NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = S.Mordechai

Found 96 matches.

Back to query form



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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1996MO03      Nucl.Phys. A599, 159c (1996)

S.Mordechai, C.F.Moore

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994MO04      Nucl.Phys. A569, 131c (1994)

S.Mordechai, C.F.Moore

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
Citations: PlumX Metrics


1994MO44      Int.J.Mod.Phys. E3, 39 (1994)

S.Mordechai, C.F.Moore

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1992BA02      Phys.Rev. C45, 197 (1992)

J.Bar-Touv, S.Mordechai

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1988BA23      Phys.Lett. 207B, 227 (1988)

J.Bar-Touv, S.Mordechai

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1985MO16      Phys.Rev. C32, 854 (1985)

S.Mordechai, H.T.Fortune

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1985MO20      Phys.Rev. C32, 2207 (1985)

S.Mordechai, H.T.Fortune

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1984BA28      J.Phys.(London) G10, 785 (1984)

J.Bar-Touv, S.Mordechai

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0530.


1984MO08      Phys.Rev. C29, 1765 (1984)

S.Mordechai, H.T.Fortune

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0020.


1984MO28      Phys.Rev. C30, 1924 (1984)

S.Mordechai, H.T.Fortune

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0028.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1309.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1310.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0022.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1978MO13      J.Phys.(London) G4, L177 (1978)

S.Mordechai, H.T.Fortune

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


Back to query form