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Search: Author = A.Moalem

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13150.


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
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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
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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
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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
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1982MO22      Phys.Rev. C26, 1757 (1982)

A.Moalem

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
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1981BA04      Nucl.Phys. A351, 285 (1981)

J.Bar-Touv, A.Moalem

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
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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
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1981MO12      Phys.Rev. C23, 1810 (1981)

A.Moalem, J.Bar-Touv

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
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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
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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
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1979MO20      Nucl.Phys. A332, 195 (1979)

A.Moalem, Z.Vardi

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
Citations: PlumX Metrics


1979MO21      Nucl.Phys. A332, 205 (1979)

A.Moalem, Z.Vardi

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
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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
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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
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1978MO32      Phys.Rev.Lett. 40, 1064 (1978)

A.Moalem, E.Friedman

Radial Distribution of 1g9/2 Nucleons in Sr Isotopes from Nucleon-Transfer Reactions

doi: 10.1103/PhysRevLett.40.1064
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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
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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
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1977MO04      Nucl.Phys. A281, 461 (1977)

A.Moalem

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
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1977MO14      Nucl.Phys. A289, 45 (1977)

A.Moalem

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
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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
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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
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1975MO02      Phys.Rev. C11, 654 (1975)

A.Moalem, B.H.Wildenthal

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
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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
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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
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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
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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
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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
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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
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1973MO23      Phys.Rev. C8, 1961 (1973)

A.Moalem, B.H.Wildenthal

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
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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
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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
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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
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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
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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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Note: The following list of authors and aliases matches the search parameter A.Moalem: , A.S.MOALEM