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NSR database version of April 26, 2024.

Search: Author = W.T.Borghols

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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
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1992PO09      Nucl.Phys. A549, 180 (1992)

V.Yu.Ponomarev, W.T.A.Borghols, S.A.Fayans, M.N.Harakeh, C.W.de Jager, J.B.van der Laan, A.P.Platonov, H.de Vries, S.Y.van der Werf

Transition Charge Densities of Low-Lying Collective States in ¹⁹⁶Pt from Inelastic Electron Scattering

NUCLEAR REACTIONS ¹⁹⁶Pt(e, e'), E=90-334 MeV; measured spectra, longitudinal form factors. ¹⁹⁶Pt levels deduced transition charge densities, J, π, B(λ). Fourier-Bessel analysis. Compared to microscopic quasiparticle phonon model.

doi: 10.1016/0375-9474(92)90039-M
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1644.

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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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, ^{104,106,108,110}Pd, ^{106,108,110,112,114,116}Cd, ^{142,144,146,148,150}Nd, ^{144,148,150,152,154}Sm, ^{154,156,158,160}Gd, ^162,164Dy; analyzed inelastic data; deduced nucleon quadrupole core polarization charges.

doi: 10.1016/0370-2693(89)91180-5
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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
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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
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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 ^{112,114,116,120,124}Sn, ^{144,148,150,152}Sm(α, α'), E=120 MeV; measured σ(E, θ); deduced compressibility of nuclear matter. ^{112,114,116,120,124}Sn, ^{144,148,150,152}Sm 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, ^{112,116,118,120,124}Sn, 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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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
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1985BO14      Phys.Lett. 152B, 330 (1985)

W.T.A.Borghols, N.Blasi, R.Bijker, M.N.Harakeh, C.W.De Jager, J.B.van der Laan, H.de Vries, S.Y.van der Werf

Excitation of Hexadecapole Transitions in ¹⁹⁶Pt via Electron Scattering and Their Interpretation in the Interacting Boson Approximation

NUCLEAR REACTIONS ¹⁹⁶Pt(e, e'), E not given; measured form factors. ¹⁹⁶Pt levels deduced transition densities, neutron, proton structure functions. Interacting boson approximations.

doi: 10.1016/0370-2693(85)90505-2
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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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