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Search: Author = J.M.Schippers

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2002RA15      Nucl.Instrum.Methods Phys.Res. A481, 253 (2002)

S.Rakers, F.Ellinghaus, R.Bassini, C.Baumer, A.M.van den Berg, D.Frekers, D.De Frenne, M.Hagemann, V.M.Hannen, M.N.Harakeh, M.Hartig, R.Henderson, J.Heyse, M.A.de Huu, E.Jacobs, M.Mielke, J.M.Schippers, R.Schmidt, S.Y.van der Werf, H.J.Wortche

Measuring the (d, 2He) Reaction with the Focal-Plane Detection System of the BBS Magnetic Spectrometer at AGOR

NUCLEAR REACTIONS 12C, 24Mg(d, 2p), E=170 MeV; measured proton spectra, correlations. 12B, 24Na deduced levels, J, π.

doi: 10.1016/S0168-9002(01)01365-1
Citations: PlumX Metrics


1995HO10      Nucl.Phys. A588, 729 (1995)

M.A.Hofstee, S.Y.van der Werf, A.M.van den Berg, N.Blasi, J.A.Bordewijk, W.T.A.Borghols, R.De Leo, G.T.Emery, S.Fortier, S.Gales, M.N.Harakeh, P.den Heijer, C.W.de Jager, H.Langevin-Joliot, S.Micheletti, M.Morlet, M.Pignanelli, J.M.Schippers, H.de Vries, A.Willis, A.van der Woude

Localized 1(h-bar x Omega) Particle-Hole Strength in Nuclei

NUCLEAR REACTIONS 90Zr, 116Sn, 196Pt, 208Pb(p, p'), E=201 MeV; 116Sn(polarized p, p'), E=133.8 MeV; 90Zr, 116Sn, 196Pt(α, α'), E=120 MeV; measured σ(θ). 116Sn, 196Pt(e, e'), E=278, 333 MeV; measured form factors. 90Zr, 116Sn, 196Pt, 208Pb deduced 0, 1(h-bar x omega) strength distribution. DWBA calculation, effective NN-force.

doi: 10.1016/0375-9474(95)00057-8
Citations: PlumX Metrics


1992AN15      Nucl.Phys. A550, 235 (1992)

E.Andersen, H.Helstrup, G.Lovhoiden, T.F.Thorsteinsen, M.Guttormsen, S.Messelt, T.S.Tveter, M.A.Hofstee, J.M.Schippers, S.Y.van der Werf

Helium-Induced One-Neutron Transfer to Levels in 162Dy

NUCLEAR REACTIONS 161Dy(α, 3He), 163Dy(3He, α), E=50 MeV; measured E(3He), Eα, σ(θ). 162Dy deduced levels, J, π. Nilsson model.

doi: 10.1016/0375-9474(92)90681-9
Citations: PlumX Metrics


1992PI08      Nucl.Phys. A540, 27 (1992)

M.Pignanelli, N.Blasi, S.Micheletti, R.De Leo, L.LaGamba, R.Perrino, J.A.Bordewijk, M.A.Hofstee, J.M.Schippers, S.Y.van der Werf, J.Wesseling, M.N.Harakeh

Hexadecapole Strength Distributions of Vibrational Nuclei in the A = 100 Mass Region

NUCLEAR REACTIONS 94,98,100Mo, 104,106,110Pd, 110,112Cd(p, p'), E=30.7 MeV; 94,98,100Mo, 104,106,110Pd, 110,112Cd(d, d'), E=50.7 MeV; 100Mo, 110Pd(p, p'), E=51 MeV; 112Cd(p, p'), E=60 MeV; measured σ(Ep', θ), σ(Ed', θ). 94,98,100Mo, 104,106,110Pd, 110,112Cd deduced levels, J, π, B(λ). Enriched targets.

doi: 10.1016/0375-9474(92)90192-M
Citations: PlumX Metrics


1992SC20      Nucl.Phys. A548, 271 (1992)

J.M.Schippers, W.T.A.Borghols, M.A.Hofstee, R.F.Noorman, J.M.Schreuder, S.Y.van der Werf, N.Blasi

A High Resolution Study of Stretched-Spin States in 116Sn with the 115In(3He, d)116Sn and 115In(α, tγ)116Sn Reactions

NUCLEAR REACTIONS 115In(3He, d), E=50 MeV; 115In(α, t), E=65 MeV; measured σ(θ). 115In(α, tγ), E=65 MeV; measured tγ-coin. 116Sn deduced levels, J, π, spectroscopic factors, stretched-spin states. Comparison with model calculations.

doi: 10.1016/0375-9474(92)90012-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1644.


1991JA04      Nucl.Phys. A526, 1 (1991)

J.Janecke, F.D.Becchetti, A.M.van den Berg, G.P.A.Berg, G.Brouwer, M.B.Greenfield, M.N.Harakeh, M.A.Hofstee, A.Nadasen, D.A.Roberts, R.Sawafta, J.M.Schippers, E.J.Stephenson, D.P.Stewart, S.Y.van der Werf

Non-Spin-Flip (3He, t) Charge-Exchange and Isobaric Analog States of Actinide Nuclei Studied at θ = 0°, E(3He) = 76 MeV and 200 MeV

NUCLEAR REACTIONS 12C, 16O, 27Al, 28Si, Ta, 230,232Th, 234,236,238U(3He, t), E=76.5 MeV; 12,13C, 16O, 19F, 28,29Si, 90Zr, 117,120Sn, Ta, W, 197Au, 208Pb, 230,232Th, 234,238U, 244Pu(3He, t), E=200 MeV; measured σ(Et); 120Sn(3He, t), E=200 MeV; measured σ(θt) for IAS; 230,232Th, 234,236,238U(3He, tp), E=76.5 MeV; measured proton decay from IAS, σ(Et, Ep, θt, θp); deduced Q-values for transitions to IAS. 90Nb, 117Sb, 120Sn, 181W, 184Re, 197Hg, 208Pb, 230,232Pa, 234,236,238Np, 244Am deduced Coulomb displacement energies, total widths Γ, escape widths, spreading widths of IAS. Non-spin-flip charge exchange effective interaction. Enriched and long-lived radioactive targets, magnetic spectrometers.

doi: 10.1016/0375-9474(91)90295-H
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0385.


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


1990PI14      Nucl.Phys. A519, 567 (1990)

M.Pignanelli, N.Blasi, S.Micheletti, R.De Leo, M.A.Hofstee, J.M.Schippers, S.Y.van der Werf, M.N.Harakeh

Octupole Excitations in Vibrational Nuclei and the sdf Interacting Boson Model

NUCLEAR REACTIONS 98,100Mo, 104,106,110Pd, 110,112Cd, 146,150Nd, 150Sm(p, p'), E=30.7 MeV; 98,100Mo, 104,106,110Pd, 110,112Cd, 146,150Nd, 150Sm(d, d'), E=50.7 MeV; 100Mo, 110Pd(p, p'), E=51 MeV; 112Cd, 150Sm(p, p'), E=60 MeV; measured σ(Ep, θ), σ(Ed, θ). 98,100Mo, 104,106,110Pd, 146,150Nd, 150Sm deduced levels, J, π, B(λ). Enriched targets.

doi: 10.1016/0375-9474(90)90447-T
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0679.


1990SC12      Nucl.Phys. A510, 70 (1990)

J.M.Schippers, J.M.Schreuder, S.Y.van der Werf, K.Allaart, N.Blasi, M.Waroquier

Study of 116Sn via Neutron Pickup and Proton Stripping Reactions

NUCLEAR REACTIONS 117Sn(d, t), E=50 MeV; 117Sn(3He, α), E=50 MeV; 115In(3He, d), E=50 MeV; 115In(α, t), E=65 MeV; measured σ(θ). 116Sn deduced levels, J, π, spectroscopic factors. Comparison with model calculations.

doi: 10.1016/0375-9474(90)90288-W
Citations: PlumX Metrics


1990WO11      Nucl.Phys. A518, 496 (1990)

P.Woldt, P.Grabmayr, G.Rau, G.J.Wagner, M.A.Hofstee, J.M.Schippers, S.Y.Van der Werf, H.Nann

Testing a Sum-Rule Approach to Occupation Numbers by the 205Tl(3He, d)206Pb Reaction

NUCLEAR REACTIONS 205Tl(3He, d), E=50.9 MeV; measured σ(θ). 206Pb levels, deduced J, π, spectroscopic factors. Sum rule analysis.

doi: 10.1016/0375-9474(90)90142-9
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


1989DE17      Phys.Lett. 226B, 5 (1989)

R.De Leo, L.Lagamba, N.Blasi, S.Micheletti, M.Pignanelli, M.Fujiwara, K.Hosono, I.Katayama, N.Matsuoka, S.Morinobu, T.Noro, S.Matsuki, H.Okamura, J.M.Schippers, S.Y.van der Werf, M.N.Harakeh

Quadrupole Mixed-Symmetry States in 106Pd

NUCLEAR REACTIONS 106Pd(polarized p, p'), E=34.93 MeV; 106Pd(d, d'), E=51 MeV; measured σ(θ). 106Pd levels deduced deformation parameter, form factor, quadrupole transition matrix elements.

doi: 10.1016/0370-2693(89)90278-5
Citations: PlumX Metrics


1989DE19      Phys.Lett. 226B, 202 (1989)

R.De Leo, N.Blasi, S.Micheletti, M.Pignanelli, M.N.Harakeh, W.T.A.Borghols, J.M.Schippers, S.Y.van der Werf

Quadrupole Core Polarization Charges in the A = 100 and 150 Mass Regions

NUCLEAR STRUCTURE 94,96,98,100Mo, 102Ru, 104,106,108,110Pd, 106,108,110,112,114,116Cd, 142,144,146,148,150Nd, 144,148,150,152,154Sm, 154,156,158,160Gd, 162,164Dy; analyzed inelastic data; deduced nucleon quadrupole core polarization charges.

doi: 10.1016/0370-2693(89)91180-5
Citations: PlumX Metrics


1989DE40      Nucl.Phys. A504, 109 (1989)

R.De Leo, N.Blasi, S.Micheletti, M.Pignanelli, W.T.A.Borghols, J.M.Schippers, S.Y.van der Werf, G.Maino, M.N.Harakeh

Multipole Strength Distribution in 112Cd

NUCLEAR REACTIONS 112Cd(p, p'), E=30.7, 50 MeV; measured σ(E(p')), σ(θ). 112Cd deduced levels, J, π, B(λ). Enriched target.

doi: 10.1016/0375-9474(89)90285-6
Citations: PlumX Metrics


1989LA21      Z.Phys. A334, 133 (1989)

H.Langevin-Joliot, E.Gerlic, J.Guillot, J.Van de Wiele, S.Y.van der Werf, T.H.Martens, J.M.Schippers

Valence and Inner Proton Hole States in 119In via the (d, 3He) Reaction

NUCLEAR REACTIONS 120Sn(d, 3He), E=108.4 MeV; measured σ(θ). 119In deduced levels, L, spectroscopic strengths.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1642.


1988PI04      Phys.Lett. 202B, 470 (1988)

M.Pignanelli, S.Micheletti, N.Blasi, R.De Leo, W.T.A.Borghols, J.M.Schippers, S.Y.van der Werf, M.N.Harakeh

Neutron Transition Moments and Quadrupole T- or F-Vector States

NUCLEAR REACTIONS 104,110Pd, 112Cd, 146,150Nd, 150Sm(p, p'), E=30.3 MeV; 104,110Pd, 112Cd, 146,150Nd, 150Sm(d, d'), E=50.4 MeV; measured σ(θ). 110,104Pd, 112Cd level deduced proton, neutron, isovector transition density E2 moments.

doi: 10.1016/0370-2693(88)91845-X
Citations: PlumX Metrics


1988RO07      Phys.Lett. 207B, 125 (1988)

J.Rogowski, N.Kaffrell, D.De Frenne, K.Heyde, E.Jacobs, M.N.Harakeh, J.M.Schippers, S.Y.van der Werf

Evidence for Shape Coexistence in Odd-Mass Rhodium Nuclei

NUCLEAR REACTIONS 104Ru(3He, d), E=50 MeV; measured σ(Ed), σ(θ). 105Rh deduced levels, J, π, band structure, spectroscopic factors.

doi: 10.1016/0370-2693(88)91402-5
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1640.


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


1987VA30      Phys.Rev. C36, 1796 (1987)

S.Y.van der Werf, J.M.Schippers, N.Blasi, G.T.Emery, M.N.Harakeh, C.W.de Jager, M.Waroquier

Core Polarization and Quenching in Stretched Spin States: Case study of the 9- E(x) = 3.522 MeV State in 116Sn

NUCLEAR REACTIONS, MECPD 116Sn(polarized p, p), E=133.8 MeV; measured σ(θ), analyzing power vs θ. 116Sn(e, e'), E not given; measured form factors. 115In(α, t), E=65 MeV; measured σ(θ). 116Sn level deduced quenching characteristics.

doi: 10.1103/PhysRevC.36.1796
Citations: PlumX Metrics


1986SC22      Nucl.Instrum.Methods Phys.Res. A247, 467 (1986)

J.M.Schippers, W.T.A.Borghols, S.Y.van der Werf

The Vertical Drift Chamber as a Two Dimensional Focal Plane Detector for Light and Heavy Ions in the QMG/2 Spectrometer

NUCLEAR REACTIONS 197Au(α, α'), E=120 MeV; 110Pd(p, d), 115In(α, t), E=65 MeV; measured Eα, Iα, Ed, Id, Et, It; deduced multi-wire drift chamber resolution.

doi: 10.1016/0168-9002(86)90409-2
Citations: PlumX Metrics


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