NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Hakansson Found 16 matches. 1997RI05 Nucl.Phys. A617, 316 (1997) A.Ringbom, A.Hakansson, G.Tibell, R.Zorro, J.Blomgren, H.Conde, J.Rahm, N.Olsson, E.Ramstrom, T.Ronnqvist, O.Jonsson, L.Nilsson, P.-U.Renberg, S.Y.van der Werf, H.Lenske The 208Pb(n, p)208Tl Reaction at E(n) = 97 MeV NUCLEAR REACTIONS 208Pb(n, p), E=97 MeV; measured σ(Ep, θ). Comparison with multistep direct reaction, DWBA calculations, multipole decomposition.
doi: 10.1016/S0375-9474(97)00019-5
1995FA18 Phys.Scr. T56, 243 (1995) C.Fahlander, A.Atac, J.Blomqvist, A.Backlin, A.Hakansson, L.-O.Norlin, J.Nyberg, M.Piiparinen, D.Seweryniak On the 2485 keV γ-Ray Line in 208Pb NUCLEAR REACTIONS 208Pb(84Kr, 84Kr'), E=5 MeV/nucleon; measured γγ-coin; deduced evidence for 2.485 MeV γ-ray. 208Pb deduced no definitive evidence for transition.
doi: 10.1088/0031-8949/1995/T56/038
1994RA40 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.542 (1994) E.Ramstrom, J.Blomgren, H.Conde, J.Nilsson, N.Olsson, T.Ronnqvist, R.Zorro, A.Hakansson, A.Ringbom, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, W.Unkelbach, H.Lenske The 208-Pb(n, p)208-Tl Reaction at En=97 MeV NUCLEAR REACTIONS 208Pb(n, x), E=97 MeV; measured products, Eπ, Iπ. 208Tl; deduced σ(θ, E). Data were imported from EXFOR entry 22330.
1993OL03 Nucl.Phys. A559, 368 (1993) N.Olsson, H.Conde, E.Ramstrom, T.Ronnqvist, R.Zorro, J.Blomgren, A.Hakansson, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, A.Brockstedt, P.Ekstrom, M.Osterlund, S.Y.van der Werf, D.J.Millener, G.Szeflinska, Z.Szeflinski The 12C(n, p)12B Reaction at E(n) = 98 MeV NUCLEAR REACTIONS 12C(n, p), E=98 MeV; measured σ(Ep, θ), θ=0°-33°. 12B deduced ΔL=0-3 multipole strength distributions. DWBA calculations, multipole decomposition.
doi: 10.1016/0375-9474(93)90159-U
1993RO18 Nucl.Phys. A563, 225 (1993) T.Ronnqvist, H.Conde, N.Olsson, E.Ramstrom, R.Zorro, J.Blomgren, A.Hakansson, A.Ringbom, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, S.Y.van der Werf, W.Unkelbach, F.P.Brady The 54,56Fe(n, p)54,56Mn Reactions at E(n) = 97 MeV NUCLEAR REACTIONS 54,56Fe(n, p), E=97 MeV; measured σ(Ep, θ), σ(θ). 56,54Mn deduced Gamow-Teller, dipole strengths. Statistical multistep direct DWBA calculations multipole decomposition, comparison with RPA calculations.
doi: 10.1016/0375-9474(93)90603-U
1992CO16 Nucl.Phys. A545, 785 (1992) H.Conde, N.Olsson, E.Ramstrom, T.Ronnqvist, R.Zorro, J.Blomgren, A.Hakansson, G.Tibell, O.Jonsson, L.Nilsson, P.-U.Renberg, M.Osterlund, W.Unkelbach, J.Wambach, S.Y.van der Werf, J.Ullmann, S.A.Wender The 90Zr(n, p)90Y Reaction at E(n) = 98 MeV NUCLEAR REACTIONS 90Zr(n, p), E=98 MeV; measured σ(Ep, θ). 90Y deduced Gamow-Teller, other multipole strengths. Statistical multistep direct, DWBA calculations, multipole decomposition, comparison with RPA-DWIA calculations.
doi: 10.1016/0375-9474(92)90530-W
1990BO25 Nucl.Phys. A515, 173 (1990) W.T.A.Borghols, S.Brandenburg, J.H.Meier, J.M.Schippers, M.M.Sharma, A.van der Woude, M.N.Harakeh, A.Lindholm, L.Nilsson, S.Crona, A.Hakansson, L.P.Ekstrom, N.Olsson, R.de Leo Neutron Decay of the Giant Resonance Region in 124Sn and Especially of the Giant Monopole Resonance NUCLEAR REACTIONS 124Sn(α, α'), E=120 MeV; measured σ(θα, θn) vs excitation energy. 124Sn deduced giant resonance, neutron decay characteristics. Statistical model calculations. 124Sn(d, t), E=50 MeV; measured σ(Et). 123Sn deduced level structure, low lying hole states.
doi: 10.1016/0375-9474(90)90365-S
1990CO30 Nucl.Instrum.Methods Phys.Res. A292, 121 (1990) H.Conde, S.Hultqvist, N.Olsson, T.Ronnqvist, R.Zorro, J.Blomgren, G.Tibell, A.Hakansson, O.Jonsson, A.Lindholm, L.Nilsson, P.-U.Renberg, A.Brockstedt, P.Ekstrom, M.Osterlund, F.P.Brady, Z.Szeflinski A Facility for Studies of Neutron-Induced Reactions in the 50-200 MeV Range NUCLEAR REACTIONS 12C(n, p), E=100 MeV; measured σ(Ep, θp). Monoenergetic beam, magnetic spectrometer, large angle, momentum acceptance.
doi: 10.1016/0168-9002(90)91739-X
1990HA19 Phys.Rev. C41, 2556 (1990) A.Hakansson, A.Lindholm, L.Nilsson, J.Blomgren, P.-O.Soderman, D.M.Drake, S.A.Wender, N.Olsson 12C(n, γ0)13C Cross Section in the 8-11 MeV Region NUCLEAR REACTIONS 12C(n, γ), E=8-11 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.41.2556
1990HA21 Nucl.Phys. A512, 399 (1990) A.Hakansson, J.Blomgren, A.Likar, A.Lindholm, L.Nilsson, N.Olsson, R.Zorro The Isovector E2 Resonance in Bismuth Excited by Neutron Radiative Capture NUCLEAR REACTIONS 209Bi(n, γ), E=17.7-22 MeV; measured γ-spectra, fore-aft asymmetry. 210Bi deduced isovector quadrupole resonance, Γ, EWSR. Direct-semidirect model.
doi: 10.1016/0375-9474(90)90078-Z
1989BO34 Nucl.Phys. A504, 231 (1989) W.T.A.Borghols, S.Brandenburg, J.H.Meier, J.M.Schippers, M.M.Sharma, A.van der Woude, M.N.Harakeh, A.Lindholm, L.Nilsson, S.Crona, A.Hakansson, L.P.Ekstrom, N.Olsson, R.De Leo Particle Decay of the Giant Resonance Region in 90Zr and Especially of the Giant Monopole Resonance NUCLEAR REACTIONS 90Zr(α, α'n), (α, α'p), E=120 MeV; measured α'p-, α'n-coin. 90Zr deduced giant resonance neutron, proton decay characteristics. Statistical model calculation.
doi: 10.1016/0375-9474(89)90344-8
1989BR15 Phys.Rev. C39, 2448 (1989) S.Brandenburg, W.T.A.Borghols, A.G.Drentje, A.van der Woude, M.N.Harakeh, L.P.Ekstrom, A.Hakansson, L.Nilsson, N.Olsson, R.De Leo Evidence for a (Semi) Direct Component in the Decay of the Isoscalar Giant Monopole in 208Pb NUCLEAR REACTIONS 208Pb(α, α'n), E=120 MeV; analyzed data. 208Pb deduced isoscalar giant monopole resonance decay features. 207Pb level deduced branching ratios.
doi: 10.1103/PhysRevC.39.2448
1987BO37 Phys.Lett. 197B, 37 (1987) W.T.A.Borghols, S.Brandenburg, S.Crona, R.De Leo, L.P.Ekstrom, A.Hakansson, M.N.Harakeh, A.Lindholm, J.H.Meier, L.Nilsson, N.Olsson, J.M.Schippers, M.M.Sharma, A.van der Woude Neutron Decay of the Giant Monopole Resonance in 124Sn NUCLEAR REACTIONS 124Sn(α, α'n), E=120 MeV; measured σ(θα', θn). 124Sn deduced isoscalar giant monopole resonance neutron decay. 123Sn deduced hole state J, π, spectroscopic strength.
doi: 10.1016/0370-2693(87)90337-6
1987BR09 Nucl.Phys. A466, 29 (1987) S.Brandenburg, W.T.A.Borghols, A.G.Drentje, L.P.Ekstrom, M.N.Harakeh, A.Van Der Woude, A.Hakansson, L.Nilsson, N.Olsson, M.Pignanelli, R.De Leo Decay of the Isoscalar Giant Monopole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(α, α'n)E=120 MeV; measured σ(θ). 208Pb deduced giant monopole resonance, neutron decay characteristics. Statistical model calculations.
doi: 10.1016/0375-9474(87)90344-7
1987ZO02 Nucl.Phys. A472, 125 (1987) R.Zorro, I.Bergqvist, S.Crona, A.Hakansson, A.Likar, A.Lindholm, L.Nilsson, N.Olsson The Isovector Quadrupole Resonance in Yttrium Excited by Neutron Radiative Capture NUCLEAR REACTIONS 89Y(n, γ), E=12-27 MeV; measured γ-spectra, asymmetry. 90Y deduced isovector quadrupole resonance, Γ, EWSR. Direct-semidirect model.
doi: 10.1016/0375-9474(87)90223-5
1984BE25 Nucl.Phys. A419, 509 (1984) I.Bergqvist, R.Zorro, A.Hakansson, A.Lindholm, L.Nilsson, N.Olsson, A.Likar The Giant Isovector E2 Resonance in Calcium Observed in Radiative Neutron Capture NUCLEAR REACTIONS 40Ca(n, γ), E=7-28 MeV; measured σ(θ) vs E, γ asymmetry. 41Ca deduced isovector GQR parameters, E1, E2 interference. Direct-semidirect capture model.
doi: 10.1016/0375-9474(84)90629-8
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