NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = A.Hakansson

Found 16 matches.

Back to query form



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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22740.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22243.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22244.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22204.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0651.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22129.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21908.


Back to query form