.Cottingame Pion Inelastic Scattering to Low-Lying States in 12C and 40Ca NUCLEAR REACTIONS 12C, 40Ca(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ). DWIA analysis.
doi: 10.1103/PhysRevC.24.231
1980BU15 Phys.Rev. C22, 1180 (1980) G.R.Burleson, G.S.Blanpied, G.H.Daw, A.J.Viescas, C.L.Morris, H.A.Thiessen, S.J.Greene, W.J.Braithwaite, W.B.Cottingame, D.B.Holtkamp, I.B.Moore, C.F.Moore Isospin Quintets in the 1p and s-d Shells NUCLEAR REACTIONS 9Be, 12,13C, 16O, 24Mg, 32S(π+, π-), E=180 MeV; measured σ(θ), Q. 12O, 16Ne, 24Si, 32Ar deduced masses. Isobaric multiplet mass equation fit.
doi: 10.1103/PhysRevC.22.1180
1980HO13 Phys.Rev.Lett. 45, 420 (1980) D.R.Holtkamp, W.J.Braithwaite, W.Cottingame, S.J.Greene, R.J.Joseph, C.F.Moore, C.L.Morris, J.Piffaretti, E.R.Siciliano, H.A.Thiessen, D.Dehnhard Isospin Mixing of 4- Particle-Hole States in 16O NUCLEAR REACTIONS 16O(π+, π+'), (π-, π-'), E=164 MeV; measured σ(θ(π), E(π')); deduced off-diagonal charge-dependent matrix elements. 16O levels deduced isospin mixing.
doi: 10.1103/PhysRevLett.45.420
1979GR18 Phys.Lett. 88B, 62 (1979) S.J.Greene, W.J.Braithwaite, D.B.Holtkamp, W.B.Cottingame, C.F.Moore, C.L.Morris, H.A.Thiessen, G.R.Burleson, G.S.Blanpied Studies of the Pion Double-Charge Exchange Reaction 18O(π+, π-)18Ne NUCLEAR REACTIONS 18O(π+, π-), E=292 MeV; measured σ(θ, E(π-)).
doi: 10.1016/0370-2693(79)90114-X
1979MO15 Phys.Lett. 86B, 31 (1979) C.L.Morris, J.Piffaretti, H.A.Thiessen, W.B.Cottingame, W.J.Braithwaite, R.J.Joseph, I.B.Moore, D.B.Holtkamp, C.J.Harvey, S.J.Greene, C.F.Moore, R.L.Boudrie, R.J.Peterson Observation of Isospin Mixing in 12C Near 19.5 MeV Excitation NUCLEAR REACTIONS 12C(π+, π+), (π-, π-'), E=162 MeV; measured σ(Eπ+, θ), σ(Eπ-, θ). 12C deduced isospin mixed doublet near 19.5 MeV.
doi: 10.1016/0370-2693(79)90614-2
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