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Search: Author = K.Allaart

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1998GI05      Phys.Rev. C57, 1691 (1998)

C.Giusti, F.D.Pacati, K.Allaart, W.J.W.Geurts, W.H.Dickhoff, H.Muther

Selectivity of the 16O(e, e'pp) Reaction to Discrete Final States

NUCLEAR REACTIONS 16O(e, e'2p), E=475, 584, 855 MeV; calculated σ(E, θ); deduced final state selectivity.

doi: 10.1103/PhysRevC.57.1691
Citations: PlumX Metrics


1998ON02      Phys.Rev.Lett. 81, 2213 (1998)

C.J.G.Onderwater, K.Allaart, E.C.Aschenauer, Th.S.Bauer, D.J.Boersma, E.Cisbani, W.H.Dickhoff, S.Frullani, F.Garibaldi, W.J.W.Geurts, C.Giusti, D.L.Groep, W.H.A.Hesselink, M.Iodice, E.Jans, N.Kalantar-Nayestanaki, W.-J.Kasdorp, C.Kormanyos, L.Lapikas, J.J.van Leeuwe, R.De Leo, A.Misiejuk, H.Muther, F.D.Pacati, A.R.Pellegrino, R.Perrino, R.Starink, M.Steenbakkers, G.van der Steenhoven, J.J.M.Steijger, M.A.van Uden, G.M.Urciuoli, L.B.Weinstein, H.W.Willering

Signatures for Short-Range Correlations in 16O Observed in the Reaction 16O(e, e'pp)14C

NUCLEAR REACTIONS 16O(e, e'2p), E=584 MeV; measured σ(Ee, θ(e), Ep, θ(p)), missing momentum; deduced short-range correlations role.

doi: 10.1103/PhysRevLett.81.2213
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1997ON03      Phys.Rev.Lett. 78, 4893 (1997)

C.J.G.Onderwater, K.Allaart, E.C.Aschenauer, Th.S.Bauer, D.J.Boersma, E.Cisbani, S.Frullani, F.Garibaldi, W.J.W.Geurts, D.L.Groep, W.H.A.Hesselink, M.Iodice, E.Jans, N.Kalantar-Nayestanaki, W.-J.Kasdorp, C.Kormanyos, L.Lapikas, J.J.van Leeuwe, R.De Leo, A.Misiejuk, A.R.Pellegrino, R.Perrino, R.Starink, M.Steenbakkers, G.van der Steenhoven, J.J.M.Steijger, M.A.van Uden, G.M.Urciuoli, L.B.Weinstein, H.W.Willering

Dominance of 1S0 Proton-Pair Emission in the 16O(e, e'pp) Reaction

NUCLEAR REACTIONS 16O(e, e'2p), E=584 MeV; measured missing momenta spectra, excitation energy spectra; deduced direct proton-pair knockout evidence.

doi: 10.1103/PhysRevLett.78.4893
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1996GE01      Phys.Rev. C53, 2207 (1996)

W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther

Spectroscopic Factors for Nucleon Knock-Out from 16O at Small Missing Energy

NUCLEAR STRUCTURE 16O; calculated one-nucleon knock-out spectroscopic factors. Green's function formalism.

doi: 10.1103/PhysRevC.53.2207
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1996GE03      Phys.Rev. C54, 1144 (1996)

W.J.W.Geurts, K.Allaart, W.H.Dickhoff, H.Muther

Two-Nucleon Spectral Function of 16O at High Momenta

NUCLEAR STRUCTURE 16O; calculated two-nucleon spectral functions.

NUCLEAR REACTIONS 16O(e, e'X), E=700 MeV; calculated longitudinal differential σ for 2p knockout. Plane wave approximation.

doi: 10.1103/PhysRevC.54.1144
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1996RI01      Phys.Rev. C53, 201 (1996)

G.A.Rijsdijk, W.J.W.Geurts, K.Allaart, W.H.Dickhoff

Hole Spectral Function and Two-Particle-One-Hole Response Propagator

NUCLEAR STRUCTURE 48Ca, 90Zr; calculated hole-state spectral functions. 47K, 89Y; calculated quasihole states spectroscopic factors.

doi: 10.1103/PhysRevC.53.201
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1994GE04      Phys.Rev. C50, 514 (1994)

W.J.W.Geurts, K.Allaart, W.H.Dickhoff

Gamow-Teller (p, n) and (n, p) Strength in a Dressed Extended Random Phase Approximation

NUCLEAR STRUCTURE 48Ca; calculated (p, n) Gamow-Teller transition strength. Dressed, extended RPA.

doi: 10.1103/PhysRevC.50.514
Citations: PlumX Metrics


1994RI07      Nucl.Phys. A573, 173 (1994)

D.E.J.Riedeman, K.Allaart, H.P.Blok, M.N.Harakeh, K.Heyde, C.W.de Jager, H.de Vries

Electron Scattering Off 65Cu and 71Ga

NUCLEAR REACTIONS 65Cu(e, e'), E=82.3-443 MeV; 71Ga(e, e'), E=132.4-357.7 MeV; measured spectra. 65Cu, 71Ga levels deduced longitudinal, transverse form factors, transition charge, current densities, B(λ). Weak-coupling, particle-vibration coupling, quasiparticle-vibration coupling models, Fourier-Bessel, gaussian polynomial analysis.

doi: 10.1016/0375-9474(94)90167-8
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1993RI08      Phys.Rev. C48, 1752 (1993)

G.A.Rijsdijk, W.J.W.Geurts, M.G.E.Brand, K.Allaart, W.H.Dickhoff

Spin-Isospin Strength and Spectral Functions

NUCLEAR REACTIONS 90Zr, 48Ca(p, n), (n, p), E not given; calculated Gamow-Teller, spin-dipole response functions. Dressed independent particle, RPA approaches.

doi: 10.1103/PhysRevC.48.1752
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1992RI08      Nucl.Phys. A550, 159 (1992)

G.A.Rijsdijk, K.Allaart, W.H.Dickhoff

Hole Spectral Functions and Collective Excitations

NUCLEAR STRUCTURE 48Ca, 90Zr; calculated spectral strength distributions, occupation probabilities. Large configuration space, realistic G-matrix interaction.

doi: 10.1016/0375-9474(92)91137-E
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1991BR22      Nucl.Phys. A531, 253 (1991)

M.G.E.Brand, G.A.Rijsdijk, F.A.Muller, K.Allaart, W.H.Dickhoff

Fragmentation of Single-Particle Strength and the Validity of the Shell Model

NUCLEAR REACTIONS 90Zr, 48Ca(e, e'p), E not given; calculated spectral functions, several l-values; deduced shell model validity features. Green function Dyson equation.

doi: 10.1016/0375-9474(91)90612-A
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1991RA01      Phys.Rev. C43, 521 (1991)

S.Raman, T.A.Walkiewicz, S.Kahane, E.T.Jurney, J.Sa, Z.Gacsi, J.L.Weil, K.Allaart, G.Bonsignori, J.F.Shriner, Jr.

Nearly Complete Level Scheme of 116Sn Below 4.3 MeV

NUCLEAR REACTIONS 115Sn(n, γ), E=thermal; 116Sn(n, n'γ), E ≤ 4.5 MeV; measured Eγ, Iγ, γ(θ) vs E. 116Sn deduced levels, J, π, neutron separation energy.

doi: 10.1103/PhysRevC.43.521
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14169.


1990BR03      Nucl.Phys. A509, 1 (1990)

M.G.E.Brand, K.Allaart, W.H.Dickhoff

Nuclear Response Beyond Mean Field Theory

NUCLEAR STRUCTURE 48Ca; calculated levels, transition densities, currents, B(λ), electric quadrupole, dipole resonance strength functions. 48Sc; calculated levels, Gamow-Teller resonance strength functions. Extended RPA.

NUCLEAR REACTIONS 48Ca(e, e'), E not given; calculated form factor. Extended RPA.

doi: 10.1016/0375-9474(90)90374-U
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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


1988BR33      Phys.Lett. 214B, 483 (1988)

M.G.E.Brand, K.Allaart, W.H.Dickhoff

Conserving RPA and the Response of 48Ca

NUCLEAR STRUCTURE 48Ca; calculated electric quadrupole, dipole resonance strength functions. 48Sc; calculated Gamow-Teller resonance strength functions.

doi: 10.1016/0370-2693(88)90104-9
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1988RA09      Phys.Rev. C37, 1203 (1988)

S.Raman, T.A.Walkiewicz, L.G.Multhauf, K.G.Tirsell, G.Bonsignori, K.Allaart

Decays of 118In, 120In, and 122In Isomers to Levels in 118Sn, 120Sn, and 122Sn

RADIOACTIVITY 118,120,122In(β-) [from 118,120,122Sn(n, p), E=14 MeV]; measured Eγ, Iγ. 118,120,122Sn deduced levels, γ transitions. Broken pair model.

NUCLEAR STRUCTURE 118,120,122Sn; calculated levels. Broken pair model.

doi: 10.1103/PhysRevC.37.1203
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1986AL20      Nucl.Phys. A458, 412 (1986)

K.Allaart, G.Bonsignori, M.Savoia, V.Paar

Construction of Microscopic Boson States and Their Relevance for IBM-2

NUCLEAR STRUCTURE N=50-82; calculated levels, quadrupole matrix element ratios, d-boson number. Four types of collective fermion states.

doi: 10.1016/0375-9474(86)90043-6
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1986DE26      Phys.Lett. 179B, 322 (1986)

L.C.De Winter, N.R.Walet, P.J.Brussaard, K.Allaart, A.E.L.Dieperink

Collective Pair Structure of K = 0 and K = 1 Bands in Deformed Nuclei

NUCLEAR STRUCTURE 156Gd; calculated level structure; deduced collective pair structure. Fermion pair description.

doi: 10.1016/0370-2693(86)90485-5
Citations: PlumX Metrics


1986HE07      Nucl.Phys. A451, 269 (1986)

W.Hengeveld, W.H.Dickhoff, K.Allaart

Self-Consistent Medium Polarization in RPA

NUCLEAR REACTIONS 56Ni(e, e'), E not given; calculated form factors. RPA, self-consistent medium polarization.

NUCLEAR STRUCTURE 56Ni; calculated levels, B(M1), transition density. 56Co; calculated levels. RPA, self-consistent medium polarization.

doi: 10.1016/0375-9474(86)90415-X
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1986VA03      Nucl.Phys. A449, 579 (1986)

J.J.Van Ruyven, J.Penninga, W.H.A.Hesselink, P.Van Nes, K.Allaart, E.J.Hengveld, H.Verheul, M.J.A.De Voigt, Z.Sujkowski, J.Blomqvist

High-Spin Neutron Excitations in Neutron-Deficient Even-Mass Pb Isotopes

NUCLEAR REACTIONS, ICPND 188Os(12C, 3n), (12C, 4n), (12C, 5n), (12C, 6n), (12C, 7n), E=70-110 MeV; measured σ(E), Eγ, Iγ(t), γγ(t), sum spectra, I(ce), σ(Eγ, θ); 198Hg(α, 6n), E=75 MeV; measured Eγ, Iγ(t), γγ(t), sum spectra, I(ce), σ(Eγ, θ). 194,196Pb deduced levels, J, π, γ-branching, T1/2, B(λ). Enriched targets, Ge(Li), Ge, Si(Li) detectors, sum spectrometer, mini-orange filter.

NUCLEAR STRUCTURE 194,196Pb; calculated levels, B(λ). 190,192,194,196,198,200,202,204,206Pb; calculated levels, energy differences. One-, two-broken-pair models.

doi: 10.1016/0375-9474(86)90235-6
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1985BO01      Nucl.Phys. A432, 389 (1985)

G.Bonsignori, M.Savoia, K.Allaart, A.Van Egmond, G.Te Velde

Spectroscopy of Even Sn Nuclei and Generalized-Seniority Breaking

NUCLEAR STRUCTURE 110,112,114,116,118,120,122,124Sn; calculated single particle energies, occupation probabilities, ground state wave functions, B(E2) ratios, B(λ). Generalized seniority breaking model.

doi: 10.1016/0375-9474(85)90250-7
Citations: PlumX Metrics


1985HE04      Nucl.Phys. A435, 381 (1985)

W.Hengeveld, K.Allaart, W.H.Dickhoff

Application of Realistic Meson-Exchange Forces in the Broken-Pair Model

NUCLEAR REACTIONS 88Sr(e, e'), E not given; calculated form factor. DWBA, broken pair model functions, meson exchange.

NUCLEAR STRUCTURE 58Ni, 88Sr; calculated levels, transition charge density. Broken pair model, meson exchange.

doi: 10.1016/0375-9474(85)90470-1
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1985VA01      Nucl.Phys. A436, 458 (1985)

A.van Egmond, K.Allaart, G.Bonsignori

Microscopic Approach to Magnetic Excitations in IBM-2

NUCLEAR REACTIONS 130,134Ba(e, e'), E not given; calculated form factors. Interacting boson approximation.

NUCLEAR STRUCTURE 130,134Ba; calculated levels, B(λ). Interacting boson approximation.

doi: 10.1016/0375-9474(85)90080-6
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1985VA18      Phys.Lett. 164B, 1 (1985)

A.Van Egmond, K.Allaart

Rotational and Intrinsic Excitations in IBA-2

NUCLEAR STRUCTURE 156Gd; calculated levels, band structure; deduced rotational, intrinsic excitation relationships. Interacting boson model, mean field approximation.

doi: 10.1016/0370-2693(85)90018-8
Citations: PlumX Metrics


1984VA22      Nucl.Phys. A425, 275 (1984)

A.Van Egmond, K.Allaart

Do We Understand IBM Parameters ( Question )

NUCLEAR STRUCTURE 124,128,132Xe; calculated B(E2), ratios. Interacting boson model, microscopic calculation dependent parameters.

doi: 10.1016/0375-9474(84)90076-9
Citations: PlumX Metrics


1983AK05      Z.Phys. A313, 213 (1983)

J.N.L.Akkermans, E.Loriaux, K.Allaart, G.Bonsignori

Correlated-Pair Structure in Nuclei and Possible Relation to IBM-2

NUCLEAR STRUCTURE 76,78,80Kr; calculated B(E2). Broken pair model.

doi: 10.1007/BF01417229
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1983VA04      Nucl.Phys. A394, 173 (1983)

A.Van Egmond, K.Allaart

Analysis of IBFA-Model Assumptions with the Broken-Pair Model

NUCLEAR STRUCTURE 125,131Xe; calculated interacting boson fermion model parameters. Broken pair model, empirical effective interaction.

doi: 10.1016/0375-9474(83)90168-9
Citations: PlumX Metrics


1983VA32      Phys.Lett. 131B, 275 (1983)

A.van Egmond, K.Allaart

Renormalization Contributions to IBM Parameters

NUCLEAR STRUCTURE 132,134Te, 130Sn; calculated levels; 120,132Xe; calculated D-pair state renormalization contributions. Shell model basis, comparision with interacting boson approximation.

doi: 10.1016/0370-2693(83)90497-5
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1982AK01      Z.Phys. A304, 245 (1982)

J.N.L.Akkermans, K.Allaart

The Empirical Form of the Effective Nucleon-Nucleon Interaction in a Model Space with Correlated J = 0 Pairs

NUCLEAR STRUCTURE 90Zr, 92Nb; calculated levels. 84Se, 86Kr, 88Sr, 92Mo, 94Ru; calculated 2+ level energies. Broken pair approximation, different effective interactions.

doi: 10.1007/BF01414500
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1981AL15      Nucl.Phys. A366, 384 (1981)

K.Allaart, P.Hofstra, V.Paar

A Quasiparticle-Cluster-Vibration Model for Odd-A Nuclei

NUCLEAR STRUCTURE 61,63,65,67Zn; calculated levels, B(λ), electric quadrupole, magnetic dipole moments. 63,65,67Zn; calculated γ-branching, T1/2. Quasicluster vibration model.

doi: 10.1016/0375-9474(81)90520-0
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1981VA10      Z.Phys. A300, 323 (1981)

A.van Egmond, P.Hofstra, E.Boeker, K.Allaart, V.Paar

Fermion-Boson Coupling Model (QCVM) Applied to Odd Zn Isotopes

NUCLEAR STRUCTURE 63,65,67Zn; calculated levels, B(λ). Quasicluster vibration model.


1981VA15      Z.Phys. A301, 137 (1981)

P.van Nes, K.Allaart, W.H.A.Hesselink, J.Konijn, H.Verheul

Nuclear g-Factors of the Jπ = (21/2)+ Isomer in 111In and the Jπ = 6+ Isomer in 112Sn

RADIOACTIVITY 111In, 112Sn [from 109Ag, 110Cd(α, 2n), E=28 MeV]; measured γ(θ, H, t). 111In, 112Sn level deduced g, configuration.


1980VA13      Nucl.Phys. A346, 70 (1980)

A.Van Poelgeest, J.Bron, W.H.A.Hesselink, K.Allaart, J.J.A.Zalmstra, M.J.Uitzinger, H.Verheul

Neutron Excitations in Even Mass Sn Nuclei

NUCLEAR REACTIONS 108,110,112,114,116Cd(α, 2n), E=17-33 MeV; measured Eγ, Iγ, γγ(t), σ(Eγ, θ), I(ce), linear polarization. 110,112,114,116,118Sn deduced levels, J, π, γ-branching, δ, T1/2, B(λ). Enriched targets, Ge(Li), Si(Li) detectors. Broken-pair model calculations.

doi: 10.1016/0375-9474(80)90489-3
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1979HO20      Z.Phys. A292, 159 (1979)

P.Hofstra, K.Allaart

A Broken-Pair Description of 89Y, 91Nb and 93Tc

NUCLEAR STRUCTURE 89Y, 91Nb, 93Tc; calculated low-energy level properties; deduced no deformed states.

doi: 10.1007/BF01441623
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1978AL11      Z.Phys. A286, 187 (1978)

K.Allaart, H.Muther

Hermitian Operator Method Calculation in the pf-Shell

NUCLEAR STRUCTURE 46,48,50Ti, 50,52Cr, 54Fe; calculated levels, B(E2).

doi: 10.1007/BF01408975
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1978VA13      Z.Phys. A288, 49 (1978)

W.F.van Gunsteren, K.Allaart, P.Hofstra

Number-Projected Three-Quasiparticle Description of the Odd Sn Isotopes

NUCLEAR STRUCTURE 115,117Sn; calculated levels, γ-branching, T1/2, B(λ).


1977AK01      Nucl.Phys. A282, 291 (1977)

J.N.L.Akkermans, K.Allaart, E.Boeker

Pairing Correlations in Excited States of Superfluid Nuclei

NUCLEAR STRUCTURE 91Nb, 118Sn; calculated levels. Pairing correlations.

doi: 10.1016/0375-9474(77)90216-0
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1977MU05      Phys.Rev. C15, 1467 (1977)

H.Muther, K.Goeke, K.Allaart, A.Faessler

Single-Particle Degrees of Freedom and the Generator-Coordinate Method

NUCLEAR STRUCTURE 46,50Ti, 52Cr, 54Fe; calculated levels, B(E2).

doi: 10.1103/PhysRevC.15.1467
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1976MU04      Phys.Lett. 60B, 427 (1976)

H.Muther, K.Goeke, A.Faessler, K.Allaart

High Spin States in Doubly Even pf-Shell Nuclei

NUCLEAR STRUCTURE 46,50Ti, 52Cr, 54Fe; calculated levels.

doi: 10.1016/0370-2693(76)90698-5
Citations: PlumX Metrics


1976VA08      Z.Phys. A276, 1 (1976)

W.F.van Gunsteren, K.Allaart

Influence of an Enlargement of the Model Space on Number Projected Quasiparticle Calculations

NUCLEAR STRUCTURE 112,114,116,118Sn; calculated quasi-particle energies, force strengths, B(λ).

NUCLEAR REACTIONS 114,116,118Sn(p, t); calculated σ.


1976VA16      Nucl.Phys. A266, 365 (1976)

W.F.Van Gunsteren, K.Allaart, E.Boeker

A Particle-Quasiparticle Description of 112,114,116Sb

NUCLEAR STRUCTURE 112,114,116Sb; calculated levels, γ-branching, T1/2.

doi: 10.1016/0375-9474(76)90364-X
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1975GO10      Nucl.Phys. A243, 440 (1975)

K.Goeke, M.V.Mihailovic, K.Allaart, A.Faessler

The Generator Coordinate Method as an Approximation to the Shell Model. A Comparison on 24Ne

NUCLEAR STRUCTURE 24Ne; calculated levels.

doi: 10.1016/0375-9474(75)90288-2
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1975MU10      Nucl.Phys. A248, 451 (1975)

H.Muther, K.Allaart, K.Goeke, A.Faessler

Microscopic Description of Collective Motion in pf Shell Nuclei

NUCLEAR STRUCTURE 56Fe, 50,52,54Cr, 46,48Ti; calculated levels. 50Cr, 56Fe; calculated B(E2).

doi: 10.1016/0375-9474(75)90524-2
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1974AL02      Phys.Rev. C9, 988 (1974)

K.Allaart, K.Goeke, H.Muther, A.Faessler

Microscopic, Nonharmonic Description of Rotations and Pairing Vibrations in Deformed pf-Shell Nuclei

NUCLEAR STRUCTURE 48Ti, 56Fe; calculated rotational spectra. Hartree-Bogoliubov, generator-coordinate method, J projection.

doi: 10.1103/PhysRevC.9.988
Citations: PlumX Metrics


1974GO33      Z.Phys. 271, 377 (1974)

K.Goeke, K.Allaart, H.Muther, A.Faessler

Study of pf-Shell Nuclei with a Symmetry Conserving Generator Coordinate Method

NUCLEAR STRUCTURE 48Ti, 52Cr, 56Fe; calculated levels.

doi: 10.1007/BF02126193
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1974GR17      Nucl.Phys. A225, 443 (1974)

F.Grummer, K.Goeke, K.Allaart, A.Faessler

Antipairing and Antistretching in 22Ne

NUCLEAR STRUCTURE 22Ne; calculated B(E2), levels, quadrupole moment.

doi: 10.1016/0375-9474(74)90352-2
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1974VA04      Z.Phys. 267, 87 (1974)

W.F.van Gunsteren, E.Boeker, K.Allaart

The FBCS Model and the Inverse Gap Equations Applied to the Tin Isotopes

NUCLEAR STRUCTURE 112,114,116,118,120,122,124Sn; calculated levels, effective charge, S. 111,113,115,117,119,121,123,125Sn calculated S.

doi: 10.1007/BF01668634
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1974VA30      Nucl.Phys. A236, 317 (1974)

W.F.Van Gunsteren, K.Allaart

Can the 0+ States of Even Superfluid Nuclei be Described by Anharmonic Pairing Vibrations (Question)

NUCLEAR REACTIONS 114Sn(t, p); calculated σ.

doi: 10.1016/0375-9474(74)90257-7
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1973AL21      Z.Phys. 263, 407 (1973)

K.Allaart, K.Goeke, A.Faessler

On Number and Angular Momentum Projection from Hartree-Bogoliubov States

NUCLEAR STRUCTURE 22,24Ne, 26Mg; calculated levels.

doi: 10.1007/BF01391990
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1972AL38      Nucl.Phys. A198, 33 (1972)

K.Allaart, E.Boeker

FBCS for Odd Nuclei and the Inverse Gap Equations: Application to N = 50 Isotones

doi: 10.1016/0375-9474(72)90770-1
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1971AL13      Nucl.Phys. A168, 630 (1971)

K.Allaart, E.Boeker

Comparison between the BCS and the FBCS Formalisms as Approximations to the Low-Seniority Shell Model

NUCLEAR STRUCTURE 116,118Sn, 88Sr, 90Zr, 92Mo; calculated levels, occupation probabilities. BCS, FBCS formalisms.

doi: 10.1016/0375-9474(71)90551-3
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