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NSR database version of May 19, 2024.

Search: Author = U.Smilansky

Found 25 matches.

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1985JA08      Nucl.Phys. A438, 536 (1985)

P.Jacobs, U.Smilansky

Alignment Effects in Subbarrier Fusion Reactions

NUCLEAR REACTIONS, ICPND 165Ho(16O, X), E(cm) ≈ 57-80 MeV; calculated fusion σ(E); deduced alignment effect role. Coupled-Channels model, incoming wave boundary condition.

doi: 10.1016/0375-9474(85)90392-6
Citations: PlumX Metrics


1982HU03      Z.Phys. A304, 225 (1982)

H.Hubel, R.M.Diamond, P.Aguer, C.Ellegaard, D.B.Fossan, H.Kluge, C.Schuck, S.Shih, F.S.Stephens, U.Smilanski

Lifetimes of Unresolved Transitions from Very High Spin States in Nuclei near N = 82

NUCLEAR REACTIONS 28Si(129Xe, xn), E=720 MeV; 28Si(136Xe, xn), E=740 MeV; measured DSA, Eγ, Iγ. 164,157Er deduced continuum transition T1/2, B(E2), β2, quadrupole moment. Ge(Li), NaI(Tl) detectors.


1980ST09      Phys.Rev. C21, 2427 (1980)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya

Fusion of 16O + 148,150,152,154Sm at Sub-Barrier Energies

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured evaporation residue Eγ, E(K X-ray), I(K X-ray); deduced fusion σ(E).

doi: 10.1103/PhysRevC.21.2427
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1608.


1979LE05      Nucl.Phys. A315, 205 (1979)

S.Levit, U.Smilansky

A Uniform Semi-Classical Approach to the Coulomb Fission Problem

NUCLEAR REACTIONS 238U(136Xe, F), E=4.5-5.5 MeV/nucleon; calculated σ(E, θ) of fragments for Coulomb fission. Semi-classical theory, path integral formalism.

doi: 10.1016/0375-9474(79)90644-4
Citations: PlumX Metrics


1978BE10      Phys.Rev. C17, 628 (1978)

M.J.Bechara, O.Dietzsch, M.Samuel, U.Smilansky

Reorientation Effect Measurements in 122Te and 128Te

NUCLEAR REACTIONS 122,128Te(α, α'), E=8-10 MeV; 122,128Te(14N, 14N'), E=32-37 MeV; 122,128Te(16O, 16O'), E=30.5-42 MeV; 122Te(18O, 18O'), E=34-35 MeV; measured σ(θ). 122,128Te deduced quadrupole moment, B(E2).

doi: 10.1103/PhysRevC.17.628
Citations: PlumX Metrics


1978ST15      Phys.Rev.Lett. 41, 465 (1978)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilansky, I.Tserruya

Effect of Nuclear Deformation on Heavy-Ion Fusion

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured fusion σ(E).

doi: 10.1103/PhysRevLett.41.465
Citations: PlumX Metrics


1978ST29      S.Afr.J.Phys. 1, 171 (1978)

R.G.Stokstad, Y.Eisen, S.Kaplanis, D.Pelte, U.Smilanski, I.Tserruya

The Effect of Nuclear Deformation on Heavy-Ion Fusion

NUCLEAR REACTIONS 148,150,152,154Sm(16O, X), E=60-75 MeV; measured σ(fusion); deduced importance of nuclear deformation.


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


1977KA26      Nucl.Phys. A293, 509 (1977)

D.Kalinsky, D.Melnik, U.Smilansky, N.Trautner, S.Weisrose, O.Dietzsch

Alpha-Transfer Reactions between Oxygen Isotopes

NUCLEAR REACTIONS 16O(16O, 12C), (18O, 14C), (18O, 22Ne), (17O, 13C), (17O, 21Ne), E(cm)=17 MeV; measured σ(θ).

doi: 10.1016/0375-9474(77)90110-5
Citations: PlumX Metrics


1977SA04      Nucl.Phys. A279, 210 (1977)

M.Samuel, U.Smilansky, B.A.Watson, Y.Eisen, A.M.Kleinfeld, D.Werdecker

Measurement of Nuclear Deformation Parameters from Elastic and Inelastic Scattering of α and 3He Ions on Te Isotopes

NUCLEAR REACTIONS 122,124,126,128Te(α, α), 128Te(3He, 3He), E=8-18 MeV; measured σ(θ, E) for ground state, first 2+ state; deduced optical model parameters. 122,124,126,128Te deduced deformations, B(E2). Enriched targets.

doi: 10.1016/0375-9474(77)90224-X
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0866.


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


1975KL09      Phys.Rev.Lett. 35, 1329 (1975)

A.M.Kleinfeld, K.P.Lieb, D.Werdecker, U.Smilansky

Measurement of the Quadrupole Moment of the First Excited 2+ State of 18O

NUCLEAR MOMENTS 18O; measured quadrupole moment of 2+ state; deduced B(E2). Reorientation effect.

doi: 10.1103/PhysRevLett.35.1329
Citations: PlumX Metrics


1974BR31      Nucl.Phys. A231, 159 (1974)

W.Bruckner, D.Husar, D.Pelte, K.Traxel, M.Samuel, U.Smilansky

Nuclear Deformations from Inelastic α-Scattering on Rare Earch Nuclei At Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 152,154Sm, 186W(α, α'), E=10-20 MeV; measured σ(E, Eα', θ). 152,154Sm, 186W levels deduced β2, β4 charge, mass deformations.

doi: 10.1016/0375-9474(74)90299-1
Citations: PlumX Metrics


1974EI05      Nucl.Phys. A236, 327 (1974)

Y.Eisen, E.Abramson, G.Engler, M.Samuel, U.Smilansky, Z.Vager

Elastic Scattering of 3He and 4He at Incident Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 110,112,113Cd, 128Te(3He, 3He), 90,91Zr, 92,94Mo, 110,111,112,113,114Cd, 128Te(α, α), E=7-17.5 MeV; measured σ(E, θ); deduced optical model parameters, α-scattering systematics. Enriched targets.

doi: 10.1016/0375-9474(74)90258-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0865.


1974LE24      Phys.Lett. 53B, 39 (1974)

S.Levit, U.Smilansky, D.Pelte

A New Semi-Classical Theory for Multiple Coulomb Excitation

NUCLEAR REACTIONS 238U(84Kr, 84Kr'γ), E=300 MeV; calculated Coulomb excitation probabilities.

doi: 10.1016/0370-2693(74)90338-4
Citations: PlumX Metrics


1973AL10      Ann.Phys.(New York) 78, 518 (1973)

K.Alder, F.Roesel, U.Smilansky

Deviations from the Rutherford Scattering Due to the Ground State Quadrupole Moment

doi: 10.1016/0003-4916(73)90270-4
Citations: PlumX Metrics


1973BR02      Phys.Rev.Lett. 30, 57 (1973)

W.Bruckner, J.G.Merdinger, D.Pelte, U.Smilansky, K.Traxel

Nuclear Deformations from the Interference Effects between Coulomb and Nuclear Excitations in Inelastic α Scattering on 152Sm

NUCLEAR REACTIONS 152Sm(α, α'), E=11-18 MeV; measured σ(E). 152Sm deduced B(EL), deformation parameters β2, β4.

doi: 10.1103/PhysRevLett.30.57
Citations: PlumX Metrics


1972BA77      Nucl.Phys. A194, 193 (1972)

A.Bamberger, G.Jansen, B.Povh, D.Schwalm, U.Smilansky

Coulomb Excitation of the 1/2- State in 7Li

NUCLEAR REACTIONS 208Pb(7Li, 7Li)208Pb, E(7Li)=18-22 MeV; measured σ at angles 170° > θ > 50°. 7Li deduced B(E2); estimated Q3/2. Enriched targets.

doi: 10.1016/0375-9474(72)91059-7
Citations: PlumX Metrics


1972BE66      Nucl.Phys. A196, 312 (1972)

Z.Berant, R.A.Eisenstein, Y.Horowitz, U.Smilansky, P.N.Tandon, J.S.Greenberg, A.M.Kleinfeld, H.G.Maggi

The Reorientation Effect in 110Cd and 114Cd

NUCLEAR REACTIONS 110,114Cd(α, α'), Eα=8-16 MeV; 110,114Cd(16O, 16O'), E(16O)=36-45 MeV; measured Coulomb excitation probability. 110,114Cd levels deduced B(E2), Q2+. Enriched targets.

doi: 10.1016/0375-9474(72)90967-0
Citations: PlumX Metrics


1972EI07      Nucl.Phys. A195, 513 (1972)

Y.Eisen, R.A.Eisenstein, U.Smilansky, Z.Vager

Elastic Scattering of 16O and 18O by Even Ca Isotopes, 52Cr and 62Ni at Incident Energies Near the Coulomb Barrier

NUCLEAR REACTIONS 62Ni, 52Cr, 48,44,40Ca(18O, 18O), 62Ni, 52Cr(16O, 16O), E=25-42 MeV; measured σ(θ, E) at backward angles; deduced differences between 16O, 18O. Enriched targets.

doi: 10.1016/0375-9474(72)91073-1
Citations: PlumX Metrics


1972SM02      Phys.Lett. 38B, 293 (1972)

U.Smilansky, B.Povh, K.Traxel

The Role of the α + t Channel in the Coulomb Excitation of the 1/2- State in 7Li

NUCLEAR REACTIONS 3H(α, γ), E=0.5-8 MeV; calculated σ. 208Pb(7Li, 7Li'), E=20, 22 MeV; analyzed B(E2); studied α+t virtual excitation. 7Li deduced quadrupole moment, B(E2).

doi: 10.1016/0370-2693(72)90249-3
Citations: PlumX Metrics


1971BE36      Phys.Rev.Lett. 27, 110 (1971)

Z.Berant, R.A.Eisenstein, J.S.Greenberg, Y.Horowitz, U.Smilansky, P.N.Tandon, A.M.Kleinfeld, H.G.Maggi

Investigation of the Reorientation Effect in Cd110 and Cd114

NUCLEAR REACTIONS 110,114Cd(α, α'), E = 8-16 MeV; (16O, 16O'), E = 37-48 MeV; measured σ(E;Eα'), σ(E; E(16O')). 110,114Cd levels deduced B(E2), quadrupole moment.

doi: 10.1103/PhysRevLett.27.110
Citations: PlumX Metrics


1969SI15      Nucl.Phys. A138, 529 (1969)

J.J.Simpson, U.Smilansky, D.Ashery

Coulomb Excitation and the Reorientation Effect in 70Ge and 76Ge

NUCLEAR REACTIONS 70,76Ge(α, α'), E = 5-11 MeV; 70,76Ge(16O, 16O'), E = 25, 34-43 MeV; measured σ(E;Eα'), σ(E;E(16O')). 70,76Ge levels deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(69)90236-X
Citations: PlumX Metrics


1968SI05      Phys.Letters 27B, 633 (1968); Erratum Phys.Letters 28B, 422 (1969)

J.J.Simpson, U.Smilansky, J.P.Wurm

The Reorientation Effect in 114Cd

NUCLEAR STRUCTURE 114Cd; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90300-6
Citations: PlumX Metrics


1965GO06      Phys.Letters 16, 151 (1965)

G.Goldring, U.Smilansky

The Quadrupole Moment of the 2+ State at 122 keV in 152Sm

NUCLEAR STRUCTURE 152Sm; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)90163-0
Citations: PlumX Metrics


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