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NSR database version of March 18, 2024.

Search: Author = S.Brandenburg

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0256.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1980KE03      Nucl.Phys. A341, 345 (1980)

J.Keinonen, S.Brandenburg

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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD5035.


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