NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of May 24, 2024.

Search: Author = S.G.Nilsson

Found 37 matches.

Back to query form



1980OL04      Phys.Lett. 90B, 193 (1980)

P.Olanders, S.G.Nilsson, P.Moller

Muon Excitation Probabilities in Muon-Induced Fission of Uranium Nuclei

NUCLEAR REACTIONS U(μ-, F), E=0; calculated muon excitation probability. Time-dependent Schrodinger equation, two point charges.

doi: 10.1016/0370-2693(80)90721-2
Citations: PlumX Metrics


1979CE01      Nucl.Phys. A315, 269 (1979)

M.Cerkaski, J.Dudek, P.Rozmej, Z.Szymanski, S.G.Nilsson

Particle-Hole Structure of Nuclear Isomers at High Angular Momenta

NUCLEAR STRUCTURE 152Dy; calculated energies, magnetic moments of high-spin isomers. Deformed Woods-Saxon potential, axial symmetry.

doi: 10.1016/0375-9474(79)90611-0
Citations: PlumX Metrics


1978AN17      Nucl.Phys. A309, 141 (1978)

C.G.Andersson, G.Hellstrom, G.Leander, I.Ragnarsson, S.Aberg, J.Krumlinde, S.G.Nilsson, Z.Szymanski

Islands of High-Spin Yrast Isomers

NUCLEAR STRUCTURE 74,78,82,86,90,94Kr; calculated yrast spin trajectories. 74Kr, 176Hf, 196Hg, 204Pb, 212Rn, 218Th; calculated potential energy surfaces. 151Dy, 152Dy, 176Hf; calculated yrast spectrum. 204Pb, 212Rn; calculated energies, level properties. Likely candidates for yrast traps, trap mechanisms discussed. Modified oscillator, RPA, BCS models.

doi: 10.1016/0375-9474(78)90540-7
Citations: PlumX Metrics


1978PL03      Nucl.Phys. A301, 477 (1978)

M.Ploszajczak, A.Faessler, G.Leander, S.G.Nilsson

Description of the Yrast Traps at Very High Angular Momenta

NUCLEAR STRUCTURE 148Sm, 150Gd, 158Yb; calculated deformation energy surfaces, angular momentum, β2, β4.

doi: 10.1016/0375-9474(78)90063-5
Citations: PlumX Metrics


1977CE03      Phys.Lett. 70B, 9 (1977)

M.Cerkaski, J.Dudek, Z.Szymanski, C.G.Andersson, G.Leander, S.Aberg, S.G.Nilsson, I.Ragnarsson

Search for the Yrast Traps in Neutron Deficient Rare Earth Nuclei

NUCLEAR STRUCTURE 148,150,152Gd, 152Dy, 156,158Er, 158,160,162Yb; calculated yrast energies.

doi: 10.1016/0370-2693(77)90331-8
Citations: PlumX Metrics


1976AN10      Nucl.Phys. A268, 205 (1976)

G.Andersson, S.E.Larsson, G.Leander, P.Moller, S.G.Nilsson, I.Ragnarsson, S.Aberg, R.Bengtsson, J.Dudek, B.Nerlo-Pomorska, K.Pomorski, Z.Szymanski

Nuclear Shell Structure at Very High Angular Momentum

NUCLEAR STRUCTURE 24Mg, 114,116,118Te, 122,124,126Xe, 122,124,126,128,130,138Ba, 150Gd, 150,154Sm, 158,160,164,166,168Yb, 178W, 182,178,186,190Os, 204Pb, 160Er, 298Fl; calculated potential energy surfaces, shell structure.

doi: 10.1016/0375-9474(76)90461-9
Citations: PlumX Metrics


1976AN15      Phys.Lett. 65B, 209 (1976)

G.Andersson, S.E.Larsson, G.Leander, S.G.Nilsson, I.Ragnarsson, S.Aberg

Superheavy Elements and Variations in the Nuclear Skin Thickness

NUCLEAR STRUCTURE A > 200; calculated skin thickness parameters.

doi: 10.1016/0370-2693(76)90164-7
Citations: PlumX Metrics


1976RA02      Phys.Rev. C13, 229 (1976)

J.Randrup, S.E.Larsson, P.Moller, S.G.Nilsson, K.Pomorski, A.Sobiczewski

Spontaneous-Fission Half-Lives for Even Nuclei with Z ≥ 92

RADIOACTIVITY, Fission 232,234,236,238U, 236,238,240,242,244Pu, 240,242,244,246,248,250Cm, 246,248,250,252,254Cf, 244,246,248,250,252,254,256,258,260,262,264Fm, 252,254,256,258No; calculated (SF)T1/2. 252,254,256,258No, 256,258,260,262Rf, 260,262,264,266Sg, 260,262,264,266,268,270Hs; calculated Qα, α-decay T1/2.

doi: 10.1103/PhysRevC.13.229
Citations: PlumX Metrics


1975BE35      Phys.Lett. 57B, 301 (1975)

R.Bengtsson, S.E.Larsson, G.Leander, P.Moller, S.G.Nilsson, S.Aberg, Z.Szymanski

Yrast Bands and High-Spin Potential-Energy Surfaces

NUCLEAR STRUCTURE 146Sm, 160Yb; calculated yrast bands, energy surfaces.

doi: 10.1016/0370-2693(75)90455-4
Citations: PlumX Metrics


1974MO18      Nucl.Phys. A229, 292 (1974)

P.Moller, S.G.Nilsson, J.R.Nix

Calculated Ground-State Properties of Heavy Nuclei

NUCLEAR STRUCTURE 208Pb, 231Th, 233Pa, 240Pu, 245Cm, 249Bk; calculated single particle energies. A=68-108 calculated ground state deformations, single particle corrections.

doi: 10.1016/0375-9474(74)90789-1
Citations: PlumX Metrics


1974NI04      Nucl.Phys. A222, 221 (1974)

S.G.Nilsson, J.R.Nix, P.Moller, I.Ragnarsson

How Much of a Bubble Is There in 184Hg (Question)

NUCLEAR STRUCTURE 184Hg; calculated shape.

doi: 10.1016/0375-9474(74)90389-3
Citations: PlumX Metrics


1973LA36      Phys.Lett. 47B, 422 (1973)

S.E.Larsson, G.Leander, S.G.Nilsson, I.Ragnarsson, R.K.Sheline

Axial Asymmetry and the Spectrum of 16O

NUCLEAR STRUCTURE 16O; calculated moment of inertia, levels.

doi: 10.1016/0370-2693(73)90103-2
Citations: PlumX Metrics


1973RA38      Nucl.Phys. A217, 221 (1973)

J.Randrup, C.F.Tsang, P.Moller, S.G.Nilsson, S.E.Larsson

Theoretical Predictions of Fission Half-Lives of Elements with Z between 92 and 106

NUCLEAR STRUCTURE U, Pu, Cm, Cf, Fm, No, Rf, Sg; calculated spontaneous fission T1/2.

doi: 10.1016/0375-9474(73)90192-9
Citations: PlumX Metrics


1972BO34      Phys.Lett. 40B, 517 (1972)

R.Boleu, S.G.Nilsson, R.K.Sheline, K.Takahashi

On the Termination of the r-Process and the Synthesis of Superheavy Elements

RADIOACTIVITY, Fission Z=90-118; analyzed potential energy surfaces, T1/2(SF), T1/2(α), T1/2(β).

doi: 10.1016/0370-2693(72)90470-4
Citations: PlumX Metrics


1972LA05      Phys.Lett. 38B, 269 (1972)

S.E.Larson, I.Ragnarsson, S.G.Nilsson

Fission Barriers and the Inclusion of Axial Asymmetry

NUCLEAR STRUCTURE, Fission 186,188,190,192W, 196Pt, 196Hg, 196,204Pb, 242Pu, 246Cm, 252Fm, 258Rf; calculated potential energy surfaces vs deformation parameters, fission barriers. Modified oscillator model, axial symmetry.

doi: 10.1016/0370-2693(72)90243-2
Citations: PlumX Metrics


1972MO20      Phys.Lett. 40B, 329 (1972)

P.Moller, S.G.Nilsson, R.K.Sheline

Octupole Deformations in the Nuclei Beyond 208Pb

NUCLEAR STRUCTURE 208Pb; calculated quadrupole-octupole potential energy surface.

doi: 10.1016/0370-2693(72)90812-X
Citations: PlumX Metrics


1972NI17      Phys.Scr. 6, 81 (1972)

S.G.Nilsson, J.Damgaard

The Present Status in Super-Heavy Element Calculations

doi: 10.1088/0031-8949/6/2-3/001
Citations: PlumX Metrics


1972SH22      Phys.Lett. 41B, 115 (1972)

R.K.Sheline, I.Ragnarsson, S.G.Nilsson

Shell Structure for Deformed Nuclear Shapes

NUCLEAR STRUCTURE 32S, 40Ca, 56Ni, Zr, Mo; A=32-110; calculated levels. Harmonic oscillator, deformed nuclear shape.

doi: 10.1016/0370-2693(72)90440-6
Citations: PlumX Metrics


1971GU04      Phys.Lett. 34B, 349 (1971)

C.Gustafsson, P.Moller, S.G.Nilsson

The Microscopic Mechanism Behind the Fission Barrier Asymmetry

NUCLEAR STRUCTURE A ≈ 242; calculated energy stability at second barrier peak.

doi: 10.1016/0370-2693(71)90621-6
Citations: PlumX Metrics


1970JO29      Ann.Phys.(Paris) 5, 377 (1970)

T.Johansson, S.G.Nilsson, Z.Szymanski

Theoretical Predictions Concerning Superheavy Elements

NUCLEAR STRUCTURE, Fission Sg, Hs, Ds; Z=112, 114, 120; calculated T1/2(SF), potential energy surfaces, single-particle levels.


1970MO05      Phys.Lett. 31B, 283 (1970)

P.Moller, S.G.Nilsson

The Fission Barrier and Odd-Multipole Shape Distortions

NUCLEAR STRUCTURE, Fission 210Po, 236U, 242Pu, 252Fm; calculated potential energy surfaces.

doi: 10.1016/0370-2693(70)90171-1
Citations: PlumX Metrics


1970RA35      Nucl.Phys. A158, 155 (1970)

I.Ragnarsson, S.G.Nilsson

The Low-Energy Spectrum of 29Si and the Existence of Large Oblate Distortions Associated with Certain Intrinsic Orbitals

NUCLEAR STRUCTURE 29Si; calculated levels, total energy, potential energy surface.

doi: 10.1016/0375-9474(70)90059-X
Citations: PlumX Metrics


1970TS01      Nucl.Phys. A140, 275 (1970)

C.F.Tsang, S.G.Nilsson

Shape Isomeric States in Heavy Nuclei

NUCLEAR STRUCTURE A=174-256; calculated potential energy surface, two-peaked fission barriers, total potential energy, T1/2.

doi: 10.1016/0375-9474(70)90326-X
Citations: PlumX Metrics


1970TS02      Nucl.Phys. A140, 289 (1970)

C.F.Tsang, S.G.Nilsson

Further Theoretical Results on the Stability of Superheavy Nuclei

NUCLEAR STRUCTURE, Fission A=280-332; calculated potential energy surfaces, masses, T1/2(α), T1/2(SF), neutron-, proton-binding energies.

doi: 10.1016/0375-9474(70)90327-1
Citations: PlumX Metrics


1969MO19      Phys.Letters 30B, 223 (1969)

P.Moller, S.G.Nilsson, A.Sobiczewski, Z.Szymanski, S.Wycech

Nonperturbative Treatment of the P3 Degree of Freedom of the Nuclear Potential at Equilibrium and Fission Distortions

NUCLEAR STRUCTURE 236U, 244Cm, 252Fm; calculated energy surface, octupole stiffness parameter. Strutinsky method.

doi: 10.1016/0370-2693(69)90422-5
Citations: PlumX Metrics


1969NI12      Phys.Letters 30B, 437 (1969)

S.G.Nilsson, G.Ohlen, C.Gustafson, P.Moller

On a New Type of Fission-Isomeric State

NUCLEAR STRUCTURE, Fission 241Pu(SF); calculated potential energy surface, T1/2.

doi: 10.1016/0370-2693(69)90162-2
Citations: PlumX Metrics


1969NI13      Nucl.Phys. A131, 1 (1969)

S.G.Nilsson, C.F.Tsang, A.Sobiczewski, Z.Szymanski, S.Wycech, C.Gustafson, I.-L.Lamm, P.Moller, B.Nilsson

On the Nuclear Structure and Stability of Heavy and Superheavy Elements

doi: 10.1016/0375-9474(69)90809-4
Citations: PlumX Metrics


1969WY02      Izv.Akad.Nauk SSSR, Ser.Fiz. 33, 1263 (1969); Bull.Acad.Sci.USSR, Phys.Ser. 33, 1169 (1970)

S.Wycech, A.Sobiczewski, Z.Szymanski, S.G.Nilsson, J.R.Nix, H.F.Tsang, C.Gustafson, P.Moller, B.Nilsson

Microscopic Values for the Mass Parameter of Heavy and Superheavy Nuclei

NUCLEAR STRUCTURE 228,230,232,234Th, 230,232,234,236,238,240U, 234,236,238,240,242,244,246Pu, 238,240,242,244,246,248,250,252Cm, 244,246,248,250,252,254,256Cf, 248,250,252,254,256,258,260Fm, 250,252,254,256,258No, 258,260,262Rf; calculated mass parameter.


1968MO30      Phys.Lett. B 26, 418 (1968)

P.Moller, B.Nilsson, S.G.Nilsson, A.Sobiczewski, Z.Szymanski, S.Wycech

Hexadecapole equilibrium distortions of nuclei

NUCLEAR STRUCTURE 230,232Th, 234,236,238U, 236,238,240,242Pu, 242,244,246,248Cm, 248,250,252Cf, 252,254Fm, 262No, 266Rf, 270,272Sg; calculated hexadecapole deformation parameters with nuclear deformed shell model. Comparison with available data.

doi: 10.1016/0370-2693(68)90582-0
Citations: PlumX Metrics


1968PR06      Nucl.Phys. A110, 257 (1968)

O.Prior, F.Boehm, S.G.Nilsson

Collective Gyromagnetic Ratios of Deformed Nuclei

doi: 10.1016/0375-9474(68)90536-8
Citations: PlumX Metrics


1965NA07      Alpha-, Beta- and Gamma-Ray Spectroscopy, Vol.1, K.Siegbahn, Ed., North-Holland Publishing Co., Amsterdam, p.601 (1965)

O.Nathan, S.G.Nilsson

Collective Nuclear Motion and the Unified Model


1962KR07      Nucl.Phys. 35, 273 (1962)

G.Kramer, S.G.Nilsson

The Penetration Effect in Electric Dipole Internal Conversion

doi: 10.1016/0029-5582(62)90112-8
Citations: PlumX Metrics


1961NI13      Kgl.Dan.Vidensk.Selsk.Mat.-Fys.Medd. 32, No.16 (1961)

S.G.Nilsson, O.Prior

The effect of pair correlation on the moment of inertia and the collective gyromagnetic ratio of deformed nuclei

NUCLEAR STRUCTURE Z=62-74; Z>88; calculated the moment of inertia and the collective gyromagnetic ratio of even-even nuclei are calculated on the basis of wave functions that take a pairing interaction into account through the quasi-particle formalism.


1959MO14      Kgl.Danske Videnskab.Selskab, Mat.fys.Skrifter 1, No.8 (1959)

B.R.Mottelson, S.G.Nilsson

The Intrinsic States of Odd-A Nuclei Having Ellipsoidal Equilibrium Shape


1958NI35      Nuclear Phys. 5, 617 (1958)

S.G.Nilsson, J.O.Rasmussen

On Anomalous Conversion Coefficients of Dipole Transitions

doi: 10.1016/0029-5582(58)90061-0
Citations: PlumX Metrics


1955NI23      Kgl.Danske Videnskab.Selskab, Mat.-fys.Medd. 29, No.16 (1955)

S.G.Nilsson

Binding States of Individual Nucleons in Strongly Deformed Nuclei


1953LA28      Phys.Rev. 92, 1501 (1953)

T.Lauritsen, T.Huus, S.G.Nilsson

Scattering of Deuterons in Helium

doi: 10.1103/PhysRev.92.1501
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1276.


Back to query form