NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = S.Bjornholm Found 57 matches. 1990BA09 Phys.Rev. C41, 1495 (1990) B.B.Back, S.Bjornholm, T.Dossing, W.Q.Shen, K.D.Hildenbrand, A.Gobbi, S.P.Sorensen Relaxation of Angular Momentum in Fission and Quasifission Reactions NUCLEAR REACTIONS 16O, 26Mg, 27Al, 32S, 35Cl, 40,48Ca, Zn(238U, X), E=1285, 1404, 1595, 1785 MeV; measured γ-ray multiplicity vs fragment mass. Quasifission reactions.
doi: 10.1103/PhysRevC.41.1495
1988CH27 Nucl.Phys. A485, 136 (1988) P.Chowdhury, B.Fabricius, C.Christensen, F.Azgui, S.Bjornholm, J.Borggreen, A.Holm, J.Pedersen, G.Sletten, M.A.Bentley, D.Howe, A.R.Mokhtar, J.D.Morrison, J.F.Sharpey-Schafer, P.M.Walker, R.M.Lieder Decay of High-Spin Isomers in Os Nuclei by Barrier Penetration NUCLEAR REACTIONS 150Nd(36S, 4n), E=160 MeV; 170Er(18O, 4n), E=85 MeV; measured E(γ), I(ce), I(γ), γγ-coin, I(γ)(θ). 182,184Os deduced levels, J, π, K, g(K), configurations, T1/2. Ge-multi-array, Compton shields, pulsed beam, recoil technique.
doi: 10.1016/0375-9474(88)90526-X
1987BO10 Nucl.Phys. A466, 371 (1987) J.Borggreen, G.Sletten, S.Bjornholm, J.Pedersen, A.Del Zoppo, D.C.Radford, R.V.F.Janssens, P.Chowdhury, H.Emling, D.Frekers, T.L.Khoo Single Particle Radiation between High Spin States in 147Gd NUCLEAR REACTIONS 122Sn(30Si, 5n), E=153 MeV; measured γγ-coin, Iγ(θ), recoil distance. 147Gd deduced levels, J, π, T1/2, configurations. Ge detectors, NaI array, plunger, bunched beam.
doi: 10.1016/0375-9474(87)90447-7
1987SH11 Phys.Rev. C36, 115 (1987) W.Q.Shen, J.Albinski, A.Gobbi, S.Gralla, K.D.Hildenbrand, N.Herrmann, J.Kuzminski, W.F.J.Muller, H.Stelzer, J.Toke, B.B.Back, S.Bjornholm, S.P.Sorensen Fission and Quasifission in U-Induced Reactions NUCLEAR REACTIONS 16O, 26Mg, 27Al, 32S, 35Cl, 40,48Ca, Zn(238U, X), E=4.6-7.5 MeV/nucleon; measured σ(fragment θ, mass), σ(fragment mass, total kinetic energy); deduced complete fusion σ, mass transfer rates, reaction times. Extra push model, nuclear dissipation mechanism.
doi: 10.1103/PhysRevC.36.115
1986SH29 Europhys.Lett. 1, 113 (1986) W.Q.Shen, J.Albinski, R.Bock, A.Gobbi, S.Gralla, K.D.Hildenbrand, N.Herrmann, J.Kuzminski, W.F.J.Muller, H.Stelzer, J.Toke, B.B.Back, S.Bjornholm, S.P.Sorensen, A.Olmi, G.Guarino Characteristic Time for Mass Asymmetry Relaxation in Quasi-Fission Reactions. NUCLEAR REACTIONS 32S, 40,48Ca, Zn(238U, F), E=4.6-7.5 MeV/nucleon; measured fission fragment σ(θ) vs mass, kinetic energy; deduced mass asymmetry degree of freedom relaxation time constant, driving force, shape characteristics, dissipation mechanism.
doi: 10.1209/0295-5075/1/3/004
1985BO37 Nucl.Phys. A443, 120 (1985) J.Borggreen, G.Sletten, S.Bjornholm, J.Pedersen, R.V.F.Janssens, I.Ahmad, P.Chowdhury, T.L.Khoo, Y.H.Chung, P.J.Daly Nuclear Structure Effects in the Feeding of Yrast States of Gd, Dy and Er Nuclei NUCLEAR REACTIONS 120,122,124Sn(30Si, xn), E=145, 153 MeV; 130Te(30Si, xn), E=137 MeV; 118,120,122,124Sn(34S, xn), E=155-165 MeV; 122,124,126,128,130Te(34S, xn), E=155, 170 MeV; measured Iγ. 146,147,148,149Gd, 148,150,151,152,154,155,156Dy, 152,153,154,155,156,157,158,159,160Er deduced yrast population. Ge detector, NaI array.
doi: 10.1016/0375-9474(85)90324-0
1985LU01 Z.Phys. A320, 529 (1985) K.Lutzenkirchen, J.V.Kratz, G.Wirth, W.Bruchle, L.Dorr, K.Summerer, R.Lucas, J.Poitou, C.Gregoire, S.Bjornholm Angular Distributions in Quasi-Fission Reactions: Evidence for incomplete relaxation of the tilting mode NUCLEAR REACTIONS 208Pb(50Ti, X), E=5, 5.5 MeV/nucleon; 208Pb(56Fe, X), E=5.7-8.3 MeV/nucleon; measured σ(fragment θ, Z); deduced reaction mechanism.
1985PE01 Phys.Rev.Lett. 54, 306 (1985) J.Pedersen, B.B.Back, S.Bjornholm, J.Borggreen, M.Diebel, G.Sletten, F.Azgui, H.Emling, H.Grein, G.Seiler-Clark, W.Spreng, H.J.Wollersheim, P.Walker, S.Aberg Population of Triaxial Rotor Levels in 182Os NUCLEAR REACTIONS 48Ca, 48,50Ti(136Xe, X), E=4.3-4.8 MeV/nucleon; measured Eγ, Iγ. 182Os deduced isomer, J, T1/2, decay characteristics, K selection rule violation, yrast configuration triaxiality.
doi: 10.1103/PhysRevLett.54.306
1985PE07 Z.Phys. A321, 567 (1985) J.Pedersen, B.B.Back, S.Bjornholm, J.Borggreen, G.Sletten, F.Azgui, H.Emling, H.Grein, G.Seiler-Clark, W.Spreng, H.J.Wollersheim, P.Walker High-Spin Isomers in W and Os Nuclei; Competition between K-quantization and triaxiality NUCLEAR REACTIONS 48Ca, 48,50Ti(136Xe, X), E=584-647 MeV; measured Eγ, Iγ, γ(t). 178,180W, 182,183,180Os deduced levels, K, J, π, γ-branching, isomers.
doi: 10.1007/BF01432431
1985TO12 Nucl.Phys. A440, 327 (1985) J.Toke, R.Bock, G.X.Dai, A.Gobbi, S.Gralla, K.D.Hildenbrand, J.Kuzminski, W.F.J.Muller, A.Olmi, H.Stelzer, B.B.Back, S.Bjornholm Quasi-Fission - The Mass-Drift Mode in Heavy-Ion Reactions NUCLEAR REACTIONS, ICPND 16O, 27Al, 48Ca, 45Sc, 48Ti, 58Fe, 64Ni, 89Y(238U, X), E=5.4, 6 MeV/nucleon; measured σ(fragment θ, E, mass); deduced reaction, capture σ, model parameters. 254Fm, 265Db, 286Cn, 283113, 286Fl, 296Og, 302120, 327131 deduced T1/2, mass asymmetry relaxation degree. Extra push model.
doi: 10.1016/0375-9474(85)90344-6
1984GU11 Nucl.Phys. A424, 157 (1984) G.Guarino, A.Gobbi, K.D.Hildenbrand, W.F.J.Muller, A.Olmi, H.Sann, S.Bjornholm, G.Rudolf Mass Drift in Reactions between a Heavy and a Light Nucleus NUCLEAR REACTIONS 48Ca, 50Ti(238U, X), 208Pb(56Fe, X), E=4.6-6.1 MeV/nucleon; measured σ(fragment, θ, E, A); deduced mass drift vs energy loss, θ.
doi: 10.1016/0375-9474(84)90133-7
1984SL03 Phys.Lett. 135B, 33 (1984) G.Sletten, S.Bjornholm, J.Borggreen, J.Pedersen, P.Chowdhury, H.Emling, D.Frekers, R.V.F.Janssens, T.L.Khoo, Y.H.Chung, M.Kortelahti Nucleon Alignment to very High Spins in 147Gd: Rapid ' rotation ' of fermion system NUCLEAR REACTIONS 122Sn(30Si, 5n), E=153 MeV; measured Eγ, Iγ, γ(θ). 147Gd deduced levels, γ-branching, J, π, yrast sequence, configuration, fermion system rotation evidence.
doi: 10.1016/0370-2693(84)90448-9
1984TO08 Phys.Lett. 142B, 258 (1984) J.Toke, R.Bock, Dai Guang-xi, A.Gobbi, S.Gralla, K.D.Hildenbrand, J.Kuzminski, W.F.J.Muller, A.Olmi, W.Reisdorf, S.Bjornholm, B.B.Back Compound Nucleus Fission and Quasi-Fission in Reactions of 238U with 16O and 27Al NUCLEAR REACTIONS 16O, 27Al(238U, F), E=6 MeV/nucleon; measured fission fragment yield vs mass, θ, energy; deduced fission mechanism, fission σ.
doi: 10.1016/0370-2693(84)91194-8
1983KH03 Phys.Scr. T5, 16 (1983) T.L.Khoo, P.Chowdhury, H.Emling, D.Frekers, R.V.F.Janssens, W.Kuhn, A.Pakkanen, Y.H.Chung, P.J.Daly, Z.W.Grabowski, H.Helppi, M.Kortelahti, S.Bjornholm, J.Borggreen, J.Pedersen, G.Sletten Nuclear Shape Transitions and Some Properties of Aligned-Particle Configurations at High Spin NUCLEAR STRUCTURE 148,152,156,160Dy, 147Gd; analyzed high-spin state, effective quadrupole moment, feeding times data; deduced shape dependence on spin, neutron number. NUCLEAR REACTIONS 122Sn(30Si, 5n), E not given; measured γγ-coin. 147Gd deduced levels, γ-branching.
doi: 10.1088/0031-8949/1983/T5/003
1983PE13 Phys.Scr. T5, 162 (1983) J.Pedersen, S.Bjornholm, J.Borggreen, J.Kownacki, G.Sletten Intrinsic Excitations as Yrast Structures in 179W above I ≈ (35/2)(h-bar) NUCLEAR REACTIONS 170Er(13C, 4n), E=61-65 MeV; measured γγ-coin. 179W deduced levels, isomer T1/2, yrast band, J, π, K, configurations, deformation aligned state dominance, high-spin degeneracy.
doi: 10.1088/0031-8949/1983/T5/030
1982BJ03 Nucl.Phys. A391, 471 (1982) Dynamical Aspects of Nucleus-Nucleus Collisions NUCLEAR REACTIONS 116Sn, 141Pr(35Cl, X), 109Ag(40Ar, X), 208Pb(26Mg, X), (27Al, X), (48Ca, X), (50Ti, X), (52Cr, X), (58Fe, X), (64Ni, X), E(cm) ≈ 100-250 MeV; calculated σ(evaporation), fast, delayed fission, quasielastic σ vs E. 248Cm, 254Es, 252Cf(48Ca, X), E(cm) ≈ 200-300 MeV; calculated superheavy formation characteristics. Macroscopic theory, touching, conditional, unconditional saddle point configurations.
doi: 10.1016/0375-9474(82)90621-2
1982BO29 Nucl.Phys. A388, 334 (1982) R.Bock, Y.T.Chu, M.Dakowski, A.Gobbi, E.Grosse, A.Olmi, H.Sann, D.Schwalm, U.Lynen, W.Muller, S.Bjornholm, H.Esbensen, W.Wolfli, E.Morenzoni Dynamics of the Fusion Process NUCLEAR REACTIONS 26Mg, 27Al, 50Ti, 52Cr, 58Fe, 64Ni(208Pb, X), E=5.2-8 MeV/nucleon; measured σ(fragment θ, E) vs mass, average γ-multiplicity, E(X-ray), I(X-ray); 48Ca(208Pb, X), E=5.2-8 MeV/nucleon; measured σ(fragment θ, E) vs mass, average γ-multiplicity; deduced σ(capture), effective moment of inertia, coalescence model parameters. 234Pu, 235Am, 256Fm, 258Rf, 260Sg, 266Hs, 272Ds deduced T1/2 limits.
doi: 10.1016/0375-9474(82)90420-1
1981BA33 Phys.Scr. 24, 290 (1981) C.V.K.Baba, S.Bjornholm, O.Christensen, B.Herskind, R.M.Lieder, J.Pedersen, G.Sletten, F.Folkmann, R.S.Simon Non-Collective Properties of the Continuum Gamma Rays Feeding Two High-Spin Isomers in 152Er NUCLEAR REACTIONS 108Pd(48Ti, 4n), E=218-232 MeV; measured γγ-coin. 152Er deduced levels, isomer T1/2, γ-branching, yrast cascade γ-multipolarity, shape. Continuum γ-rays.
doi: 10.1088/0031-8949/24/1B/025
1981SA29 Phys.Rev.Lett. 47, 1248 (1981) H.Sann, R.Bock, Y.T.Chu, A.Gobbi, A.Olmi, U.Lynen, W.Muller, S.Bjornholm, H.Esbensen Deformability as a Critical Factor in Initiating Fusion between very Heavy-Ions NUCLEAR REACTIONS 26Mg, 27Al, 48Ca, 50Ti, 52Cr, 58Fe(208Pb, X), E > barrier; measured σ(fusion); deduced deformability role.
doi: 10.1103/PhysRevLett.47.1248
1980BJ02 Rev.Mod.Phys. 52, 725 (1980) The Double-Humped Fission Barrier NUCLEAR STRUCTURE A=231-245; analyzed resonance structure, fission data; deduced fission features. Double-humped fission barrier concept.
doi: 10.1103/RevModPhys.52.725
1980BO07 Z.Phys. A294, 113 (1980) J.Borggreen, S.Bjornholm, O.Christensen, A.Del Zoppo, B.Herskind, J.Pedersen, G.Sletten, F.Folkmann, R.S.Simon Gamma-Spectroscopy within the Island of High-Spin Isomers Near N=82 NUCLEAR REACTIONS 106Pd, 100Mo(50Ti, xnγ), (65Cu, xnγ), E=4.6 MeV/nucleon; measured Eγ, Iγ, γ(t), sum spectra. 144,147Gd, 148Tb, 151,152Dy, 149,150,151,152,153Ho, 151,152,153,154Er deduced levels, T1/2, J, π.
doi: 10.1007/BF01435046
1978BA33 Nucl.Phys. A302, 343 (1978) Fission Induced by Heavy-Ion Collisions NUCLEAR REACTIONS 197Au, 209Bi, 238U(α, F); calculated fragment (θ) parameters for totally, partly polarized nuclei.
doi: 10.1016/0375-9474(78)90304-4
1977PE15 Phys.Rev.Lett. 39, 990 (1977) J.Pedersen, B.B.Back, F.M.Bernthal, S.Bjornholm, J.Borggreen, O.Christensen, F.Folkmann, B.Herskind, T.L.Khoo, M.Neiman, F.Puhlhofer, G.Sletten Island of High-Spin Isomers Near N = 82 NUCLEAR STRUCTURE 146,147Gd; measured reaction γ-multiplicities, delayed S-width; deduced T1/2 of high spin isomers.
doi: 10.1103/PhysRevLett.39.990
1974BA26 Nucl.Phys. A222, 377 (1974) B.B.Back, J.Bang, S.Bjornholm, J.Hattula, P.Kleinheinz, J.R.Lien Neutron Strength Functions in Rare Earth Nuclei NUCLEAR REACTIONS 156,158,160Gd, 160,162,164Dy, 166,168,170Er, 170,172,174,176Yb(d, p), E=9 MeV; measured σ(Ep). 157,159,161Gd, 161,163,165Dy, 167,169,171Er, 171,173,175,177Yb deduced neutron strength functions.
doi: 10.1016/0375-9474(74)90397-2
1974ME10 Nucl.Instrum.Methods 114, 445 (1974) V.Metag, E.Liukkonen, G.Sletten, O.Glomset, S.Bjornholm Detection of Fission Isomers with Half-Lives in the Picosecond Range by the Recoil-Distance Technique NUCLEAR REACTIONS 237Np(p, F), 242Pu(d, pnF); measured recoil distance. 242Pu level deduced T1/2.
doi: 10.1016/0029-554X(74)90165-7
1973ME23 Nucl.Phys. A213, 397 (1973) V.Metag, S.M.Lee, E.Liukkonen, G.Sletten, S.Bjornholm, A.S.Jensen Neutron-Fission Competition Near Threshold; The Influence of Shells and Pairing on the Decay of the 241Cm Compound Nucleus NUCLEAR REACTIONS 238Pu(α, n), E=19.9-23 MeV; 238Pu(α, 2n), E=19.9-27 MeV; 241Am(p, 2n), E=8.2-16 MeV; measured σ(241Cm), σ(240Cm), σ(fission). 241,242Cm deduced n-width, F-width.
doi: 10.1016/0375-9474(73)90160-7
1973SO01 Nucl.Phys. A202, 274 (1973) The Moment of Inertia and the Energy Gap of Fission Isomers
doi: 10.1016/0375-9474(73)90224-8
1970BJ02 Nucl.Phys. A156, 561 (1970) S.Bjornholm, J.Borggreen, E.K.Hyde Search for New Islands of Fission Isomerism NUCLEAR REACTIONS 197Au(HI, X), E=5-10 MeV/nucleon for HI=11B, 12C, 14N, 16O; measured σ(E) for SF-isomers. 200,201,202,203,204Po, 201,202,203,204,205At, 202,203,204,205,206,207Rn, 202,203,204,205,206,207,208,209,210Fr deduced no SF-isomer (σ < 0.1 μb) with 2ns < T1/2<2000s.
doi: 10.1016/0375-9474(70)90252-6
1969BJ02 Nucl.Phys. A136, 1 (1969) Intermediate States in Fission
doi: 10.1016/0375-9474(69)90035-9
1969LA14 Nucl.Phys. A139, 481 (1969) N.L.Lark, G.Sletten, J.Pedersen, S.Bjornholm Spontaneously Fissioning Isomers in U, Np, Pu and Am Isotopes RADIOACTIVITY, Fission 236mU, 239mNp, 236mPu, 237mPu, 240mPu, 241mPu, 242mPu, 243mPu, 239mAm, 241mAm(SF); measured T1/2. NUCLEAR REACTIONS 235U, 239,241,242Pu(d, p), 240Pu(d, X), E=11-13 MeV; measured σ delayed fission. 237Np(p, 2n), E=9-14 MeV; 240Pu(p, 2n), E=10-13 MeV; 242Pu(p, 2n), E=8.8-13 MeV; measured σ delayed fission; deduced thresholds. 238U, 237Np(d, X), 239Pu, 241Pu(d, 2n), E=13 MeV; measured σ delayed fission. 237Np(p, 2n), E=13 MeV; measured σ ground state. Enriched targets.
doi: 10.1016/0375-9474(69)90273-5
1968BJ04 Yadern.Fiz. 8, 459 (1968); Soviet J.Nucl.Phys. 8, 267 (1969) S.Bjornholm, I.Borggreen, Y.P.Gangrskii, G.Sletten Investigation of (d, p) and (d, t) Reactions Leading to Spontaneously Fissile Isomeric States NUCLEAR REACTIONS 241,243Am(d, p), (d, t), E=9-13 MeV; measured σ(E); deduced isomeric ratio.
1968BJ05 Nucl.Phys. A118, 241 (1968) S.Bjornholm, J.Dubois, B.Elbek Energy Levels in 234U Populated by the 233U(d, p) and 235U(d, t) Processes NUCLEAR REACTIONS 233U(d, p), 235U(d, t), E=13 MeV; measured σ(Ep, 90°), σ(Ep, 125°), σ(Et, 90°), σ(Et, 125°). 234U levels deduced J, K, π, S. Enriched targets.
doi: 10.1016/0375-9474(68)90336-9
1968BJ06 Nucl.Phys. A118, 261(1968) S.Bjornholm, J.Borggreen, D.Davies, N.J.S.Hansen, J.Pedersen, H.L.Nielsen Energy Levels in 234U Populated in the β-Decay of 234Pa(UZ) RADIOACTIVITY 234Pa [from 238U decay]; measured Eγ, Eβ, Iγ, I(ce), Iβ, βγ-, γγ-, ceγ-coin, γγ-delay. 234U deduced levels, J, π. Ge(Li) detector.
doi: 10.1016/0375-9474(68)90337-0
1967BJ03 Nucl.Phys. A95, 513 (1967) S.Bjornholm, J.Borggreen, L.Westgaard, V.A.Karnaukhov Excitation Energy of the Spontaneously Fissioning Isomeric State in 240Am NUCLEAR REACTIONS 240Pu(d, 2n), E = 12.1 MeV; 240Pu(p, n), E = 10.3-11.3 MeV; measured σ (delayed fission). 241Pu(p, 2n), E = 9.6-13.6 MeV; measured σ (delayed fission); deduced threshold. Enriched target. 240mAm measured T1/2 for spontaneous fission.
doi: 10.1016/0375-9474(67)90846-9
1967BO08 Nucl.Phys. A96, 561 (1967) J.Borggreen, N.J.S.Hansen, J.Pedersen, L.Westgaard, J.Zylicz, S.Bjornholm Isomerism in 176Hf and Some Neighbouring Even Nuclei NUCLEAR REACTIONS 176Lu(p, nγ), 181Ta(p, 2nγ), E = 10, 12 MeV; measured pγ-delay. 173Yb(d, pγ), 176Yb(d, d'γ), E = 12 MeV; measured dγ-delay. 176Hf, 174,176Yb, 180W levels deduced T1/2. Enriched 176Lu, 173,176Yb targets, Ge(Li) detector. 176mHf, 174m,176mYb, 180mW; measured Eγ, Iγ, I(ce), γγ-, γce-coin, γce-delay. 176Hf, 174,176Yb, 180W deduced levels, T1/2, J, π.
doi: 10.1016/0375-9474(67)90605-7
1967BO23 Phys.Letters 25B, 402 (1967) J.Borggreen, Y.P.Gangrsky, G.Sletten, S.Bjornholm A New Spontaneously Fissioning Isomer: 238Am NUCLEAR STRUCTURE 238Am; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90158-X
1966BJ04 Priv.Comm. (1966) NUCLEAR STRUCTURE 242Am; measured not abstracted; deduced nuclear properties.
1966BO02 Nucl.Phys. 77, 619 (1966) J.Borggreen, H.J.Frahm, N.J.S.Hansen, S.Bjornholm Lifetimes of E3 Transitions in the Odd-Mass Ho Isotopes RADIOACTIVITY 159Ho, 161Ho, 163Ho isomers [from 160Dy, 161Dy, 162Dy, 163Dy(p, n)(p, 2n)], measured Eγ, Iγ, ce, ICC, T1/2. 159Ho, 161Ho, 163Ho deduced level , J, π. Enriched targets. 160Dy, 161Dy, 162Dy, 163Dy (p, n)(p, 2n), E=9-13 MeV; measured σ, p, isomer. Enriched targets.
doi: 10.1016/0029-5582(66)90787-5
1966BR23 Nucl.Phys. 89, 267 (1966) D.S.Brenner, L.Westgaard, S.Bjornholm A Study of Nuclear Isomers Which Decay by Spontaneous Fission RADIOACTIVITY 242Am isomer [from 242Pu(d, 2n)]; measured T1/2(SF), E(fragment)-spectrum. Enriched target. 242Pu(d, 2n), (d, F), E = 12 MeV; measured σ(F)(delayed)/σ(F)(prompt). Enriched target. 232Th, 235U, 239Pu, 241Am, 243Am(d, xn)(d, F), E = 12 MeV; 243Am(p, xn)(p, F), E = 13 MeV; measured upper limits σ(F)(delayed)/σ(F)(prompt). Enriched targets.
doi: 10.1016/S0029-5582(66)80089-5
1965BJ01 Nucl.Phys. 73, 593 (1965) S.Bjornholm, J.Borggreen, H.J.Frahm, N.J.S.Hansen Isomers in Odd-Mass Lu Isotopes, Ascribed to the (541)1/2- Nilsson Configuration RADIOACTIVITY 169,171,173,175Lu [from 170,171,173,176Yb (p, xn)]; measured T1/2, Eγ, ICC. 169,171,173,175Lu deduced levels, J, π. Enriched targets.
doi: 10.1016/0029-5582(65)90704-2
1965BJ03 Phys.Rev. 140, B816 (1965) S.Bjornholm, J.Borggreen, H.J.Frahm, N.J.S.Hansen, O.Schult Decay of the 185-μsec Isomer in Ho166 NUCLEAR STRUCTURE 166Ho; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.140.B816
1965BO22 Nucl.Phys. 72, 509 (1965) J.Borggreen, H.J.Frahm, N.J.S.Hansen, S.Bjornholm Observation of the (505)11/2- Nilsson State as an Isomer in 159Dy NUCLEAR REACTIONS 159Tb(p, n), E = 8-12 MeV; 159Tb(d, 2n) E = 12 MeV; Gd(α, xn), E = 18 MeV; measured σ(Ep), pγ-delay. 159Dy deduced T1/2. 159Dy; measured Eγ, Iγ, ICC. 159Dy deduced levels, J, π.
doi: 10.1016/0029-5582(65)90407-4
1964AS01 Phys. Rev. 133, B291 (1964) F.Asaro, S.Bjornholm, I.Perlman Decay Scheme of Fm255 NUCLEAR STRUCTURE 255Fm; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B291
1963BJ01 Nucl.Phys. 42, 469 (1963) S.Bjornholm, F.Boehm, A.B.Knutsen, O.B.Nielsen Levels in U232 Excited in the β Decay of Pa232 NUCLEAR STRUCTURE 232Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90750-8
1963BJ02 Nucl.Phys. 42, 642 (1963) The Decay of the 1.14 min Isomer of Pa234 (UX2) NUCLEAR STRUCTURE 234Th, 234Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90766-1
1963BJ03 Phys.Rev. 130, 2000 (1963) S.Bjornholm, C.M.Lederer, F.Asaro, I.Perlman Alpha Decay to Vibrational States NUCLEAR STRUCTURE 234U, 242Cm, 244Cm, 252Cf, 238Pu, 239Pu, 254Fm, 253Es; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.2000
1963HA30 Nucl.Phys. 45, 417 (1963) P.G.Hansen, K.Wilsky, S.Bjornholm Decay of an Isomeric State in U234 NUCLEAR STRUCTURE 234Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90816-2
1962BJ01 Nuclear Phys. 30, 488 (1962) A Study of the β-Decay of Pa234 (UZ) NUCLEAR STRUCTURE 234Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90073-1
1961AR14 Nuclear Phys. 27, 352 (1961); Erratum Nuclear Phys. 21, 406 (1960) E.Arbman, S.Bjornholm, O.B.Nielsen Levels in Th228 in the Electron Capture Decay of Pa228 NUCLEAR STRUCTURE 228Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90356-X
1961BJ01 Bull.Am.Phys.Soc. 6, No.3, 239, E9 (1961) S.Bjornholm, A.B.Knutsen, O.B.Nielsen Rotational and Vibrational Levels in U232 NUCLEAR STRUCTURE 232Pa; measured not abstracted; deduced nuclear properties.
1961BJ02 J.Inorg.Nuclear Chem. 21, 193 (1961) S.Bjornholm, H.L.Nielsen, O.B.Nielsen, G.Sidenius, O.Skilbreid, A.Svanheden Some Neutron-Deficient Isotopes of Thulium and Erbium. A Survey of Half-Lives and Gamma-Ray Spectra with the Use of Mass-Separated Samples NUCLEAR STRUCTURE 159Dy, 162Tm, 161Ho, 160Er, 167Tm, 166Tm, 163Er, 163Ho, 163Tm, 165Er, 164Tm, 168Tm, 169Er, 165Tm; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(61)80292-3
1961NI12 Quoted in 64Hy02, p.679 (1961); Priv.Comm. (1970) O.B.Nielsen, H.Nordby, S.Bjornholm NUCLEAR STRUCTURE 230Pa; measured not abstracted; deduced nuclear properties.
1960AR06 Nuclear Phys. 21, 406 (1960) E.Arbman, S.Bjornholm, O.B.Nielsen Levels in Th228 Excited in the Electron Capture Decay of Pa228 NUCLEAR STRUCTURE 228Pa; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90066-3
1960BE25 Kgl.Danske Videnskab.Selskab, Mat.-fys.Medd. 32, No.12 (1960) R.E.Bell, S.Bjornholm, J.C.Severiens Half Lives of First Excited States of Even Nuclei of Fm, Ra, Th, U, and Pu NUCLEAR STRUCTURE 233U, 232Th, 232U, 234Th, 236Pu, 236U, 234U, 220Rn, 222Th, 218Rn, 222Ra, 224Ra, 222Rn, 230Pa, 230Th, 230U, 228Th, 228Ac, 226Ra, 228Ra, 226Th, 242Cm, 244Cm, 240Pu, 238U, 238Pu; measured not abstracted; deduced nuclear properties.
1960TO10 J.Inorg.Nuclear Chem. 14, 1 (1960) K.S.Toth, S.Bjornholm, M.H.Jorgensen, O.B.Nielsen, O.Skilbreid, A.Svanheden The Light Terbium Isotopes. A Survey of Half-Lives and γ-Ray Spectra With the Use of Mass-Separated Samples NUCLEAR STRUCTURE 150Tb, 151Tb, 152Tb, 149Tb; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0022-1902(60)80190-X
1959BJ39 Phys.Rev. 115, 1613 (1959) S.Bjornholm, O.B.Nielsen, R.K.Sheline Levels in Zr90: Experimental
doi: 10.1103/PhysRev.115.1613
1959TO29 Phys.Rev. 116, 118 (1959) K.S.Toth, S.Bjornholm, M.Jorgensen, O.B.Nielsen, O.Skilbreid Tb150: A New Terbium Isotope
doi: 10.1103/PhysRev.116.118
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