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NSR database version of May 30, 2024.

Search: Author = P.J.Mulders

Found 31 matches.

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2018MU04      Few-Body Systems 59, 10 (2018)

P.J.Mulders

The 3D Entangled Structure of the Proton: Transverse Degrees of Freedom in QCD, Momenta, Spins and More

NUCLEAR STRUCTURE 1H; calculated 3D structure including partonic transverse momenta.

doi: 10.1007/s00601-018-1334-6
Citations: PlumX Metrics


2005MU16      Prog.Part.Nucl.Phys. 55, 243 (2005)

P.J.Mulders

Polarized structure functions

doi: 10.1016/j.ppnp.2005.01.016
Citations: PlumX Metrics


2004BA55      Phys.Lett. B 595, 309 (2004)

A.Bacchetta, P.J.Mulders, F.Pijlman

New observables in longitudinal single-spin asymmetries in semi-inclusive DIS

NUCLEAR REACTIONS 1H(e, e'X), (polarized e, e'X), E not given; calculated polarization observables. Polarized and unpolarized targets considered.

doi: 10.1016/j.physletb.2004.06.052
Citations: PlumX Metrics


2002BB09      Acta Phys.Pol. B33, 3761 (2002)

A.Bacchetta, R.Kundu, A.Metz, P.J.Mulders

Estimate of the Collins Function in a Chiral Invariant Approach


2002OG11      Nucl.Phys. A711, 89c (2002)

K.A.Oganessyan, P.J.Mulders, E.De Sanctis, L.S.Asilyan

Kinematical contributions to the transverse asymmetry in semi-inclusive DIS

NUCLEAR REACTIONS 1H(polarized e, e'X), E=high; calculated pion production associated double spin asymmetries. Polarized target.

doi: 10.1016/S0375-9474(02)01200-9
Citations: PlumX Metrics


2001MU15      Phys.Rev. D63, 094021 (2001)

P.J.Mulders, J.Rodrigues

Transverse Momentum Dependence in Gluon Distribution and Fragmentation Functions

doi: 10.1103/PhysRevD.63.094021
Citations: PlumX Metrics


2000BA60      Phys.Rev.Lett. 85, 712 (2000)

A.Bacchetta, M.Boglione, A.Henneman, P.J.Mulders

Bounds on Transverse Momentum Dependent Distribution and Fragmentation Functions

doi: 10.1103/PhysRevLett.85.712
Citations: PlumX Metrics


2000BA97      Phys.Rev. D62, 114004 (2000)

A.Bacchetta, P.J.Mulders

Deep Inelastic Leptoproduction of Spin-One Hadrons

doi: 10.1103/PhysRevD.62.114004
Citations: PlumX Metrics


2000BO09      Phys.Lett. 478B, 114 (2000)

M.Boglione, P.J.Mulders

Azimuthal Spin Asymmetries in Semi-Inclusive Production from Positron-Proton Scattering

NUCLEAR REACTIONS 1H(e+, X), E not given; calculated polarized fragmentation and distribution functions.

doi: 10.1016/S0370-2693(00)00285-9
Citations: PlumX Metrics


2000MU09      Nucl.Phys. A666-667, 257c (2000)

P.J.Mulders, M.Boglione

Perspectives in Polarized Leptoproduction

doi: 10.1016/S0375-9474(00)00034-8
Citations: PlumX Metrics


1999BO35      Phys.Rev. D60, 054007 (1999)

M.Boglione, P.J.Mulders

Time-Reversal Odd Fragmentation and Distribution Functions in pp and ep Single Spin Asymmetries

NUCLEAR REACTIONS 1H(p, X), (e, X), E not given; calculated time-reversal-odd distribution, fragmentation functions. Polarized target.

doi: 10.1103/PhysRevD.60.054007
Citations: PlumX Metrics


1998MU15      Acta Phys.Pol. B29, 1225 (1998)

P.J.Mulders

Single Spin Asymmetries in Semi-Inclusive Deep Inelastic Scattering

NUCLEAR REACTIONS 1H(e, e'X), E not given; calculated deep inelastic scattering nucleon structure effects. Polarized target.


1997AM07      Nucl.Phys. A622, 315c (1997)

C.Amsler, T.Bressani, F.E.Close, E.De Sanctis, B.Frois, D.von Harrach, F.Kunne, J.M.Laget, V.Metag, P.J.Mulders, D.O.Riska

Perspective in Hadron and Quark Dynamics

NUCLEAR REACTIONS 208Pb(e, e'p), 12C, 16O(e, e'X), 12C(γ, X), E not given; compiled, reviewed data, analyses. Reviewed available accelerator facilities.

doi: 10.1016/S0375-9474(97)00348-5
Citations: PlumX Metrics


1997JA11      Nucl.Phys. A626, 937 (1997)

R.Jakob, P.J.Mulders, J.Rodrigues

Modelling Quark Distribution and Fragmentation Functions

NUCLEAR STRUCTURE 1n, 1H; calculated quark distribution, fragmentation functions. Non-local operators, spectator model.

doi: 10.1016/S0375-9474(97)00588-5
Citations: PlumX Metrics


1997MU26      Nucl.Phys. A622, 239c (1997)

P.J.Mulders

Prospects for Spin Physics in Semi-Inclusive Processes

doi: 10.1016/S0375-9474(97)00344-8
Citations: PlumX Metrics


1995MU08      Nucl.Phys. A588, 876 (1995)

P.J.Mulders, S.J.Pollock

Evolution of the Spin of the Nucleon

doi: 10.1016/0375-9474(95)00083-D
Citations: PlumX Metrics


1995UM02      Phys.Rev.Lett. 74, 4993 (1995)

Y.Umino, J.M.Udias, P.J.Mulders

Exchange Current Correlations to Neutrino-Nucleus Scattering

NUCLEAR REACTIONS 12C(ν, ν'p), (ν, μ-), E not given; calculated differential σ. Relativistic exchange current corrections.

doi: 10.1103/PhysRevLett.74.4993
Citations: PlumX Metrics


1994ME05      Nucl.Phys. A570, 497 (1994)

H.Meyer, P.J.Mulders, W.F.M.Spit

Quark Antisymmetrization and Deep-Inelastic Scattering II. Nuclear Structure Functions

NUCLEAR STRUCTURE 4He, 6Li, 14N; calculated structure functions ratio f(q/A)(x)/f(q/A)(a)(x). Quark antisymmetrization, deep inelastic scattering.

doi: 10.1016/0375-9474(94)90070-1
Citations: PlumX Metrics


1994SP02      Nucl.Phys. A570, 472 (1994)

W.F.M.Spit, A.G.M.van Hees, P.J.Brussaard, P.J.Mulders

Quark Antisymmetrization and Deep-Inelastic Scattering I. Nuclear Quark Momentum Distributions

NUCLEAR STRUCTURE 6Li, 14N, 16O; calculated charge density for different deformations. Full, impulse approximation calculations. Quark antisymmatrization, deep inelastic scattering.

doi: 10.1016/0375-9474(94)90069-8
Citations: PlumX Metrics


1993SP03      Nucl.Phys. A553, 689c (1993)

W.F.M.Spit, V.Vento, A.G.M.van Hees, P.J.Brussaard, P.J.Mulders

Quark Antisymmetrization in Nuclei

NUCLEAR STRUCTURE 6Li, 16O; calculated Coulomb, magnetic form factors, charge density. 14N; calculated charge density. Quark antisymmetrization.

doi: 10.1016/0375-9474(93)90680-V
Citations: PlumX Metrics


1991KU06      Phys.Lett. 255B, 11 (1991)

J.Kunz, P.J.Mulders, G.A.Miller

Charge Distributions of Hyperons

NUCLEAR STRUCTURE 1n, 1H; calculated electric rms radii. Skyrme model.

doi: 10.1016/0370-2693(91)91131-E
Citations: PlumX Metrics


1991ME01      Nucl.Phys. A528, 589 (1991)

H.Meyer, P.J.Mulders

Polarized and Unpolarized Structure Functions in a Diquark Model for the Nucleon

NUCLEAR STRUCTURE 1n, 1H; calculated structure function, ratio. Diquark model.

doi: 10.1016/0375-9474(91)90252-2
Citations: PlumX Metrics


1990KU05      Z.Phys. C46, S25 (1990)

J.Kunz, P.J.Mulders

Hyperons in the Bound State Approach to the Skyrme Model. Magnetic Moments of Baryons

NUCLEAR STRUCTURE 1H, 1n; calculated μ. Skyrme model.


1990SP03      Nucl.Phys. A510, 609 (1990)

W.F.M.Spit, A.G.M.van Hees, P.J.Mulders

Quark Exchange and Nuclear Form Factors

NUCLEAR STRUCTURE 6Li, 16O; calculated form factors. Quark exchange.

doi: 10.1016/0375-9474(90)90351-L
Citations: PlumX Metrics


1989KU25      Phys.Lett. 231B, 335 (1989)

J.Kunz, P.J.Mulders

Magnetic Moments of Hyperons in the Bound State Approach to the Skyrme Model

NUCLEAR STRUCTURE 1n, 1H; calculated μ. Skyrme model, Callan-Klebanov ansatz.

doi: 10.1016/0370-2693(89)90671-0
Citations: PlumX Metrics


1988DI10      Nucl.Phys. A489, 627 (1988)

A.E.L.Dieperink, P.J.Mulders

Quark Exchange in Quasi-Elastic Electron-Nucleus Scattering

NUCLEAR STRUCTURE 2H, 4He; calculated longitudinal, transverse structure function. Quark exchange.

NUCLEAR REACTIONS 4He(e, e'p), E not given; calculated spectroscopic function. Quark exchange.

doi: 10.1016/0375-9474(88)90113-3
Citations: PlumX Metrics


1988MU11      Nucl.Phys. A483, 461 (1988)

P.J.Mulders, A.E.L.Dieperink

Quark Exchange Effects in Nuclei

NUCLEAR STRUCTURE 2,3H, 3,4He; calculated nuclear, electromagnetic form factors.

doi: 10.1016/0375-9474(88)90079-6
Citations: PlumX Metrics


1987VA08      Phys.Rev.Lett. 58, 1727 (1987)

G.van der Steenhoven, A.M.van den Berg, H.P.Blok, S.Boffi, J.F.J.van den Brand, R.Ent, T.de Forest, Jr., C.Giusti, J.W.A.den Herder, E.Jans, G.J.Kramer, J.B.J.M.Lanen, L.Lapikas, J.Mougey, P.J.Mulders, F.D.Pacati, E.N.M.Quint, P.K.A.de Witt Huberts

Nuclear-Density Dependence of the Electron-Proton Coupling

NUCLEAR REACTIONS 6Li(e, e'p), E=322, 479.9 MeV; measured reduced σ ratios; deduced electron-proton coupling nuclear density dependence. Enriched target. DWIA analyses.

doi: 10.1103/PhysRevLett.58.1727
Citations: PlumX Metrics


1987VA15      Phys.Lett. 191B, 227 (1987)

G.Van der Steenhoven, H.P.Blok, M.Thies, P.J.Mulders

Charge-Exchange Processes in the Quasi-Elastic (e, e'p) and (e, e'n) Reactions

NUCLEAR REACTIONS 12C(e, e'p), (e, e'n), E=313, 443 MeV; calculated quasielastic σ; deduced channel differences. Lane equations.

doi: 10.1016/0370-2693(87)90244-9
Citations: PlumX Metrics


1986MU14      Nucl.Phys. A459, 525 (1986)

P.J.Mulders

Effective Hadronic Degrees of Freedom in Electron-Nucleus Scattering

NUCLEAR REACTIONS 12C(e, e'), E not given; calculated longitudinal, transverse structure function. Six quark hadronic states, y-scaling.

NUCLEAR STRUCTURE 3He, 12C, 40,48Ca, 56Fe; calculated protonic μ, scaling function. Six quark hadronic states.

doi: 10.1016/0375-9474(86)90159-4
Citations: PlumX Metrics


1986VA17      Phys.Rev.Lett. 57, 182 (1986)

G.van der Steenhoven, H.P.Blok, J.F.J.van den Brand, T.de Forest, Jr., J.W.A.den Herder, E.Jans, P.H.M.Keizer, L.Lapikas, P.J.Mulders, E.N.M.Quint, P.K.A.de Witt Huberts, J.Mougey, S.Boffi, C.Giusti, F.D.Pacati

Effect of Nuclear Medium on the Proton Investigated with Reaction 12C(e, e'p)11B

NUCLEAR REACTIONS 12C(e, e'p), E=312.8, 443.3 MeV; measured σ(E(e'), θ(e'), Ep', θp); deduced longitudinal, transverse response functions, medium effects.

doi: 10.1103/PhysRevLett.57.182
Citations: PlumX Metrics


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