NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.Mordechai Found 96 matches. 2003BO23 Phys.Rev. C 68, 024317 (2003) K.Boretzky, A.Grunschloss, S.Ilievski, P.Adrich, T.Aumann, C.A.Bertulani, J.Cub, W.Dostal, B.Eberlein, Th.W.Elze, H.Emling, M.Fallot, J.Holeczek, R.Holzmann, C.Kozhuharov, J.V.Kratz, R.Kulessa, Y.Leifels, A.Leistenschneider, E.Lubkiewicz, S.Mordechai, T.Ohtsuki, P.Reiter, H.Simon, K.Stelzer, J.Stroth, K.Summerer, A.Surowiec, E.Wajda, W.Walus, and the LAND Collaboration Two-phonon giant resonances in 136Xe, 208Pb, and 238U NUCLEAR REACTIONS C, Sn, 208Pb(136Xe, X), E=700 MeV/nucleon; C, Sn, Ho, Pb, U(208Pb, X), E=640 MeV/nucleon; C, Sn, Pb(238U, X), E=500 MeV/nucleon; measured Eγ, En, σ(E) and σ(θ) for electromagnetic excitation of projectile. 136Xe, 208Pb, 238U deduced two-phonon GDR energies, widths, decay properties.
doi: 10.1103/PhysRevC.68.024317
1999GR24 Phys.Rev. C60, 051601 (1999) A.Grunschloss, K.Boretzky, T.Aumann, C.A.Bertulani, J.Cub, W.Dostal, B.Eberlein, Th.W.Elze, H.Emling, J.Holeczek, R.Holzmann, M.Kaspar, J.V.Kratz, R.Kulessa, Y.Leifels, A.Leistenschneider, E.Lubkiewicz, S.Mordechai, I.Peter, P.Reiter, M.Rejmund, H.Simon, K.Stelzer, A.Surowiec, K.Summerer, J.Stroth, E.Wajda, W.Walus, S.Wan, H.J.Wollersheim Impact-Parameter Dependence of Giant Resonance Excitations in Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS Sn, 208Pb(136Xe, X), E=700 MeV/nucleon; measured Xe fragments angular distribution; deduced sharp-cutoff minimum impact parameters, related reaction mechanism features.
doi: 10.1103/PhysRevC.60.051601
1997KA22 Phys.Rev. C55, 2533 (1997) G.Kahrimanis, G.Burleson, C.M.Chen, B.C.Clark, K.Dhuga, D.J.Ernst, J.A.Faucett, H.T.Fortune, S.Hama, A.Hussein, M.F.Jiang, K.W.Johnson, L.Kurth Kerr, S.Mathews, J.McGill, C.F.Moore, S.Mordechai, C.L.Morris, J.O'Donnell, M.Snell, M.Rawool-Sullivan, L.Ray, C.Whitley, A.L.Williams Pion-Nucleus Elastic Scattering on 12C, 40Ca, 90Zr, and 208Pb at 400 and 500 MeV NUCLEAR REACTIONS 12C, 40Ca, 208Pb(π+, π+), (π-, π-), E=400, 500 MeV; 90Zr(π+, π+), E=400, 500 MeV; 90Zr(π-, π-), E=400 MeV; measured σ(θ). 208Pb(π+, π+), (π-, π-), E=662.7 MeV; 40Ca(π+, π+), (π-, π-), 12C(π+, π+), E=672.5 MeV; 12C(π-, π-), E=672.5, 486.2 MeV; analyzed σ(θ). Impulse approximation approach.
doi: 10.1103/PhysRevC.55.2533
1996MO03 Nucl.Phys. A599, 159c (1996) Isotensor Double Giant Resonance from Charge-Exchange Reactions NUCLEAR REACTIONS 93Nb, 90Zr, 40Ca, 56Fe, 13C, 27Al, 59Co(π+, π-), E=295 MeV; 13C(π+, π-), E=140-260 MeV; 40Ca(π-, π+), E=295 MeV; analyzed σ(θ), σ(θ, E(π)); deduced isotensor double giant resonances related features.
doi: 10.1016/0375-9474(96)00058-9
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
1995HU09 Phys.Rev. C51, 3169 (1995) P.Hui, H.T.Fortune, M.A.Kagarlis, J.M.O'Donnell, A.R.Fazely, R.Gilman, S.Mordechai, D.L.Watson Pion Double Charge Exchange on the Even Selenium Isotopes NUCLEAR REACTIONS 76,78,80,82Se(π+, π-), E=293.2 MeV; measured σ(θ, E(π-)). Model comparison.
doi: 10.1103/PhysRevC.51.3169
1994FO07 Phys.Rev. C50, 306 (1994) H.T.Fortune, G.B.Liu, J.M.O'Donnell, J.D.Silk, S.Mordechai Energy Dependence of 58Ni(π+, π-)58Zn Double Charge Exchange NUCLEAR REACTIONS 58Ni(π+, π-), E=120-292 MeV; measured σ(θ, E(π)); deduced double charge exchange σ.
doi: 10.1103/PhysRevC.50.306
1994MO04 Nucl.Phys. A569, 131c (1994) New Results on Multiple Excitations of Giant Resonances NUCLEAR REACTIONS 13C, 27Al, 59Co, 93Nb, 40Ca(π+, π-), E=295 MeV; analyzed σ(θ(π), E(π)) vs Q. 13O, 27P, 59Cu, 93Tc, 40Ti deduced GDR based on IAS, other type double giant resonance features.
doi: 10.1016/0375-9474(94)90103-1
1994MO44 Int.J.Mod.Phys. E3, 39 (1994) Double Giant Resonances NUCLEAR REACTIONS 12,13C, 27Al, 32S, 40Ca, 51V, 56Fe, 59Co, 80Se, 93Nb, 115In, 138Ba, 197Au, 208Pb(π+, π-), E=295 MeV; compiled, reviewed σ(θ), other data, analyses; deduced GDR excitation, associated exotic vibrational modes evidence.
doi: 10.1142/S0218301394000036
1994SM05 Phys.Rev. C50, 1216 (1994) D.A.Smith, H.T.Fortune, D.R.Benton, J.M.O'Donnell, M.A.Kagarlis, S.Mordechai, K.Johnson, H.Ward Double Analog State in Odd-A Nuclei NUCLEAR REACTIONS 51V, 59Co, 115In, 197Au(π+, π-), E=295 MeV; measured pion spectra, double IAS excitation σ(θ).
doi: 10.1103/PhysRevC.50.1216
1993GR03 Phys.Rev. C47, 1466 (1993) Y.Grof, N.Auerbach, D.Benton, H.T.Fortune, K.Johnson, M.A.Kagarlis, G.Kahrimanis, S.Mordechai, C.L.Morris, J.M.O'Donnell, I.Orion, D.Saunders, D.A.Smith, H.Ward, C.F.Moore Double Giant Resonances in Pion Double Charge Exchange on 51V, 115In, and 197Au NUCLEAR REACTIONS 51V, 115In, 197Au(π+, π-), E=295 MeV; measured σ(θ, E(π)), σ(θ). 51Mn, 197Tl, 115Sb deduced GDR, double IAS excitation, Γ.
doi: 10.1103/PhysRevC.47.1466
1993WA02 Phys.Rev. C47, 687 (1993) H.Ward, J.M.Applegate, N.Auerbach, J.Beck, J.Johnson, K.Koch, C.F.Moore, S.Mordechai, C.L.Morris, J.M.O'Donnell, M.Rawool-Sullivan, B.G.Ritchie, D.L.Watson, C.Whitley Systematics of the Double Isobaric Analog State Cross Section at 50 MeV NUCLEAR REACTIONS 44Ca, 56Fe, 93Nb(π+, π-), E=50 MeV; measured σ(θ, E(π)); deduced short range component of effective double charge exchange operator. 93Tc level deduced isospin mixing mechanism role in excitation.
doi: 10.1103/PhysRevC.47.687
1993WA07 Phys.Rev.Lett. 70, 3209 (1993) H.Ward, J.Johnson, K.Johnson, S.Greene, Y.Grof, C.F.Moore, S.Mordechai, C.L.Morris, J.M.O'Donnell, C.Whitley Energy Dependence of Double Giant Resonances in Pion Double Charge Exchange NUCLEAR REACTIONS 13C(π+, π-), E=140-295 MeV; measured σ(θ) vs E. 13O deduced levels, Γ, configuration.
doi: 10.1103/PhysRevLett.70.3209
1992BA02 Phys.Rev. C45, 197 (1992) Systematics of the Double Giant Dipole Resonances in Nuclei NUCLEAR STRUCTURE 12,13C, 27Al, 32S, 40Ca, 56Fe, 59Co, 93Nb, 115In, 138Ba, 197Au; analyzed pion double charge exchange reaction data; deduced double GDR systematics. Temperature-dependent RPA.
doi: 10.1103/PhysRevC.45.197
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
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
1992SM06 Phys.Rev. C46, 477 (1992) D.A.Smith, H.T.Fortune, G.-B.Liu, J.M.O'Donnell, M.Burlein, S.Mordechai, A.R.Fazely Pion Double Charge Exchange on 128,130Te NUCLEAR REACTIONS 128,130Te(π+, π-), E=292 MeV; measured σ(θ, E(π)); deduced collective states mass dependence. Other data analyzed.
doi: 10.1103/PhysRevC.46.477
1992WA11 Phys.Rev. C45, 2723 (1992) H.Ward, K.Johnson, G.Kahrimanis, D.Saunders, C.F.Moore, S.Mordechai, C.L.Morris, N.Auerbach Double Giant Dipole Resonance in the (π-, π+) Reaction NUCLEAR REACTIONS 13C, 27Al, 40Ca, 56Fe, 59Co, 93Nb(π-, π+), E=295 MeV; measured σ(θ), σ(θ, E(π)); deduced Pauli blocking effects, isospin splitting features. 13Be, 27Na, 40Ar, 59Mn, 93Y, 56Cr deduced double giant dipole resonance. Coupled-channels impulse approximation.
doi: 10.1103/PhysRevC.45.2723
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
1991MO02 Phys.Rev. C43, 1111 (1991) S.Mordechai, C.L.Morris, J.M.O'Donnell, M.A.Kagarlis, D.Fink, H.T.Fortune, D.L.Watson, R.Gilman, H.Ward, A.Williams, S.H.Yoo, C.F.Moore Analog of the T(>) Giant Dipole Resonance in Light Nuclei NUCLEAR REACTIONS 13C, 27Al, 59Co(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 13O, 27P, 59Cu deduced giant resonances, Γ, T.
doi: 10.1103/PhysRevC.43.1111
1991MO05 Phys.Rev. C43, R1509 (1991) S.Mordechai, H.Ward, K.Johnson, G.Kahrimanis, D.Saunders, C.F.Moore, J.M.O'Donnell, M.A.Kagarlis, D.Smith, H.T.Fortune, C.L.Morris Comparison of the Double Giant-Dipole States Observed in (π-, π+) and (π+, π-) Reactions on 40Ca and 27Al NUCLEAR REACTIONS 27Al, 40Ca(π-, π+), (π+, π-), E=295 MeV; measured σ(θ(π), E(π)); deduced σ(ratio). 27Na, 27P, 40Ar, 40Ti deduced double isovector GDR.
doi: 10.1103/PhysRevC.43.R1509
1991MO15 Phys.Rev. C44, 2209 (1991) C.F.Moore, K.Johnson, G.P.Kahrimanis, J.McDonald, M.Snell, H.J.Ward, S.H.Yoo, C.L.Morris, S.Mordechai, M.Burlein, N.Claytor, H.T.Fortune, R.Ivie, G.B.Liu, J.M.O'Donnell, D.Smith, N.Auerbach, D.Robson Angular Distributions for the Double Isobaric Analog and a T (<) State at High Excitation in Pion Double Charge Exchange on 93Nb NUCLEAR REACTIONS 93Nb(π+, π-), E=295 MeV; measured σ(θ(π), E(π)), σ(θ). 93Tc deduced large probability for T< excitation.
doi: 10.1103/PhysRevC.44.2209
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
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
1990MO02 Phys.Rev. C41, 202 (1990) S.Mordechai, H.T.Fortune, J.M.O'Donnell, G.Liu, M.Burlein, A.H.Wuosmaa, S.Greene, C.L.Morris, N.Auerbach, S.H.Yoo, C.F.Moore Observation of Double Isovector Giant Dipole Resonances from Pion Double Charge Exchange NUCLEAR REACTIONS 40Ca, 93Nb, 56Fe(π+, π-), E=292 MeV; measured σ(θ(π), E(π)). 56Ni, 40Ti, 93Tc deduced isovector GDR excitation. Other data analyzed.
doi: 10.1103/PhysRevC.41.202
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
1990YO02 J.Phys.(London) G16, L89 (1990) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom, M.Jones, S.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 208Pb(π±, π±'n) Reaction in the Giant-Resonance Region NUCLEAR REACTIONS 208Pb(π+, π+'n), (π-, π-'n), E=180 MeV; measured σ(θn, θπ), missing mass spectra. 208Pb deduced giant resonance neutron decay features.
doi: 10.1088/0954-3899/16/5/002
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
1989MO09 Phys.Rev. C40, 850 (1989) S.Mordechai, N.Auerbach, S.Greene, C.L.Morris, J.M.O'Donnell, H.T.Fortune, G.Liu, M.Burlein, A.Wuosmaa, S.H.Yoo, C.F.Moore Properties of the Giant Dipole Resonance Built on the Isobaric Analog State NUCLEAR REACTIONS 13C, 59Co, 93Nb, 138Ba, 197Au(π+, π-), E=292 MeV; measured σ(θ). 13O, 59Cu, 93Tc, 138Ce, 197Tl deduced GDR built on IAS.
doi: 10.1103/PhysRevC.40.850
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
1989YO06 Phys.Rev.Lett. 63, 738 (1989) S.H.Yoo, A.Williams, S.Mordechai, C.F.Moore, C.L.Morris, S.J.Seestrom-Morris, M.K.Jones, S.M.Sterbenz, D.Dehnhard, D.S.Oakley, A.Fazely 12C(π±, π±'p)11B Reaction Near the Giant Dipole Region NUCLEAR REACTIONS 12C(π+, π+'p), (π-, π-'p), E=180 MeV; measured σ(θ(π), θ(p), E(π)); deduced σ(π+, π+p)/σ(π-, π-p) near GDR. DWIA analysis.
doi: 10.1103/PhysRevLett.63.738
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
1988BA23 Phys.Lett. 207B, 227 (1988) A Unified Approach to Statistical Analysis of Nuclear Reactions NUCLEAR REACTIONS 12C(10B, p), E=20 MeV; analyzed data. Hauser-Feshbach analysis, TDHF level densities.
doi: 10.1016/0370-2693(88)90565-5
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
1988MO33 Phys.Rev. C38, 2709 (1988) S.Mordechai, N.Auerbach, H.T.Fortune, C.L.Morris, C.F.Moore Isospin Splitting of the Giant Dipole Built on the Isobaric Analog State NUCLEAR REACTIONS 56Fe(π+, π-), E=292 MeV; measured σ(E(π), θ(π)), σ(θ). 56Fe deduced double IAS, giant resonances, Γ.
doi: 10.1103/PhysRevC.38.2709
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
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
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
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
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
1987MO25 Phys.Rev. C36, 1950 (1987) S.Mordechai, C.Harvey, W.B.Cottingame, P.A.Seidl, C.F.Moore, L.C.Bland, M.Carchidi, H.T.Fortune, S.J.Seestrom-Morris, C.L.Morris Inelastic Pion Scattering to Low-Lying Excited States of 44Ca NUCLEAR REACTIONS 44Ca(π+, π+'), (π-, π-'), E=180 MeV; measured σ(θ), missing mass spectrum. 44Ca levels deduced neutron, proton matrix elements. DWIA analysis.
doi: 10.1103/PhysRevC.36.1950
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
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
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
1985MO16 Phys.Rev. C32, 854 (1985) 21Ne from 12C(10B, p) NUCLEAR REACTIONS 12C(10B, p), E=20 MeV; measured σ(θ), σ(Ep). 21Ne deduced levels J, π. Hauser-Feshbach, compound nucleus calculations.
doi: 10.1103/PhysRevC.32.854
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
1985MO20 Phys.Rev. C32, 2207 (1985) Reply to ' Comment on ' Negative-Parity Alpha Cluster in 19F ' ' NUCLEAR REACTIONS 15N(6Li, d), E=22 MeV; analyzed data. 19F levels deduced α-cluster characteristics.
doi: 10.1103/PhysRevC.32.2207
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
1984BA28 J.Phys.(London) G10, 785 (1984) Open-Shell Linear Response Model and the Systematics of Octupole States in Ge and Se Isotopes NUCLEAR STRUCTURE 70,72,74,76,78Ge, 74,76,78,80,82,84Se; analyzed octupole level systematics. Open shell linear response model.
doi: 10.1088/0305-4616/10/6/012
1984FO17 Phys.Lett. 145B, 4 (1984) H.T.Fortune, M.Carchidi, S.Mordechai Proton Occupation Numbers in Ge Isotopes NUCLEAR STRUCTURE 70,72,74,76Ge; analyzed two-nucleon transfer data; deduced proton occupation number.
doi: 10.1016/0370-2693(84)90935-3
1984MO07 Phys.Rev. C29, 1699 (1984) S.Mordechai, H.T.Fortune, M.Carchidi, R.Gilman Distribution of 0+ Strength in Ge(t, p) Reactions NUCLEAR REACTIONS 70,72,74,76Ge(t, p), E=15 MeV; measured absolute σ(θ) for (g.s.) → (g.s.), σ(Ep). 72,74,76,78Ge deduced 0+ strength. Natural, enriched targets. DWBA analysis.
doi: 10.1103/PhysRevC.29.1699
1984MO08 Phys.Rev. C29, 1765 (1984) Negative-Parity Alpha Clusters in 19F NUCLEAR REACTIONS 15N, 16O(6Li, d), E=22 MeV; measured σ(θ), σ(Ed). 19F, 20Ne deduced levels, L, J, π, Γα, σ(ratio).
doi: 10.1103/PhysRevC.29.1765
1984MO17 Phys.Rev. C30, 507 (1984) S.Mordechai, H.T.Fortune, C.F.Clement 43K from the 41K(t, p) Reaction NUCLEAR REACTIONS 41K(t, p), E=15 MeV; measured σ(θ), σ(Ep). 43K deduced levels, L, J, π, enhancement factors. DWBA analysis, shell model comparison.
doi: 10.1103/PhysRevC.30.507
1984MO28 Phys.Rev. C30, 1924 (1984) Mechanism of the 16O(7Li, α)19F Reaction at 20 MeV NUCLEAR REACTIONS, ICPND 16O(7Li, α), E=20 MeV; measured σ(Eα), σ(θ); deduced reaction mechanism, σ. 19F deduced levels, excitation σ dependence on band characteristics. Finite-range DWBA, Hauser-Feshbach analyses.
doi: 10.1103/PhysRevC.30.1924
1983MO09 Phys.Rev. C28, 623 (1983) S.Mordechai, S.LaFrance, H.T.Fortune 79As via Proton Pickup NUCLEAR REACTIONS 80Se(t, α), E=18 MeV; measured σ(Eα), σ(θ). 79As deduced levels, L, π, possible J, spectroscopic factors. DWBA analysis. Enriched target.
doi: 10.1103/PhysRevC.28.623
1982MO04 Phys.Rev. C25, 1276 (1982) S.Mordechai, S.Lafrance, H.T.Fortune Excitation of 81As by the 82Se(t, α) Reaction NUCLEAR REACTIONS 82Se(t, α), E=18 MeV; measured σ(Eα), σ(θ). 81As deduced levels, L, J, π, S. Enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.25.1276
1981CO13 Phys.Rev. C23, 2387 (1981) M.E.Cobern, L.C.Bland, H.T.Fortune, G.E.Moore, S.Mordechai, R.Middleton 16O(t, p)18O to Low-Lying States in 18O NUCLEAR REACTIONS 16O(t, p), E=15 MeV; measured σ(Ep, θ). 18O deduced levels, L, two-particle transfer amplitudes. Microscopic DWBA.
doi: 10.1103/PhysRevC.23.2387
1981ST18 Phys.Rev. C24, 1785 (1981) G.Stephans, S.Mordechai, H.T.Fortune Masses of 78Ge and 78As NUCLEAR REACTIONS Ge, 76,72,74Ge(t, p), E=17 MeV; 80Se(d, α), E not given; measured Q. 78Ge, 78As deduced mass excess. Enriched targets.
doi: 10.1103/PhysRevC.24.1785
1979FO14 Phys.Rev. C20, 1228 (1979) H.T.Fortune, G.E.Moore, L.Bland, M.E.Cobern, S.Mordechai, R.Middleton, R.D.Lawson Reaction 15N(t, p)17N NUCLEAR REACTIONS 15N(t, p), E=15.0 MeV; measured σ(Ep, θ). 17N levels deduced L, π, J. Enriched gas target. Comparison with shell model.
doi: 10.1103/PhysRevC.20.1228
1979LA04 J.Phys.(London) G5, L59 (1979) S.LaFrance, H.T.Fortune, S.Mordechai, R.Middleton 4p and 6p-2h States in 20O NUCLEAR REACTIONS 18O(t, p), E=15 MeV; measured σ(θ). 20O deduced levels, J, π, configurations. DWBA analysis.
doi: 10.1088/0305-4616/5/1/008
1979LA18 Phys.Rev. C20, 1673 (1979) S.LaFrance, H.T.Fortune, S.Mordechai, M.E.Cobern, G.E.Moore, R.Middleton, W.Chung, B.H.Wildenthal 20O from 18O(t, p) NUCLEAR REACTIONS 18O(t, p), E=15.0 MeV; measured σ(Ep, θ). 20O deduced levels, L, π, J. DWBA analysis, shell, weak-coupling models. Enriched gas target.
doi: 10.1103/PhysRevC.20.1673
1979MO08 Phys.Rev. C19, 1733 (1979) S.Mordechai, H.T.Fortune, R.Middleton, G.Stephans 72Ge from the 70Ge(t, p) Reaction NUCLEAR REACTIONS 70Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). 72Ge deduced levels, L, π, J. DWBA analysis.
doi: 10.1103/PhysRevC.19.1733
1978AL29 Phys.Rev. C18, 2727 (1978) D.E.Alburger, S.Mordechai, H.T.Fortune, R.Middleton Mass and Excited States of 12Be NUCLEAR REACTIONS 10Be(t, p), E=17 MeV; measured Q; deduced coefficients of isobaric mass multiplet equation. 12Be deduced mass excess, levels.
doi: 10.1103/PhysRevC.18.2727
1978FO06 Phys.Rev.Lett. 40, 1236 (1978) H.T.Fortune, M.E.Cobern, S.Mordechai, G.E.Moore, S.Lafrance, R.Middleton (sd)2 States in 14,16C NUCLEAR STRUCTURE 14,16C; calculated levels. Shell model.
doi: 10.1103/PhysRevLett.40.1236
1978LA12 Nucl.Phys. A307, 52 (1978) S.Lafrance, S.Mordechai, H.T.Fortune, R.Middleton Structure of 74Ge from the 72Ge(t, p) Reaction NUCLEAR REACTIONS 72Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). 74Ge deduced levels, L, π, J. DWBA analysis.
doi: 10.1016/0375-9474(78)90425-6
1978LI27 Nucl.Phys. A311, 61 (1978) J.Lichtenstadt, A.Marinov, M.Paul, J.Burde, S.Mordechai Study of the 41K(d, p)42K Reaction NUCLEAR REACTIONS 41K(d, p), E=10 MeV; measured σ(θ). 42K deduced levels, L, J, π, S. DWBA analysis. Enriched target.
doi: 10.1016/0375-9474(78)90502-X
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
1978MO07 J.Phys.(London) G4, 407 (1978) S.Mordechai, H.T.Fortune, G.E.Moore, M.E.Cobern, R.V.Kollarits, R.Middleton Spins of States Near 10 MeV Excitation in 14C NUCLEAR REACTIONS 12C(t, p), E=18 MeV; measured σ(Ep, θ). 14C levels deduced L, J, π. Enriched targets, DWBA analysis.
doi: 10.1088/0305-4616/4/3/015
1978MO08 Nucl.Phys. A301, 463 (1978) S.Mordechai, H.T.Fortune, G.E.Moore, M.E.Cobern, R.V.Kollarits, R.Middleton Structure of 14C from 12C(t, p) NUCLEAR REACTIONS 12C(t, p), E=18 MeV; measured σ(Ep, θ). 14C deduced levels, L, J, π. Comparison of data with shell-model calculations. Enriched targets.
doi: 10.1016/0375-9474(78)90062-3
1978MO13 J.Phys.(London) G4, L177 (1978) What Is V(so) for Tritons (Question) NUCLEAR REACTIONS 90Zr, 60Ni(polarized t, t), E=15.0 MeV; calculated σ(θ), A(θ).
doi: 10.1088/0305-4616/4/7/005
1978MO18 Phys.Lett. 76B, 192 (1978) G.E.Moore, M.E.Cobern, H.T.Fortune, S.Mordechai, R.V.Kollarits, R.Middleton 2p-1h States in 17N NUCLEAR REACTIONS 15N, 16O(t, p), E=15 MeV; measured σ(Ep, θ). 17N levels deduced J, π.
doi: 10.1016/0370-2693(78)90272-1
1978MO24 Phys.Rev. C18, 2498 (1978) S.Mordechai, H.T.Fortune, R.Middleton, G.Stephans 74Ge(t, p)76Ge Reaction NUCLEAR REACTIONS 74Ge(t, p), E=15.0 MeV; measured σ(Ep, θ). 76Ge deduced levels, L, π, J. DWBA analysis.
doi: 10.1103/PhysRevC.18.2498
1977DR01 Nucl.Phys. A275, 100 (1977) C.Drory, A.Marinov, E.Navon, J.Burde, S.Mordechai, E.Engler, M.Paul Study of Elastic and Inelastic Scattering of Protons from 74Ge at Isobaric Analogue Resonances NUCLEAR REACTIONS 74Ge(p, p), (p, p'), E=3.34-5.4 MeV; measured σ(Ep, θ), σ(Ep', θ). 75As deduced resonances, L(p), J, π, Γp, Γp', S. Enriched target.
doi: 10.1016/0375-9474(77)90278-0
1977FO09 Phys.Lett. 70B, 408 (1977) H.T.Fortune, R.Middleton, M.E.Cobern, G.E.Moore, S.Mordechai, R.V.Kollarits, H.Nann, W.Chung, B.H.Wildenthal Spectroscopy of 16C NUCLEAR REACTIONS 14C(t, p), E=15, 17, 18 MeV; measured σ(Ep, θ). 16C deduced levels, J, π, configuration.
doi: 10.1016/0370-2693(77)90400-2
1977FR02 Phys.Rev. C15, 456 (1977) E.Friedman, A.Moalem, D.Suraqui, S.Mordechai Isotope Shifts of 1f7/2 Radii from Nucleon-Transfer Reactions NUCLEAR REACTIONS 48Ca(3He, d), E=8-10 MeV; 48Ca(d, t), E=8.5 MeV; measured σ(E, θ). 40Ca(3He, d), E=10.7 MeV; 40Ca(t, d), E=3 MeV; analyzed data. 41,48Ca, 41,49Sc deduced isotope shift.
doi: 10.1103/PhysRevC.15.456
1977FR07 Phys.Rev. C15, 1604 (1977) E.Friedman, A.Moalem, D.Suraqui, S.Mordechai Absolute Normalization of the (α, 3He) Reaction NUCLEAR REACTIONS 48Ca(3He, α), E=9-13 MeV; measured σ(E, θ); deduced normalization constant for (α, 3he).
doi: 10.1103/PhysRevC.15.1604
1977KA21 Nucl.Phys. A289, 205 (1977) D.Kalinsky, D.Melnik, U.Smilansky, N.Trautner, Y.Horowitz, S.Mordechai Nuclear Reactions Induced by the Bombardment of 18O with 18O NUCLEAR REACTIONS 18O(18O, 18O), (18O, 19O), (18O, 20O), E(cm)=10-18 MeV; measured σ(θ); deduced deformation parameters, S.
doi: 10.1016/0375-9474(77)90529-2
1977MO10 Nucl.Phys. A287, 109 (1977) S.Mordechai, H.T.Fortune, W.J.Courtney Neutron Pickup on 93Nb NUCLEAR REACTIONS 93Nb(3He, α), E=19.5 MeV; measured σ(Eα, θ). 92Nb deduced levels, L(n), S. Enriched target.
doi: 10.1016/0375-9474(77)90566-8
1977MO13 Nucl.Phys. A289, 36 (1977) S.Mordechai, M.E.Cobern, G.E.Moore, H.T.Fortune Study of 78As with the 80Se(d, α) Reaction NUCLEAR REACTIONS 80Se(d, α), E=16.0 MeV; measured σ(Eα, θ); deduced Q. 78As deduced levels, L, J, π.
doi: 10.1016/0375-9474(77)90518-8
1977PA24 Nucl.Phys. A289, 94 (1977) M.Paul, A.Marinov, J.Burde, C.Drory, J.Lichtenstadt, S.Mordechai, E.Navon Particle-Hole States in 42K Studied by the 44Ca(d, α)43K Reaction NUCLEAR REACTIONS 44Ca(d, α), E=11 MeV; measured σ(θ). 42K deduced levels, L, J, π. DWBA analysis. Enriched target.
doi: 10.1016/0375-9474(77)90523-1
1976FR22 Phys.Rev. C14, 2082 (1976) E.Friedman, A.Moalem, D.Suraqui, S.Mordechai Absolute Normalization of (t, d) and (3He, d) Reactions NUCLEAR REACTIONS 40Ca(d, p), E=3, 4, 6 MeV; 40Ca(3He, d), E=9 MeV; 40Ca(d, 3He), E=11 MeV; measured σ(θ); deduced normalization constants for (t, d), (3He, d) reactions. 40Ca, 208Pb(t, d), 208Pb(p, d); calculated σ(θ).
doi: 10.1103/PhysRevC.14.2082
1976MO32 Nucl.Phys. A272, 82 (1976) S.Mordechai, E.Friedman, A.A.Jaffe, D.Nir, M.Paul A Study of Low-Lying States of 76As Using the 75As(d, p) Reaction NUCLEAR REACTIONS 75As(d, p), E=11 MeV; measured σ(Ep, θ); deduced Q. 76As deduced levels, L(n), spectroscopic strengths. DWBA analysis.
doi: 10.1016/0375-9474(76)90319-5
1976OS04 Nucl.Phys. A265, 142 (1976) R.Ost, N.E.Sanderson, S.Mordechai, J.B.A.England, B.R.Fulton, J.M.Nelson, G.C.Morrison Do Many-Particle Reactions Contribute to 'Deep-Inelastic' Peaks (Question) NUCLEAR REACTIONS 60Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8. 58,64Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8, light particle coin for Li, B, Be, α, p; deduced reaction mechanism. Enriched targets.
doi: 10.1016/0375-9474(76)90120-2
1975KA24 Nucl.Phys. A250, 364 (1975) D.Kalinsky, D.Melnik, U.Smilansky, N.Trautner, B.A.Watson, Y.Horowitz, S.Mordechai, G.Baur, D.Pelte Nuclear Reactions between Oxygen Isotopes NUCLEAR REACTIONS 16O(17O, 17O), (18O, 18O), E(cm)=12-16, 19-20 MeV; measured σ(θ).
doi: 10.1016/0375-9474(75)90266-3
1974BE54 Nucl.Phys. A230, 235 (1974) R.R.Betts, S.Mordechai, D.J.Pullen, B.Rosner, W.Scholz Study of 71,73,75,77As with Ge(3He, d) Reactions NUCLEAR REACTIONS 70,72,74,76Ge(3He, d), E=17.0 MeV; measured σ(Ed, θ). 71,73,75,77As deduced levels, L(p), J, π. Enriched targets.
doi: 10.1016/0375-9474(74)90305-4
1974MO19 Nucl.Phys. A230, 343 (1974) S.Mordechai, E.Friedman, A.A.Jaffe, D.Nir, M.Paul A Study of Low-Lying States of 72As Using the 72Ge(p, nγ)72As Reaction NUCLEAR REACTIONS 72Ge(p, nγ), Ep=5.1-6.2 MeV; measured σ(E, Eγ, θ), γγ-coin. 72As deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(74)90312-1
1973MO14 Nucl.Phys. A208, 410 (1973) S.Mordechai, A.A.Jaffe, D.Nir, M.Paul The Angular Distribution of γ-Rays Following the (p, n) Reaction on 74Ge NUCLEAR REACTIONS 74Ge(p, nγ), E=3.50, 3.80, 4.00 MeV; measured σ(Eγ, θ), 74As levels deduced J, π. Enriched target.
doi: 10.1016/0375-9474(73)90384-9
1973RO14 Nucl.Phys. A206, 76 (1973) B.Rosner, S.Mordechai, D.J.Pullen Study of 74As by the 73Ge(3He, d) Reaction NUCLEAR REACTIONS 73Ge(3He, d), E(3He)=17 MeV; measured σ(θ). 74As deduced levels, L(p), spectroscopic strengths.
doi: 10.1016/0375-9474(73)90607-6
1971PA16 Nucl.Phys. A168, 267 (1971) M.Paul, A.Marinov, C.Drory, J.Burde, E.Navon, S.Mordechai The Level Structure of 46K Studied by Comparison of the (d, α) Reaction on 42Ca and 48Ca NUCLEAR REACTIONS 48,42Ca(d, α), E=11.0 MeV; measured σ(θ). 46K levels deduced J, π. Enriched targets.
doi: 10.1016/0375-9474(71)90793-7
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