NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Moalem Found 50 matches. 2004GE05 Nucl.Phys. A732, 125 (2004) E.Gedalin, A.Moalem, L.Razdolskaya Meson U(3)L (X) U(3)R chiral theory with flavor and nonet symmetry breaking
doi: 10.1016/j.nuclphysa.2003.12.007
2004GE08 Nucl.Phys. A733, 213 (2004) E.Gedalin, A.Moalem, L.Razdolskaya A chiral effective field U(3)L (X) U(3)R theory for light mesons
doi: 10.1016/j.nuclphysa.2003.12.019
2000HI13 Eur.Phys.J. A 7, 537 (2000) F.Hibou, C.Wilkin, A.M.Bergdolt, G.Bergdolt, O.Bing, M.Boivin, A.Bouchakour, F.Brochard, M.P.Combes-Comets, P.Courtat, R.Gacougnolle, Y.Le Bornec, A.Moalem, F.Plouin, F.Reide, B.Tatischeff, N.Willis Near-Threshold η Production in the pd → pdη Reaction NUCLEAR REACTIONS 2H(p, pX), E=905, 909 MeV; measured η production associated missing mass spectra, σ. Comparison with model predictions.
doi: 10.1007/s100500050426
1999GE06 Nucl.Phys. A650, 471 (1999) E.Gedalin, A.Moalem, L.Razdolskaja On the pp → ppη(η') Reactions Near Threshold NUCLEAR REACTIONS 1H(p, pX), (π0, X), E ≈ threshold; calculated η, η' production σ. One boson exchange model.
doi: 10.1016/S0375-9474(99)00110-4
1999GE08 Nucl.Phys. A652, 287 (1999) E.Gedalin, A.Moalem, L.Rasdolskaya S-Wave π0 Production in pp Collisions in a OBE Model NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated σ; deduced role of two-pion exchange. Covariant one boson exchange model. Comparison with data.
doi: 10.1016/S0375-9474(99)00140-2
1999GE16 Phys.Rev. C60, 031001 (1999) E.Gedalin, A.Moalem, L.Razdolskaya S-Wave π0 Production in pp Collision from Chiral Perturbation Theory Calculations with Loop Contributions NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated total σ; deduced one-loop contributions. Chiral perturbation theory.
doi: 10.1103/PhysRevC.60.031001
1998GE03 Nucl.Phys. A634, 368 (1998) E.Gedalin, A.Moalem, L.Razdolskaja A Convariant OBE Model for η Production in NN Collisions
doi: 10.1016/S0375-9474(98)00152-3
1998HI19 Phys.Lett. 438B, 41 (1998) F.Hibou, O.Bing, M.Boivin, P.Courtat, G.Faldt, R.Gacougnolle, Y.Le Bornec, J.M.Martin, A.Moalem, F.Plouin, A.Taleb, B.Tatischeff, C.Wilkin, N.Willis, R.Wurzinger Comparison of η and η' Production in the pp → ppη(η') Reactions near Threshold NUCLEAR REACTIONS 1H(p, pX), E=2416, 2430 MeV; measured η, η' production σ.
doi: 10.1016/S0370-2693(98)01026-0
1996MA15 Phys.Rev. C53, 2068 (1996) B.Mayer, A.Boudard, B.Fabbro, M.Garcon, C.Kerboul, J.Poitou, F.Wellers, W.W.Jacobs, J.Saudinos, E.Tomasi-Gustafsson, J.P.Mouly, R.S.Kessler, B.M.K.Nefkens, B.Tippens, A.van der Schaaf, R.Abegg, W.T.H.van Oers, W.Briscoe, A.Petrov, A.Moalem Reaction pd → 3Heη and pd → 3Heπ+π- Near the η Threshold NUCLEAR REACTIONS 2H(p, X), E=831.6-902.4 MeV; measured σ(E, θ) for η production; deduced η3He-scattering length. Tagging facility.
doi: 10.1103/PhysRevC.53.2068
1996MO07 Nucl.Phys. A600, 445 (1996) A.Moalem, E.Gedalin, L.Razdolskaja, Z.Shorer The NN → NNη Reaction Close to Threshold NUCLEAR REACTIONS 1n, 1H(p, X), E=η-production threshold; calculated η-production σ vs (Q(cm)), energy spectra. Nonrelativistic one-boson exchange model.
doi: 10.1016/0375-9474(95)00496-3
1995MO21 Nucl.Phys. A589, 649 (1995) A.Moalem, E.Gedalin, L.Razdolskaja, Z.Shorer Threshold Production Cross Section of the pp → pp(eta) Reaction in a Nonrelativistic OBE Model NUCLEAR REACTIONS 1H(p, X), E=threshold; calculated eta production σ. Nonrelativistic one-boson exchange model.
doi: 10.1016/0375-9474(95)00127-M
1992TA05 Phys.Rev. C45, 2005 (1992) B.Tatischeff, M.P.Combes-Comets, P.Courtat, R.Gacougnolle, Y.Le Bornec, E.Loireleux, F.Reide, N.Willis, A.M.Bergdolt, G.Bergdolt, O.Bing, F.Hibou, M.Boivin, A.Moalem Measurement of the 1H(d(pol), pp)X Reaction and Possible Evidence for a Structure at M(pp) = 1945 MeV NUCLEAR REACTIONS 1H(polarized d, pX), E=2.1, 1.722 GeV; measured analyzing powers vs invariant mass M(pp); deduced a possible evidence for a structure at M(pp)=1945 MeV.
doi: 10.1103/PhysRevC.45.2005
1991CO04 Phys.Rev. C43, 973 (1991) M.P.Combes-Comets, P.Courtat, R.Frascaria, Y.Le Bornec, E.Loireleux, F.Reide, B.Tatischeff, N.Willis, E.Aslanides, D.Benabdelouahed, A.M.Bergdolt, G.Bergdolt, O.Bing, P.Fassnacht, F.Hibou, M.Boivin, A.Chisholm, C.Kerboul, A.Moalem Search for T = 2 Dibaryons in the p(pol) + p → π- + X Reaction and Study of Highly Inelastic NN Scattering NUCLEAR REACTIONS 1H(polarized p, π-X), E=1.45-2.7 GeV; measured σ(θ), analyzing power vs missing mass; deduced 6-quarks state σ upper limits, 2π production mechanism.
doi: 10.1103/PhysRevC.43.973
1990TA37 J.Phys.(Paris), Colloq.C-6, 371 (1990) B.Tatischeff, M.P.Comets, P.Courtat, Y.Le Bornec, E.Loireleux, F.Reide, N.Willis, A.M.Bergdolt, G.Bergdolt, O.Bing, F.Hibou, M.Boivin, A.Moalem Search for Narrow Isovector Dibaryons Close to Low Masses Threshold NUCLEAR REACTIONS 1H(polarized d, pX), E=1.722 GeV; measured vector, tensor analyzing power vs 2p-invariant mass.
1989WI18 Phys.Lett. 229B, 33 (1989) N.Willis, A.Moalem, M.P.Comets, J.Arvieux, A.M.Bergdolt, G.Bergdolt, L.Bimbot, O.Bing, M.Boivin, A.Chisholm, P.Courtat, F.Hibou, Y.Le Bornec, E.Loireleux, F.Reide, B.Tatischeff Experimental Search for B = 2, T = 2 Bound States Around the πNN Threshold NUCLEAR REACTIONS 1H(polarized p, π-), E=1.45 GeV; measured σ(θ), analyzing power vs missing mass; deduced no definitive dibaryonic T=2 structures.
doi: 10.1016/0370-2693(89)90150-0
1988JA01 Phys.Lett. 201B, 25 (1988) K.P.Jackson, A.Celler, W.P.Alford, K.Raywood, R.Abegg, R.E.Azuma, C.K.Campbell, S.El-Kateb, D.Frekers, P.W.Green, O.Hausser, R.L.Helmer, R.S.Henderson, K.H.Hicks, R.Jeppesen, P.Lewis, C.A.Miller, A.Moalem, M.A.Moinester, R.B.Schubank, G.G.Shute, B.M.Spicer, M.C.Vetterli, A.I.Yavin, S.Yen The (n, p) Reaction as a Probe of Gamow-Teller Strength NUCLEAR REACTIONS 6Li, 12,13C(n, p), E=198 MeV; measured σ(θ), σ(θp).
doi: 10.1016/0370-2693(88)90073-1
1987MO04 Phys.Lett. 183B, 269 (1987) A.Moalem, D.Frekers, S.A.Gurvitz, R.Abegg, C.Davis, K.P.Jackson, C.A.Miller, R.S.Henderson, S.Yen, R.L.Helmer, K.H.Hicks, J.S.Wesick Inclusive Analyzing Power and Scattering Mechanisms in Proton-Nucleus Scattering at Backward Angles NUCLEAR REACTIONS 9Be, C(polarized p, p'), E=303 MeV; measured analyzing power (θ=120°); deduced scattering mechanism. ΔE-E telescopes.
doi: 10.1016/0370-2693(87)90961-0
1984MO25 Phys.Lett. 146B, 379 (1984) A.Moalem, J.A.Niskanen, A.M.Green Direct Formation of NN(bar) Bound States in a Single Nucleon Pickup NUCLEAR REACTIONS 4He(p-bar, X), E=low; calculated σ(θ) for nucleon-antinucleon (X) bound states; deduced nucleon-antinucleon state parameters.
doi: 10.1016/0370-2693(84)90143-6
1982FI14 Nucl.Phys. A389, 18 (1982) D.Fink, E.Friedman, M.Paul, A.Moalem Experimental Determination of the Normalization Constant of the (α, t) Reaction NUCLEAR REACTIONS 48Ca, 92Mo(α, t), E=26-30 MeV; 48Ca, 92Mo(3He, d), E=16 MeV; measured absolute σ(θ). 49Sc, 93Tc level deduced normalizations. Enriched targets.
doi: 10.1016/0375-9474(82)90287-1
1982MO03 Nucl.Phys. A378, 251 (1982) A.Moalem, H.T.Fortune, G.Stephans Orbit Sizes in the 91Zr ± N Systems from Transfer Reactions NUCLEAR REACTIONS 91Zr(d, 3He), (3He, d), (α, t), E not given; analyzed data. 91Zr levels deduced S for 2p1/2, 1g9/2 proton-, 2d5/2 neutron-transfer. 90Y, 90,92Zr, 92Nb deduced nucleon orbit rms radii. DWBA, spin-dependent sum rule renormalization.
doi: 10.1016/0375-9474(82)90591-7
1982MO22 Phys.Rev. C26, 1757 (1982) Regularities of Orbit Sizes of Valence Nucleons NUCLEAR STRUCTURE A=29-92; analyzed single particle orbit point rms radii; deduced particle separation energy dependence.
doi: 10.1103/PhysRevC.26.1757
1981BA04 Nucl.Phys. A351, 285 (1981) Low Multipole States in 18O from Open-Shell Linear Response Model NUCLEAR STRUCTURE 18O; calculated isovector dipole, isoscalar quadrupole, octupole transition strength distribution, EWSR. Open-shell linear response method, intermediate coupling, Skyrme forces. NUCLEAR REACTIONS 16O(γ, p), (γ, n), E=1-40 MeV; calculated isovector dipole σ(E). Open-shell linear response method, intermediate coupling, Skyrme forces.
doi: 10.1016/0375-9474(81)90445-0
1981BU22 Nucl.Phys. A351, 238 (1981) J.Burde, V.Richter, I.Labaton, A.Moalem Low-Energy Excited States in 128I Produced by the (p, n) Reaction NUCLEAR REACTIONS 128Te(p, n), E=2.8-5 MeV; measured Eγ, Iγ, γγ-coiin, γγ(t), Iγ(θ). 128I deduced levels, J, π, γ-multipolarity, γ-branching, configurations. Enriched target.
doi: 10.1016/0375-9474(81)90442-5
1981MO12 Phys.Rev. C23, 1810 (1981) Extension of Linear-Response Method to Open-Shell Multipole Giant Resonances NUCLEAR STRUCTURE 12C; calculated B(E1), B(E2), B(E3), T=1 dipole, T=0 quadrupole, T=0 octupole transition strength distributions. Extended linear responce open shell RPA, Skyrme forces.
doi: 10.1103/PhysRevC.23.1810
1980BA09 Nucl.Phys. A339, 303 (1980) J.Bar Touv, A.Moalem, S.Shlomo Isotopic Dependence of Giant Multipole Resonances NUCLEAR STRUCTURE 40,42,44,46,48Ca; calculated giant multipole strength distributions; deduced isotopic dependence. Open-shell RPA, linear response theory.
doi: 10.1016/0375-9474(80)90095-0
1979MO12 Phys.Rev. C20, 1593 (1979) A.Moalem, Y.Gaillard, A.M.Bemolle, M.Buenerd, J.Chauvin, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, P.de Saintignon Isotopic Dependence of the Giant Quadrupole Resonance in the Stable Even-Mass Molybdenum Nuclei NUCLEAR REACTIONS 100,98,96,94,92Mo(3He, 3He'), E=110 MeV; measured σ(E, θ). 100,98,96,94,92Mo deduced E, Γ, strength of GQR.
doi: 10.1103/PhysRevC.20.1593
1979MO20 Nucl.Phys. A332, 195 (1979) Radial Distributions of 1f Nucleons from Transfer Data on 51V NUCLEAR REACTIONS 51V(d, 3He), E=34.4, 52, 80 MeV; 51V(d, t), E=16 MeV, 19.5 MeV; 51V(3He, d), E=10.48, 22 MeV; 51V(α, t), E=29 MeV; analyzed data. 51V, 52Cr deduced rms radii of 1f7/2 n, p. DWBA model.
doi: 10.1016/0375-9474(79)90104-0
1979MO21 Nucl.Phys. A332, 205 (1979) On Absolute Normalization of the (α, t) Reaction NUCLEAR REACTIONS 51V(α, t), E=29 MeV; analyzed data; deduced zero-range normalization. Spin-dependent sum rule analysis.
doi: 10.1016/0375-9474(79)90105-2
1978BU15 Nucl.Instrum.Methods 151, 261 (1978) J.Burde, V.Richter, I.Labaton, A.Moalem, D.Kalinsky Multiparameter Data Acquisition and Analysis in Nuclear Reaction on-Line Measurements NUCLEAR REACTIONS 128Te(p, nγ), E=5 MeV; measured γγ(t). 128I level deduced T1/2.
doi: 10.1016/0029-554X(78)90498-6
1978MO20 Nucl.Phys. A307, 277 (1978) A.Moalem, J.F.A.Van Hienen, E.Kashy Role of the rms Radius in DWBA Calculations of the (p, d) Reaction NUCLEAR REACTIONS 46,48,50Ti(p, d), E=35 MeV; calculated σ(θ). 45,47,49Ti levels deduced S.
doi: 10.1016/0375-9474(78)90617-6
1978MO32 Phys.Rev.Lett. 40, 1064 (1978) Radial Distribution of 1g9/2 Nucleons in Sr Isotopes from Nucleon-Transfer Reactions
doi: 10.1103/PhysRevLett.40.1064
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
1977MO04 Nucl.Phys. A281, 461 (1977) Properties of the GQR from the 40Ca(3He, 3He'α)36Ar and 40Ca(3He, 3He'p)39K Reactions NUCLEAR REACTIONS 40Ca(3He, 3Heα), 40Ca(3He, 3Hep), E=70 MeV; measured w(θ) in the reaction plane for θ(3He)=-22°; comparison with two-step mechanism calculations.
doi: 10.1016/0375-9474(77)90508-5
1977MO14 Nucl.Phys. A289, 45 (1977) Consistency Check of (d, p), (t, d) and (3He, α) Absolute Normalizations From Spin-Dependent Sum-Rule Analysis NUCLEAR REACTIONS 45Sc(d, p), (d, t), (3He, α); reanalyzed data; deduced normalization constant for (3He, α). Spin-dependent sum-rule analysis of f7/2 neutron transfers.
doi: 10.1016/0375-9474(77)90519-X
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
1976MO07 Phys.Lett. 61B, 167 (1976) A.Moalem, W.Benenson, G.M.Crawley, T.L.Khoo Decay Modes of the Giant Resonance Region in 40Ca NUCLEAR REACTIONS 40Ca(3He, 3He'), E=70 MeV; measured p3He'(θ), 3He'α(θ). 40Ca resonance deduced Γp/Γα.
doi: 10.1016/0370-2693(76)90617-1
1975MO02 Phys.Rev. C11, 654 (1975) Structure of 33S from a Study of the 34S(p, d)33S Reaction at 35 MeV NUCLEAR REACTIONS 34S(p, d), E=35 MeV; measured σ(Ed, θ). 33S deduced levels, J, π, S, L.
doi: 10.1103/PhysRevC.11.654
1975MO26 Phys.Lett. 58B, 286 (1975) A.Moalem, M.A.M.Shahabuddin, R.G.Markham, H.Nann Splitting of the Lowest T = 2 States in 44Ti, 48Cr and 52Fe NUCLEAR REACTIONS 46Ti, 50Cr, 54Fe(p, t), E=46.0 MeV; measured σ(Et, θ). 44Ti, 48Cr deduced level splitting.
doi: 10.1016/0370-2693(75)90654-1
1974BE20 Phys.Rev. C9, 2130 (1974) W.Benenson, E.Kashy, D.H.Kong-A-Siou, A.Moalem, H.Nann T = 3/2 States in Mass-11 Nuclei NUCLEAR REACTIONS 14N(3He, 6He), E=70 MeV; 13C(p, t), E=46.7 MeV; 13C(p, 3He), E=40 MeV; measured σ(E(6He), Et, E(3He)). 11N, 11C, 11B deduced levels.
doi: 10.1103/PhysRevC.9.2130
1974HA24 Phys.Lett. 49B, 235 (1974) G.R.Hammerstein, H.McManus, A.Moalem, T.T.S.Kuo The Excitation of Giant Resonances in Electron and Proton Scattering NUCLEAR REACTIONS 40Ca(e, e'), (p, p'); measured nothing, calculated σ, B(EL) for giant resonances.
doi: 10.1016/0370-2693(74)90421-3
1974MO26 Nucl.Phys. A236, 307 (1974) A.Moalem, W.Benenson, G.M.Crawley A Study of the Nuclear Continuum in 16O by Inelastic 3He Scattering NUCLEAR REACTIONS 16O(3He, 3He'), E=71 MeV; measured σ(E(3He'), θ). 16O resonances deduced E2 strength.
doi: 10.1016/0375-9474(74)90256-5
1973CO21 Nucl.Phys. A211, 21 (1973) S.Cochavi, A.Moalem, D.Ashery, J.Alster, G.Bruge, A.Chaumeaux Study of the (p, d) Reaction on 95Mo and 97Mo NUCLEAR REACTIONS 95,97Mo(p, d); E=26 MeV, measured σ(Ed, θ), 94,96Mo deduced levels, L(n), C2S. Enriched targets.
doi: 10.1016/0375-9474(73)90762-8
1973MO10 Phys.Rev.Lett. 31, 482 (1973) A.Moalem, W.Benenson, G.M.Crawley Excitation of Giant Resonances by Inelastic 3He Scattering NUCLEAR REACTIONS 27Al, 40Ca, 58Ni, 90Zr, 122Sn, 197Au, 208Pb, 209Bi(3He, 3He'), E=71 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevLett.31.482
1973MO23 Phys.Rev. C8, 1961 (1973) Mass of 31S NUCLEAR REACTIONS 23Na, 27Al, 32,33,34S, 35,37Cl(p, d), E=35 MeV, measured Q. 31S deduced new value for the mass.
doi: 10.1103/PhysRevC.8.1961
1972AG04 Phys.Rev. C6, 385 (1972) D.Agassi, N.Auerbach, A.Moalem Stripping to Isobaric Analog Resonances NUCLEAR REACTIONS 92Mo(3He, d), E not given; analyzed σ(θ). 93Tc deduced IAR S.
doi: 10.1103/PhysRevC.6.385
1972AS07 Phys.Rev. C5, 1729 (1972) D.Ashery, S.Alper, A.Moalem, Y.Shamai, A.I.Yavin, G.Bruge, A.Chaumeaux, M.A.Moinester (3He, d) Stripping to Unbound Analog States in Tc Isotopes NUCLEAR REACTIONS 92,94,96Mo(3He, d), E=30.2 MeV; measured σ(Ed, θ). 93,95,97Tc deduced isobaric analog states, S.
doi: 10.1103/PhysRevC.5.1729
1972MO35 Nucl.Phys. A196, 605 (1972) A.Moalem, M.A.Moinester, J.Alster, Y.Dupont Study of the Even Molybdenum Isotopes with the (p, t) Reaction NUCLEAR REACTIONS 96,98Mo(p, t), E=40 MeV; measured σ(Et, θ). 94,96Mo deduced levels, J, π, L.
doi: 10.1016/0375-9474(72)90796-8
1971MO08 Phys.Lett. 34B, 392 (1971) A.Moalem, M.A.Moinester, J.Alster, Y.Dupont, M.Chabre The 92Mo(p, t)90Mo Reaction at 40 MeV NUCLEAR REACTIONS 92Mo(p, t), E=40 MeV; measured σ(Et, θ). 90Zr(p, t); reanalyzed data. 88Zr, 90Mo deduced levels, J, π.
doi: 10.1016/0370-2693(71)90634-4
1971MO32 Nucl.Phys. A177, 145 (1971) A.Moalem, M.A.Moinester, N.Auerbach, J.Alster, Y.Dupont A Nuclear Structure Study with the 94Mo, (p, t)92Mo Reaction NUCLEAR REACTIONS 94Mo(p, t), E=40 MeV; measured σ(Et, θ). 92Mo deduced levels, L, J, π. Enriched target.
doi: 10.1016/0375-9474(71)90167-9
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