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NSR database version of April 27, 2024.

Search: Author = U.Smilanski

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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 T_1/2, 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 + ^{148,150,152,154}Sm at Sub-Barrier Energies

NUCLEAR REACTIONS ^{148,150,152,154}Sm(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 ^{148,150,152,154}Sm(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 ^{148,150,152,154}Sm(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 ^{122,124,126,128}Te(α, α), ¹²⁸Te(³He, ³He), E=8-18 MeV; measured σ(θ, E) for ground state, first 2+ state; deduced optical model parameters. ^{122,124,126,128}Te 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, ^{110,111,112,113,114}Cd, 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