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NSR database version of April 25, 2024.

Search: Author = E.H.Aarts

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1985AA01      Nucl.Phys. A439, 45 (1985)

E.H.L.Aarts, R.A.R.L.Malfliet, R.J.De Meijer, S.Y.Van Der Werf, G.Baur, R.Shyam, F.Rosel, D.Trautmann

Comparison between a Distorted-Wave Breakup Model Description and a Quasi-Free Breakup Model Description of ³He Projectile Breakup Data at 52 MeV

NUCLEAR REACTIONS ²⁸Si, ⁵⁸Ni(³He, dX), (³He, dp), E=52 MeV; calculated inclusive σ(θd, Ed), σ(θp, θd, Ed). Quasifree breakup, DWBA.

doi: 10.1016/0375-9474(85)90208-8
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1984AA01      Nucl.Phys. A425, 23 (1984)

E.H.L.Aarts, R.A.R.L.Malfliet, R.J.De Meijer, S.Y.Van Der Werf

Reaction Mechanisms in ³He Projectile Breakup at 52 MeV on ¹²C, ²⁸Si and ⁵⁸Ni

NUCLEAR REACTIONS, ICPND ¹²C, ²⁸Si, ⁵⁸Ni(³He, p), (³He, d), (³He, 2p), (³He, pd), E=52 MeV; measured inclusive σ(θp), σ(θd), σ(Ep), σ(Ed), σ(θp, θd, Ed), σ(θp, θd), σ(θ₁, θ₂, Ep₁), σ(θ₁, θ₂); deduced reaction mechanism, σ vs target mass. Quasifree breakup calculations.

doi: 10.1016/0375-9474(84)90217-3
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1983DE22      Nucl.Phys. A402, 15 (1983)

R.J.De Meijer, E.H.L.Aarts, M.B.Greenfield, W.A.Sterrenburg

Mechanisms for Reactions of α-Particles on ²⁸Si at Eα = 65 MeV leading to Three-Body Final States

NUCLEAR REACTIONS ²⁸Si(α, p), (α, d), (α, t), (α, ³He), (α, α), (α, ⁶Li), (α, ⁷Li), (α, ⁹Be), (α, 2p), (α, pd), (α, pt), (α, 2d), (α, αd), (α, αt), Eα=65 MeV; measured σ(θ, E), σ(θ₁, θ₂, E). Comparison with ³He breakup at 52 MeV. Kinematically complete measurement.

doi: 10.1016/0375-9474(83)90559-6
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1983JA03      Nucl.Phys. A394, 39 (1983)

J.Janecke, E.H.L.Aarts, A.G.Drentje, M.N.Harakeh, C.Gaarde

Isobaric Analog States in Rare-Earth Nuclei Studied with the (³He, t) Charge Exchange Reaction at θ(L) = 0°

NUCLEAR REACTIONS ^{152,154,156,158,160}Gd, ^160,162Dy, ^{162,164,166,168,170}Er, ^{170,172,174,176}Yb, ^176,178,180Hf(³He, t), E=60.5 MeV; measured σ(E(t), θ=0°). ^{152,154,156,158,160}Tb, ^160,162Ho, ^{162,164,166,168,170}Tm, ^{170,172,174,176}Lu, ^176,178,180Ta deduced IAS, Γ, Coulomb displacement energies. Enriched targets, magnetic spectrometer.

doi: 10.1016/0375-9474(83)90160-4
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1982AA03      Nucl.Phys. A380, 465 (1982)

E.H.L.Aarts, R.Malfliet, S.Y.Van Der Werf, R.J.De Meijer

The Quasi-Free Breakup of ³He

NUCLEAR REACTIONS ²⁸Si(³He, pd), (³He, pt), E=52 MeV; calculated σ(θ₁, θ₂), σ(θ₁, θ₂, E₂). DWBA formalism, quasifree breakup.

doi: 10.1016/0375-9474(82)90571-1
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1981AA01      Phys.Lett. 102B, 307 (1981)

E.H.L.Aarts, R.K.Bhowmik, R.J.de Meijer, S.Y.van der Werf

The Continuum Part of (³He, t) Spectra at E(³He) = 52 MeV

NUCLEAR REACTIONS ¹²C, ²⁶Mg, ²⁷Al, Si, ²⁰⁸Pb(³He, t), (³He, 2d), (³He, pt), (³He, p³He), E=52 MeV; measured σ(Et), σ(Et, θt), pt-coin, σ(E₁, θ₁, θ₂); deduced reaction mechanisms. Plane wave impulse approximation.

doi: 10.1016/0370-2693(81)90623-7
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1981AA02      Phys.Lett. 105B, 130 (1981)

E.H.L.Aarts, P.Grasdijk, R.J.de Meijer, S.Y.van der Werf

Contributions of Elastic, Inelastic and Absorptive Breakup to the Inclusive Deuteron Spectrum of the Reaction ²⁸Si(³He, d) at E(³He) = 52 MeV

NUCLEAR REACTIONS ²⁸Si(³He, pd), E=52 MeV; measured σ(θp, θd) vs total kinetic energy, pd-coin, σ(θp, Ep, θd), σ(θp, θd, Ed); deduced reaction mechanism.

doi: 10.1016/0370-2693(81)91005-4
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1981IW01      Phys.Rev. C23, 1477 (1981)

Y.Iwasaki, E.H.L.Aarts, M.N.Harakeh, R.H.Siemssen, S.Y.van der Werf

¹⁹⁴Pt(d, ³He)¹⁹³Ir Reaction: Spectroscopic factors and supersymmetry predictions

NUCLEAR REACTIONS ¹⁹⁴Pt(d, ³He), E=50 MeV; measured σ(θ). ¹⁹³Ir levels deduced L, S, supersymmetry model validation. DWBA analysis.

doi: 10.1103/PhysRevC.23.1477
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1980AA01      Nucl.Instrum.Methods 176, 605 (1980)

E.H.L.Aarts, A.M. van den Berg, R.J.de Meijer

On the Detection of ²He with the QMG/2 Spectrograph

NUCLEAR REACTIONS ²⁸Si, ¹²C(³He, 2p), E=52 MeV; measured σ(E₁, E₂, θ); deduced evidence for unbound diproton. QMG/2 spectrograph. Watson-Migdal calculation.

doi: 10.1016/0029-554X(80)90395-X
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