NSR Query Results
Output year order : Descending NSR database version of March 18, 2024. Search: Author = S.Brandenburg Found 54 matches. 2010HY01 Phys.Rev. C 81, 024303 (2010) S.Hyldegaard, M.Alcorta, B.Bastin, M.J.G.Borge, R.Boutami, S.Brandenburg, J.Buscher, P.Dendooven, C.Aa.Diget, P.Van Duppen, T.Eronen, S.P.Fox, L.M.Fraile, B.R.Fulton, H.O.U.Fynbo, J.Huikari, M.Huyse, H.B.Jeppesen, A.S.Jokinen, B.Jonson, K.Jungmann, A.Kankainen, O.S.Kirsebom, M.Madurga, I.Moore, A.Nieminen, T.Nilsson, G.Nyman, G.J.G.Onderwater, H.Penttila, K.Perajarvi, R.Raabe, K.Riisager, S.Rinta-Antila, A.Rogachevskiy, A.Saastamoinen, M.Sohani, O.Tengblad, E.Traykov, Y.Wang, K.Wilhelmsen, H.W.Wilschut, J.Aysto R-matrix analysis of the β decays of 12N and 12B RADIOACTIVITY 12N(β+), 12B(β-); measured 3α summed spectra and associated branching ratios for breakup via the 8Be ground-state and via excited states of 8Be. 12C; deduced levels, resonances, Gammow-Teller strengths and widths using multilevel, many-channel R-matrix formalism.
doi: 10.1103/PhysRevC.81.024303
2009HY01 Phys.Lett. B 678, 459 (2009) S.Hyldegaard, C.Forssen, C.Aa.Diget, M.Alcorta, F.C.Barker, B.Bastin, M.J.G.Borge, R.Boutami, S.Brandenburg, J.Buscher, P.Dendooven, P.Van Duppen, T.Eronen, S.Fox, B.R.Fulton, H.O.U.Fynbo, J.Huikari, M.Huyse, H.B.Jeppesen, A.Jokinen, B.Jonson, K.Jungmann, A.Kankainen, O.Kirsebom, M.Madurga, I.Moore, P.Navratil, T.Nilsson, G.Nyman, G.J.G.Onderwater, H.Penttila, K.Perajarvi, R.Raabe, K.Riisager, S.Rinta-Antila, A.Rogachevskiy, A.Saastamoinen, M.Sohani, O.Tengblad, E.Traykov, J.P.Vary, Y.Wang, K.Wilhelmsen, H.W.Wilschut, J.Aysto Precise branching ratios to unbound 12C states from 12N and 12B β-decays NUCLEAR REACTIONS 1H(12C, n), 2H(11B, p), 12C(p, n), 11B(d, p), E not given; measured Eγ, Iγ, Eα, Iα, γα-coin, αα-coin, decay spectra; deduced branching ratio, log ft, B(GT) to various 12C states. Comparison with no-core shell model calculations. RADIOACTIVITY 12B(β-), 12N(β+); deduced branching ratio, log ft, B(GT) to various 12C states. Comparison with no-core shell model calculations.
doi: 10.1016/j.physletb.2009.06.064
2008HY03 Int.J.Mod.Phys. E17, 2182 (2008) S.Hyldegaard, H.O.U.Fynbo, K.Riisager, S.Brandenburg, P.Dendooven, K.Jungmann, C.J.G.Onderwater, A.Rogachevskiy, M.Sohani, E.Traykov, H.W.Wilschut, J.Buscher, M.Huyser, R.Raabe, M.Alcorta, M.J.G.Borge, M.Madurga, O.Tengblad, C.A.A.Diget, B.R.Fulton, A.S.Jokinen, K.Perajarvi, A.Saastamoinen, J.Aysto, B.Jonson, G.Nyman Studies of 12C using β-decays NUCLEAR REACTIONS 1H(12C, X)12N, 2H(11B, X)12B, E not given; measured Eα, Iα; deduced branching ratios, Gamow-Teller transition strengths.
doi: 10.1142/S0218301308011318
2006GU02 Phys.Rev. C 73, 014616 (2006) J.Guillot, S.Gales, D.Beaumel, S.Fortier, E.Rich, N.Van Giai, G.Colo, A.M.van den Berg, S.Brandenburg, B.Davids, M.N.Harakeh, M.Hunyadi, M.de Huu, S.Y.van der Werf, H.J.Wortche, C.Baumer, D.Frekers, E.-W.Grewe, P.Haefner, B.C.Junk, M.Fujiwara The (t, 3He) reaction at 43 MeV/nucleon on 48Ca and 58Ni: Results and microscopic interpretation NUCLEAR REACTIONS 12C, 48Ca, 58Ni(t, 3He), E=43 MeV/nucleon; measured excitation energy spectra, σ(E, θ). 48K, 58Co deduced giant resonance features.
doi: 10.1103/PhysRevC.73.014616
2005AL32 Nucl.Instrum.Methods Phys.Res. A547, 616 (2005) O.Alyakrinskiy, A.Andrighetto, M.Barbui, S.Brandenburg, M.Cinausero, B.Dalena, P.Dendooven, E.Fioretto, G.Lhersonneau, W.Lyapin, G.Prete, G.Simonetti, L.Stroe, L.B.Tecchio, W.H.Trzaska Neutron yield from a thick 13C target irradiated by 90 MeV protons NUCLEAR REACTIONS 13C(p, nX), E=90 MeV; measured En, σ(E, θ), thick-target yield.
doi: 10.1016/j.nima.2005.03.161
2005GU11 Nucl.Phys. A752, 349c (2005) J.Guillot, C.Baumer, D.Beaumel, A.M.van den Berg, S.Brandenburg, G.Colo, B.Davids, S.Fortier, D.Frekers, E.-W.Grewe, M.Fujiwara, S.Gales, P.Haefner, M.N.Harakeh, M.Hunyadi, M.de Huu, B.C.Junk, E.Rich, N.Van Giai, S.Y.van der Werf, H.J.Wortche Investigation of Isovector Excitations via the (t, 3He) reaction at Et=43 MeV/u on 58Ni and 48Ca targets: microscopic interpretation NUCLEAR REACTIONS 48Ca, 58Ni(t, 3He), E=130 MeV; analyzed particle spectra, σ(θ); deduced resonance features.
doi: 10.1016/j.nuclphysa.2005.02.044
2004GU02 Nucl.Phys. A731, 106 (2004) J.Guillot, D.Beaumel, A.M.van den Berg, S.Brandenburg, B.Davids, S.Fortier, M.Fujiwara, S.Gales, M.N.Harakeh, M.Hunyadi, M.de Huu, H.J.Wortche Investigation of IVGRs via the 58Ni(t, 3He)58Co reaction NUCLEAR REACTIONS 58Ni(t, 3He), E=130 MeV; measured particle spectra, σ(θ); deduced monopole resonance strength distribution. Comparison with RPA predictions.
doi: 10.1016/j.nuclphysa.2003.11.022
2004KR02 Nucl.Phys. A731, 224 (2004) A.Krasznahorkay, H.Akimune, A.M.van den Berg, N.Blasi, S.Brandenburg, M.Csatlos, M.Fujiwara, J.Gulyas, M.N.Harakeh, M.Hunyadi, M.de Huu, Z.Mate, D.Sohler, S.Y.van der Werf, H.J.Wortche, L.Zolnai Neutron-skin thickness in neutron rich isotopes NUCLEAR REACTIONS 208Pb(α, α'), E=196 MeV; measured Eγ, Iγ, αγ-coin; deduced GDR excitation. 112,114,116,118,120,122,124Sn(3He, t), E=177 MeV; measured triton spectra, σ(E, θ); deduced spin-dipole resonance excitation. 112,114,116,118,120,122,124Sn, 208Pb deduced neutron skin thickness, related features. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2003.11.034
2003NA09 Phys.Scr. T104, 69 (2003) P.Nadel-Turonski, A.Atac, B.Bergenwall, J.Blomgren, S.Brandenburg, S.Dangtip, C.Johansson, J.Klug, S.Kopecky, H.Laurent, L.Nilsson, J.Nyberg, N.Olsson, D.Reistad, P.-U.Renberg, L.Westerberg Studies of Inelastic Scattering of Fast Heavy Ions NUCLEAR REACTIONS Ar, Xe(17O, 17O'), E=250 MeV/nucleon; measured neutron spectra, (particle)n-coin; deduced fast neutron component.
doi: 10.1238/Physica.Topical.104a00069
2001SO04 Nucl.Phys. A683, 79 (2001) P.-O.Soderman, A.Ringbom, J.Blomgren, N.Olsson, L.Nilsson, J.A.Bordewijk, S.Brandenburg, G.van't Hof, M.A.Hofstee, H.van der Ploeg, S.Y.van der Werf, A.Krasznahorkay, A.Balanda, D.Chmielewska, H.Laurent Neutron Decay of Deep Hole States and Isobaric Analog States in 115Sn Populated by the (3He, α) Reaction at 102 MeV NUCLEAR REACTIONS 116Sn(3He, α), E=102 MeV; measured Eα, neutron spectra following residual nucleus decay, nα angular correlations. 115Sn deduced branching ratios for neutron decay from deep hole states and IAS. Comparison with statistical model calculations.
doi: 10.1016/S0375-9474(00)00469-3
2001ZE02 Phys.Rev. C63, 034613 (2001) R.G.T.Zegers, A.M.van den Berg, S.Brandenburg, M.Fujiwara, J.Guillot, M.N.Harakeh, H.Laurent, S.Y.van der Werf, A.Willis, H.W.Wilschut Excitation of the Isovector Giant Monopole Resonances via the natPb(3He, tp) Reaction NUCLEAR REACTIONS Pb(3He, pt), E=177 MeV; measured triton spectra, proton spectra following excited nucleus decay; deduced isovector giant monopole resonance excitation.
doi: 10.1103/PhysRevC.63.034613
2001ZE04 Nucl.Phys. A687, 262c (2001) R.G.T.Zegers, A.M.van den Berg, S.Brandenburg, F.R.R.Fleurot, M.Fujiwara, J.Guillot, V.M.Hannen, M.N.Harakeh, H.Laurent, K.van der Schaaf, S.Y.van der Werf, A.Willis, H.W.Wilschut Observation of the Isovector Giant Monopole Resonances in the (3He, t) Reaction NUCLEAR REACTIONS Pb(3He, t), E=177 MeV; measured σ at small angles, Ep, (proton)(triton)-coin, isovector giant monopole resonance parameters. DWBA calculations.
doi: 10.1016/S0375-9474(01)00630-3
2000ZE03 Phys.Rev.Lett. 84, 3779 (2000) R.G.T.Zegers, A.M.van den Berg, S.Brandenburg, F.R.R.Fleurot, M.Fujiwara, J.Guillot, V.M.Hannen, M.N.Harakeh, H.Laurent, K.van der Schaaf, S.Y.van der Werf, A.Willis, H.W.Wilschut Search for Isovector Giant Monopole Resonances via the Pb(3He, tp) Reaction NUCLEAR REACTIONS Pb(3He, pt), E=177 MeV; measured triton, proton spectra, tp-coin. Bi deduced isovector monopole resonance strengths. Comparison with theory.
doi: 10.1103/PhysRevLett.84.3779
2000ZE05 Phys.Rev. C61, 054602 (2000) R.G.T.Zegers, S.Brandenburg, M.N.Harakeh, S.Y.van der Werf, J.Janecke, T.O'Donnell, D.A.Roberts, S.Shaheen, G.P.A.Berg, C.C.Foster, T.Rinckel, E.J.Stephenson Search for Isovector Giant Monopole Resonances via the 124Sn(3He, tn) Reaction NUCLEAR REACTIONS 124Sn(3He, t), E=199 MeV; measured excitation energy spectra, tn-, tγ-coin following residual nucleus decay; deduced no monopole resonance strength at high excitation energy.
doi: 10.1103/PhysRevC.61.054602
1996BE16 Nucl.Phys. A599, 265c (1996) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Decay Properties of High-Lying Single-Particles Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn, 208Pb(α, n3He), E=120 MeV; measured neutron spectra, nn(θ). 91Zr, 209Pb deduced resonances, J, π, neutron decay features.
doi: 10.1016/0375-9474(96)00068-1
1995FO19 Phys.Rev. C52, 2401 (1995) S.Fortier, D.Beaumel, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche Damping of Unbound Single-Particle Modes NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn(α, 3He), E=120 MeV; measured 3He-spectra, neutron spectra following residual decay, n(3He)-coin. 91Zr, 121Sn, 65Ni deduced non-statistical neutron branching ratios. Statistical analysis.
doi: 10.1103/PhysRevC.52.2401
1995LH02 Nucl.Phys. A583, 115c (1995) I.Lhenry, D.Beaumel, S.Fortier, S.Gales, H.Laurent, J.M.Maison, F.Azaiez, Y.Blumenfeld, J.Guillot, H.Langevin-Joliot, T.Suomijarvi, S.Brandenburg, G.M.Crawley, J.Finck, J.Stasko A Search for the Isovector Monopole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(13C, 13N), E=60 MeV/nucleon; measured σ(θ), missing energy spectra. 208Tl deduced level, neutron decay features.
doi: 10.1016/0375-9474(94)00643-2
1995SO05 Nucl.Phys. A587, 55 (1995) P.-O.Soderman, J.Blomgren, A.Ringbom, N.Olsson, L.Nilsson, J.A.Bordewijk, S.Brandenburg, G.van't Hof, M.A.Hofstee, H.van der Ploeg, S.Y.van der Werf, A.Krasznahorkay, A.Balanda, D.Chmielewska, H.Laurent Neutron Decay of Deep-Hole States in 89Zr Populated by the 90Zr(3He, α)89Zr Reaction at 102 MeV NUCLEAR REACTIONS 90Zr(3He, α), E=102 MeV; measured α-spectra, αn-coin. 89Zr deduced neutron decay of hole states. Statistical model calculations.
doi: 10.1016/0375-9474(94)00818-8
1994BE07 Phys.Rev. C49, 2444 (1994) D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.A.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria Decay Modes of High-Lying Single-Particle States in 209Pb NUCLEAR REACTIONS 208Pb(α, n3He), E=122 MeV; measured E(3He), (3He)n-, γ(3He)-coin, neutron angular correlations. 209Pb deduced direct decay branching ratios, Γ(spreading)/Γ, Γn/Γ for structures at high excitation. Statistical model calculations.
doi: 10.1103/PhysRevC.49.2444
1994BL08 Nucl.Phys. A578, 267 (1994) J.Blomgren, A.M.van den Berg, J.A.Bordewijk, S.Brandenburg, D.Chmielewska, A.van der Woude, L.Nilsson, N.Olsson, Y.Blumenfeld, N.Frascaria, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, N.Alamanos, F.Auger, A.Gillibert, P.Roussel-Chomaz, R.Turcotte Neutron Decay of the Excitation-Energy Region Up to 60 MeV, Excited by Heavy-Ion Scattering. (II) 90Zr and 124Sn NUCLEAR REACTIONS 90Zr, 124Sn(17O, 17O'), E=1428 MeV; measured 17O spectra. 90Zr, 124Sn deduced giant resonances, neutron decay features. Comparison with statistical model.
doi: 10.1016/0375-9474(94)90979-2
1994BO22 Nucl.Phys. A574, 453 (1994) J.A.Bordewijk, A.Balanda, D.Beaumel, J.Blomgren, S.Brandenburg, G.van't Hof, M.N.Harakeh, M.A.Hofstee, J.Janecke, A.Krasznahorkay, H.Laurent, L.Nilsson, N.Olsson, R.Perrino, R.Siebelink, P.O.Soderman, S.Y.van der Werf, A.van der Woude Neutron Decay of the Isobaric Analog State in 208Bi NUCLEAR REACTIONS 208Pb(3He, t), E=61.2 MeV; measured neutron spectra. 208Bi deduced neutron spectrum from IAS decay, branching ratio. Statistical-decay calculations, isospin impurity. Magnetic spectrograph, neutron time-of-flight multi-detector.
doi: 10.1016/0375-9474(94)90239-9
1994KR02 Nucl.Phys. A567, 521 (1994) A.Krasznahorkay, A.Balanda, J.A.Bordewijk, S.Brandenburg, M.N.Harakeh, N.Kalantar-Nayestanaki, B.M.Nyako, J.Timar, A.van der Woude Excitation of the Isovector GDR by Inelastic α-Scattering as a Measure of the Neutron Skin of Nuclei NUCLEAR REACTIONS 116,124Sn, 150Nd, 208Pb(α, α'γ), E=120 MeV; measured σ(θ, E), αγ-coin, isovector GDR excitation. 116,124Sn, 150Nd, 208Pb deduced neutron-skin thicknesses. QMG/2 magnetic spectrograph, NaI(Tl) spectrometer with anticoincidence shield, enriched targets.
doi: 10.1016/0375-9474(94)90022-1
1994SO13 Nucl.Phys. A576, 215 (1994) P.-O.Soderman, J.Blomgren, A.Ringbom, N.Olsson, L.Nilsson, J.A.Bordewijk, S.Brandenburg, G.van't Hof, M.A.Hofstee, H.van der Ploeg, S.Y.van der Werf, A.van der Woude, A.Krasznahorkay, A.Balanda, D.Chmielewska, H.Laurent Neutron Decay of Deep-Hole States Populated by the 208Pb(3He, α)207Pb Reaction at 102 MeV NUCLEAR REACTIONS 208Pb(3He, α), E=102 MeV; measured nα(θ) following neutron decay of hole states; deduced nonstatistical decay branching. Comparison with statistical-model calculations. Tof.
doi: 10.1016/0375-9474(94)90258-5
1994VA06 Nucl.Phys. A569, 383c (1994) A.van der Woude, D.Chmielewska, A.M.van den Berg, Y.Blumenfeld, N.Alamanos, F.Auger, J.Blomgren, J.Bordewijk, S.Brandenburg, N.Frascaria, A.Gillibert, L.Nilsson, N.Olsson, P.Roussel-Chomaz, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, R.Turcotte Some Recent Results on Neutron Decay of 208Pb Excited to Energies in the 14 to 25 MeV Range NUCLEAR REACTIONS 208Pb(17O, 17O'), E=84 MeV/nucleon; measured missing energy (17O)n-coin spectra following Coulomb excitation. 124Sn(α, α'), E=120 MeV; measured σ(θα, θn) vs neutron efficiency following Coulomb exitation. 208Pb deduced GDR decay features.
doi: 10.1016/0375-9474(94)90129-5
1994VA25 Nucl.Phys. A578, 238 (1994) A.M.van den Berg, D.Chmielewska, J.A.Bordewijk, S.Brandenburg, A.van der Woude, Y.Blumenfeld, N.Frascaria, J.C.Roynette, J.A.Scarpaci, T.Suomijarvi, N.Alamanos, F.Auger, A.Gillibert, P.Roussel-Chomaz, J.Blomgren, L.Nilsson, N.Olsson, R.Turcotte Neutron Decay of the Excitation-Energy Region Up to 60 MeV, Excited by Heavy Ion Scattering. (I) 208Pb NUCLEAR REACTIONS 208Pb(17O, 17O'), E=1428 MeV; measured neutron decay spectrum, angular correlation of hole-state population versus 208Pb excitation energy. 208Pb deduced continuum neutron decay features.
doi: 10.1016/0375-9474(94)90978-4
1993LA31 Nucl.Instrum.Methods Phys.Res. A326, 517 (1993) H.Laurent, H.Lefort, D.Beaumel, Y.Blumenfeld, S.Fortier, S.Gales, J.Guillot, J.C.Roynette, P.Volkov, S.Brandenburg EDEN: A neutron time-of-flight multidetector for decay studies of giant states NUCLEAR REACTIONS 48Ca(20Ne, X), E=48 MeV/nucleon; measured n+γ spectra. 16O, 12C(α, n3He), E=120 MeV; measured neutron spectra. 16O(α, n3He), E=120 MeV; measured n(3He)(θ). 17O level deduced Γn/Γ. Neutron tof multi-detector.
doi: 10.1016/0168-9002(93)90854-B
1991GR03 Nucl.Phys. A524, 228 (1991) M.B.Greenfield, S.Brandenburg, A.G.Drentje, P.Grasdijk, H.Riezebos, S.Y.van der Werf, A.van der Woude, M.N.Harakeh, W.A.Sterrenburg, B.A.Brown The 24Mg(3He, t)24Al Reaction and L=1 Giant Resonance Systematics using an Effective 3He-n Interaction at 27 MeV/Nucleon NUCLEAR REACTIONS 24Mg(3He, t), E=81 MeV; measured σ(E(t), θ(t)). 24Al deduced levels, L, J, π. 12C, 16O, 24Mg, 28Si(3He, t), E=81 MeV; 32S(3He, t), E=73 MeV; 40Ca(3He, t), E=75 MeV; measured σ(E(t), θ(t)=0°). 12N, 16F, 24Al, 28P, 32Cl, 40Sc deduced isovector giant resonances. DWBA analysis, effective 3He-n force, shell model form factors.
doi: 10.1016/0375-9474(91)90025-2
1991KR09 Phys.Rev.Lett. 66, 1287 (1991) A.Krasznahorkay, J.Bacelar, J.A.Bordewijk, S.Brandenburg, A.Buda, G.van't Hof, M.A.Hofstee, S.Kato, T.D.Poelhekken, S.Y.van der Werf, A.van der Woude, M.N.Harakeh, N.Kalantar-Nayestanaki Excitation of the Isovector Giant Dipole Resonance by Inelastic α Scattering and the Neutron Skin of Nuclei NUCLEAR REACTIONS 116,124Sn, 208Pb(α, α'γ), E=120 MeV; measured αγ-coin, Iγ(θ), σ(θα, Eα); deduced GDR excitation σ, form factor dependence on n, p radii.
doi: 10.1103/PhysRevLett.66.1287
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
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
1989VA09 Nucl.Phys. A496, 305 (1989) S.Y.van der Werf, S.Brandenburg, P.Grasdijk, W.A.Sterrenburg, M.N.Harakeh, M.B.Greenfield, B.A.Brown, M.Fujiwara The Effective 3He-Nucleon Force in a Microscopic DWBA Approach to the (3He, t) Charge-Exchange Reaction NUCLEAR REACTIONS 12C, 16O, 24,26Mg, 28Si, 32S, 42,48Ca, 54Fe, 58Ni, 90Zr(3He, t), E=66-90 MeV; measured σ(Et, θt); deduced effective projectile-nucleon force parameters. DWBA analysis.
doi: 10.1016/0375-9474(89)90177-2
1988KR02 Nucl.Phys. A477, 55 (1988) G.J.Kramer, H.P.Blok, J.F.A.van Hienen, S.Brandenburg, M.N.Harakeh, S.Y.van der Werf, P.W.M.Glaudemans, A.A.Wolters Spectroscopic Factors from the 51V(d, 3He)50Ti Reaction NUCLEAR REACTIONS, MECPD 51V(d, 3He), E=52.9 MeV; measured σ(E(3He), θ). 50Ti deduced levels, L, spectroscopic factors.
doi: 10.1016/0375-9474(88)90360-0
1988SH38 Phys.Rev. C38, 2562 (1988) M.M.Sharma, W.T.A.Borghols, S.Brandenburg, S.Crona, A.van der Woude, M.N.Harakeh Giant Monopole Resonance in Sn and Sm Nuclei and the Compressibility of Nuclear Matter NUCLEAR REACTIONS 112,114,116,120,124Sn, 144,148,150,152Sm(α, α'), E=120 MeV; measured σ(E, θ); deduced compressibility of nuclear matter. 112,114,116,120,124Sn, 144,148,150,152Sm deduced GQR, GMR, Γ, sum rule strength. DWBA analysis.
doi: 10.1103/PhysRevC.38.2562
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
1987VA10 Phys.Rev.Lett. 58, 2383 (1987) A.van der Woude, W.T.A.Borghols, S.Brandenburg, M.M.Sharma Comment on ' Compression Modulus of Nuclear Matter and Charge-Distribution Differences ' NUCLEAR STRUCTURE 28Si, 64,66Zn, 112,116,118,120,124Sn, 142Nd, 144Sm, 197Au, 208Pb; analyzed giant monople resonance data, E0 transition EWSR; deduced nuclear matter compression modulus parameters.
doi: 10.1103/PhysRevLett.58.2383
1986LA14 Phys.Lett. 174B, 246 (1986) S.Lawitzki, D.Pade, B.Gonsior, C.D.Uhlhorn, S.Brandenburg, M.N.Harakeh, H.W.Wilschut Fission Decay of the Isoscalar Giant Quadrupole Resonance in 24Mg NUCLEAR REACTIONS 24Mg(α, α'), E=120 MeV; measured σ(θα', Eα'), σ(Eα'), (12C)(12C)(θ). 24Mg deduced isoscalar GQR fission decay to 12C fragments, EWSR.
doi: 10.1016/0370-2693(86)91092-0
1986LU02 Phys.Rev. C33, 1116 (1986) H.J.Lu, S.Brandenburg, R.De Leo, M.N.Harakeh, T.D.Poelhekken, A.van der Woude Isoscalar Monopole and Dipole Strength between 10 and 20 MeV in 24Mg from Inelastic α Scattering at and around 0° NUCLEAR REACTIONS 24Mg(α, α'), E=120 MeV; measured σ(E, θ) near θ=0°. 24Mg deduced isoscalar monopole, dipole strength.
doi: 10.1103/PhysRevC.33.1116
1986PI01 Phys.Rev. C33, 40 (1986) M.Pignanelli, S.Micheletti, R.De Leo, S.Brandenburg, M.N.Harakeh Nuclear Matter Density Effects in Monopole Transitions NUCLEAR REACTIONS 12C, 24Mg, 28Si(p, p), (p, p'), E=26-40 MeV; measured σ(θ). 12C, 24Mg(α, α), (α, α'), E=120 MeV; measured σ(θ). 24Mg(α, α'), E=40 MeV; analyzed σ(θ); deduced transition potentials. 12C, 24Mg, 28Si deduced ground state transition densities, multipole moments. Folded density-dependent interaction, coupled-channels method.
doi: 10.1103/PhysRevC.33.40
1985DE32 Nucl.Phys. A441, 591 (1985) R.De Leo, S.Brandenburg, A.G.Drentje, M.N.Harakeh, H.Janszen, A.Van Der Woude Study of the Fission Decay of the Isoscalar Monopole Resonance via the 238U(α, α') Reaction at 0° NUCLEAR REACTIONS 238U(α, α'F), E=120 MeV; measured fission σ(fragment, θ). 238U deduced fission probabilities, isoscalar giant resonance decay modes.
doi: 10.1016/0375-9474(85)90440-3
1985DE47 Phys.Lett. 162B, 1 (1985) R.De Leo, M.Pignanelli, W.T.A.Borghols, S.Brandenburg, M.N.Harakeh, H.J.Lu, S.Y.van der Werf, C.W.de Jager, J.B.van der Laan, H.de Vries Quadrupole Boson Structure Form Factors for Proton Scattering from the IBA Model and Electron Scattering NUCLEAR REACTIONS 110Pd(p, p'), E=30.7 MeV; measured σ(θ). 110Pd levels deduced B(E2). Coupled-channels, electron scattering data form factors, interacting boson model reduced matrix elements.
doi: 10.1016/0370-2693(85)91048-2
1985DE57 Phys.Lett. 165B, 30 (1985) R.De Leo, M.Pignanelli, W.T.A.Borghols, S.Brandenburg, M.N.Harakeh, H.J.Lu, S.Y.Van der Werf Low-Lying Octupole Strength in 112Cd NUCLEAR REACTIONS 112Cd(p, p'), E=30.7 MeV; measured σ(Ep'), σ(θ). 112Cd deduced levels, B(E3), fragmentation, EWSR, β3. Interacting boson model.
doi: 10.1016/0370-2693(85)90684-7
1985HO01 Nucl.Phys. A433, 181 (1985) H.J.Hofmann, S.Brandenburg, P.Grasdijk, M.N.Harakeh, W.A.Sterrenburg, S.Y.Van Der Werf Spreading Width of IAS in Even Pm Isotopes Measured via the (A)Nd(3He, t)(A)Pm and (A)Nd(3He, tp)(A-1)Nd Reactions NUCLEAR REACTIONS 142,144,146,148,150Nd(3He, t), (3He, pt), E=75 MeV; measured σ(Et), pt-coin spectra. 142,144,146,148,150Pm deduced IAS, Γ, Γp, spreading width, semi-direct proton escape probabilities.
doi: 10.1016/0375-9474(85)90176-9
1985SA24 Nucl.Phys. A441, 640 (1985) H.Sakai, R.K.Bhowmik, S.Brandenburg, J.H.Van Dijk, A.G.Drentje, M.N.Harakeh, Y.Iwasaki, R.H.Siemssen, S.Y.Van Der Werf, A.Van Der Woude γ-Decay of the Deeply-Bound Hole States in 101Pd, 105Pd, 107Pd, 111Sn, 117Sn Observed in the (3He, αγ) Reaction at 70 MeV NUCLEAR STRUCTURE 101,105,107Pd; calculated levels, δ, γ-branching. Quasiparticle-plus-rotor model. NUCLEAR REACTIONS 102,106,108Pd, 112,118Sn(3He, αγ), E=70 MeV; measured αγ-coin, Iγ(θ). 101,105,107Pd, 111,117Sn levels deduced C2S, mixing ratio. DWBA analysis. Enriched targets, magnetic spectrometer. NaI, Ge detectors.
doi: 10.1016/0375-9474(85)90442-7
1984ST10 Nucl.Phys. A420, 257 (1984) W.A.Sterrenburg, S.Brandenburg, J.H.Van Dijk, A.G.Drentje, M.B.Greenfield, M.N.Harakeh, H.Riezebos, H.Sakai, W.Segeth, S.Y.Van Der Werf, A.Van Der Woude Study of Isovector Charge-Exchange Excitations and Their Decay via the 16O(3He, tp) Reaction NUCLEAR REACTIONS 16O(3He, t), E=81 MeV; measured σ(E(t), θ(t)), σ(E(t), θ(t), E(p), θ(p)). 16F deduced levels, widths, L, J, π, decay. DWBA analysis, microscopic form factors. Ta2O5 target.
doi: 10.1016/0375-9474(84)90442-1
1984VA17 J.Phys.(Paris), Colloq.C4, 471 (1984); See 1984Va43 S.Y.van der Werf, S.Brandenburg, A.G.Drentje, P.Grasdijk, M.B.Greenfield, M.N.Harakeh, W.Segeth, W.A.Sterrenburg, A.van der Woude Isovector ΔL = 1 Strength Observed in the (3He, t) Reaction on Self Conjugate Nuclei
1984VA43 J.Phys.(Paris), Colloq.C-4, 471 (1984) S.Y.van der Werf, S.Brandenburg, A.G.Drentje, P.Grasdijk, M.B.Greenfield, M.N.Harakeh, W.Segeth, W.A.Sterrenburg, A.van der Woude Isovector ΔL = 1 Strength Observed in the (3He, t) Reaction on Self Conjugate Nuclei NUCLEAR REACTIONS 12C, 16O, 24,26Mg, 28Si, 40Ca(3He, t), E=75, 81 MeV; measured σ(Et, θt), σ(θt). 12N, 16F, 24Al, 28P, 40Sc deduced transition strengths. QMG/2 spectrograph.
1983BR21 Phys.Lett. 130B, 9 (1983) S.Brandenburg, R.De Leo, A.G.Drentje, M.N.Harakeh, H.Sakai, A.van der Woude Experimental Determination of Monopole Strength in 40Ca between 10 and 20 MeV Excitation Energy NUCLEAR REACTIONS 40Ca(α, α'), (α, 2α), E=120 MeV; measured σ(θα'), σ(Eα', θ=0°), αα-coin, σ(θα1, θα2); deduced σ(total). 40Ca deduced E0 transition strength distribution, EWSR.
doi: 10.1016/0370-2693(83)91052-3
1982BL21 Phys.Rev. C26, 1893 (1982) N.Blasi, S.Brandenburg, M.N.Harakeh, W.A.Sterrenburg, S.Y.van der Werf 197Au(3He, d)198Hg Reaction at E(3He) = 50 MeV NUCLEAR REACTIONS 197Au(3He, d), E=50 MeV; measured σ(θ). 198Hg deduced levels, J, π, configuration, C2S, supersymmetry model breakdown, Alaga model validity. DWBA analysis.
doi: 10.1103/PhysRevC.26.1893
1982BR26 Phys.Rev.Lett. 49, 1687 (1982) S.Brandenburg, R.De Leo, A.G.Drentje, M.N.Harakeh, H.Janszen, A.van der Woude Fission Decay of the Isoscalar Giant Monopole Resonance in 238U NUCLEAR REACTIONS 238U(α, α'F), E=120 MeV; measured fission (fragment)α'-coin, σ(Eα, fragment θ). 238U deduced giant monopole fission decay, Γ, E0 isoscalar EWSR. QMG/2 spectrograph, parallel plate avalanche detectors.
doi: 10.1103/PhysRevLett.49.1687
1981VA18 Phys.Lett. 105B, 111 (1981) S.Y.van der Werf, N.Blasi, S.Brandenburg, A.G.Drentje, M.N.Harakeh, W.A.Sterrenburg, B.Visscher, A.van der Woude, R.De Leo, H.Janszen Fission Probability of the IAR in the Actinide Region Studied Via the (3He, tf) Reaction NUCLEAR REACTIONS, Fission 232Th, 238U(3He, t), (3He, tF), E=81 MeV; measured σ(θt, Et), (fragment)t-coin. 232Pa, 238Np deduced IAR widths, total fission probabilities, spreading widths. Hydrodynamic, microscopic models.
doi: 10.1016/0370-2693(81)91001-7
1980AN02 Nucl.Phys. A334, 205 (1980) A.Anttila, S.Brandenburg, J.Keinonen, M.Bister Lifetimes of Low-Lying States in 19F NUCLEAR REACTIONS 15N(α, γ), E=1.68, 1.79, 1.84 MeV; measured Eγ, DSA. 19F levels deduced T1/2. Ge(Li) detector. Enriched, implanted targets.
doi: 10.1016/0375-9474(80)90064-0
1980KE03 Nucl.Phys. A341, 345 (1980) Hydrogen Burning of 24,25,26Mg in Explosive Carbon Burning NUCLEAR REACTIONS 24Mg(p, γ), E=0.82 MeV; 25Mg(p, γ), E=0.3-1.7 MeV; 26Mg(p, γ), E=0.3-2.1 MeV; measured σ(Ep), Ep, Iγ(θ). 25,26,27Al levels deduced γ-ray branching ratios, resonance strengths, Γ, astrophysical reaction rates. Ge(Li) detector. Natural, enriched targets.
doi: 10.1016/0375-9474(80)90317-6
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