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NSR database version of May 22, 2024.

Search: Author = U.Mosel

Found 271 matches.

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2022GA34      Phys.Rev. C 106, 064910 (2022)

K.Gallmeister, U.Mosel, L.von Smekal

Dilepton decay of low-mass ρ mesons

doi: 10.1103/PhysRevC.106.064910
Citations: PlumX Metrics

2020LA14      Phys.Rev. C 102, 064913 (2020)

A.B.Larionov, U.Mosel, L.von Smekal

Dilepton production in microscopic transport theory with an in-medium ρ-meson spectral function

doi: 10.1103/PhysRevC.102.064913
Citations: PlumX Metrics

2019MO13      Phys.Rev. C 99, 035502 (2019)

U.Mosel, K.Gallmeister

Addendum to "Muon-neutrino-induced charged-current pion production on nuclei"

NUCLEAR REACTIONS C, 1H(ν, π+), at pion momentum of 0.2-1 GeV; calculated differential σ(E) and angular distribution of pions, momentum distribution and angular distribution of outgoing muons in π+ production mechanism using Giessen-Boltzmann-Uehling-Uhlenbeck (GiBUU) calculations. Comparison with pion production data on H2O in the T2K experiment as well as those from MINERvA experiment.

doi: 10.1103/PhysRevC.99.035502
Citations: PlumX Metrics

2019MO22      Phys.Rev. C 99, 064605 (2019)

U.Mosel, K.Gallmeister

Cross sections for A(e, e')X reactions

NUCLEAR REACTIONS 12C, 40Ar, 48Ti(e, e'), E=2.222 GeV; calculated inclusive differential σ(E, θ) using transport theoretical framework and the GIBUU code. Comparison with experimental data from Jefferson Lab.

doi: 10.1103/PhysRevC.99.064605
Citations: PlumX Metrics

2018DO13      Phys.Rev. C 98, 045502 (2018)

S.Dolan, U.Mosel, K.Gallmeister, L.Pickering, S.Bolognesi

Sensitivity of neutrino-nucleus interaction measurements to 2p2h excitations

NUCLEAR REACTIONS 1H(ν, μ), E ∼ 0.6 GeV; calculated differential σ(θ) of T2K measurements as a function of muon kinematics for C8H8 target near the detector using GIBUU transport code; analyzed differential σ(θ) data from T2K collaboration; deduced strength of 2p2h multinucleon correlations between electron-nucleus and neutrino-nucleus reactions.

doi: 10.1103/PhysRevC.98.045502
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2018MO10      Phys.Rev. C 97, 045501 (2018)

U.Mosel, K.Gallmeister

Muon-neutrino-induced charged-current cross section without pions: Theoretical analysis

NUCLEAR REACTIONS 12C(e, e'), (e, X), E=680 MeV; 16O(e, e'), (e, X), E=0.7, 0.737, 0.88, 1.08, 1.20, 1.50 GeV; 12C, 16O(ν, μ), E at 0-1500 MeV/c; calculated inclusive double differential σ(ω, θ), inclusive double differential σ(p(-μ), θ) muon momentum distributions per nucleon using quantum-kinetic transport theory, and GiBUU code; discussed contribution of 2p2h processes. Comparison with theoretical predictions and experimental results from T2K Collaboration.

doi: 10.1103/PhysRevC.97.045501
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2017MO20      Phys.Rev. C 96, 015503 (2017)

U.Mosel, K.Gallmeister

Muon-neutrino-induced charged-current pion production on nuclei

NUCLEAR REACTIONS H, C, O, Cl, 40Ar(ν, π), E(π)=0-0.5 GeV; calculated kinetic energy and momentum spectra per nucleon, angular distribution and momentum distribution of positively charged pions for the MiniBooNE flux with a CH2 target, MicroBooNE flux for 40Ar target, T2K ND280 flux for H2O target, for the MINERvA flux for a CH target, and NOvA flux at the ND for CH2+Cl (NOvA) target. Giessen-Boltzmann-Uehling-Uhlenbeck (GBUU) model. Comparison with experimental data.

doi: 10.1103/PhysRevC.96.015503
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2016GA35      Phys.Rev. C 94, 035502 (2016)

K.Gallmeister, U.Mosel, J.Weil

Neutrino-induced reactions on nuclei

NUCLEAR REACTIONS 12C(e, e'), E=240, 560 MeV; calculated inclusive σ(E, θ). 12C(ν, μ), (ν-bar, μ), at Q2<1 GeV2; calculated double differential cross sections and forward angle double differential cross section per neutron and per proton using Giessen-Boltzmann-Uehling-Uhlenbeck (GiBUU) quantum-kinetic transport theory with improvements in the treatment of nuclear g.s. and 2p2h interactions. Comparison with experimental data from MiniBooNE collaboration.

doi: 10.1103/PhysRevC.94.035502
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2016MO25      Phys.Rev. C 94, 034610 (2016)

U.Mosel, K.Gallmeister

Mass dependence and isospin dependence of short-range correlated pairs

NUCLEAR REACTIONS 12C, 24Mg, 58Ni, 208Pb(e, e'pp), (e, e'np), E not given; calculated numbers of pp and pn pairs with short-range correlations for target mass in the range of A=10-250 using transparent geometrical model within a zero-range approximation Comparison with available experimental data.

doi: 10.1103/PhysRevC.94.034610
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2016SH14      Phys.Rev. C 93, 045206 (2016)

V.Shklyar, H.Lenske, U.Mosel

2π production in the Giessen coupled-channels model

doi: 10.1103/PhysRevC.93.045206
Citations: PlumX Metrics

2015MO11      Phys.Rev. C 91, 065501 (2015)


Pion production in high-energy neutrino reactions with nuclei

doi: 10.1103/PhysRevC.91.065501
Citations: PlumX Metrics

2013GA37      Nucl.Phys. A914, 405c (2013)

T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel, A.Obermann

In-medium effects on hypernuclear formation

NUCLEAR REACTIONS 1H(Λ, Λ), E at 0.1-0.5 GeV/c;1H(Λ, Σ0), E at 0.5-2 GeV/c;1H(Σ-, Σ-), E at 0.12-0.18 GeV/c;1H(Σ-, Λ), (Σ-, Σ0), E at 0.1-0.8 GeV/c;1H(p(bar), Λ), (p-bar, Ξ-bar), E at 2.2-3.2 GeV/c; calculated σ using parameterization. 1n(Σ+, Σ+), E=0-400 MeV;1H(Λ, Λ), E=0-400 MeV; calculated σ using GiBUU (Giessen BUU).

doi: 10.1016/j.nuclphysa.2012.12.124
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2013LA04      Phys.Rev. C 87, 014602 (2013)

O.Lalakulich, U.Mosel

Pion production in the MiniBooNE experiment

doi: 10.1103/PhysRevC.87.014602
Citations: PlumX Metrics

2013LA24      Phys.Rev. C 88, 017601 (2013)

O.Lalakulich, U.Mosel

Pion production in the T2K experiment

doi: 10.1103/PhysRevC.88.017601
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2013SH03      Phys.Rev. C 87, 015201 (2013)

V.Shklyar, H.Lenske, U.Mosel

η-meson production in the resonance-energy region

doi: 10.1103/PhysRevC.87.015201
Citations: PlumX Metrics

2012GA19      Nucl.Phys. A881, 240 (2012)

T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel

Formation of double-Λ hypernuclei at PANDA

NUCLEAR REACTIONS 12C, Cu, 165Ho, 197Au, 238U(p-bar, X), E-1.22 GeV; calculated σ, dσ. 64Cu(p-bar, X), (p, X), E=5 GeV; calculated fragment multiplicity, yields, fragment E*, Λ, 2Λ, Ξ- rapidity distribution, dσ, σ.

doi: 10.1016/j.nuclphysa.2011.12.010
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2012LA06      Phys.Rev. C 85, 024614 (2012)

A.B.Larionov, T.Gaitanos, U.Mosel

Kaon and hyperon production in antiproton-induced reactions on nuclei

doi: 10.1103/PhysRevC.85.024614
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2012LA15      Phys.Rev. C 86, 014607 (2012)

O.Lalakulich, K.Gallmeister, U.Mosel

Neutrino- and antineutrino-induced reactions with nuclei between 1 and 50 GeV

doi: 10.1103/PhysRevC.86.014607
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2012LA16      Phys.Rev. C 86, 014614 (2012); Erratum Phys.Rev. C 90, 029902 (2014)

O.Lalakulich, K.Gallmeister, U.Mosel

Many-body interactions of neutrinos with nuclei: Observables

doi: 10.1103/PhysRevC.86.014614
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2012LA28      Phys.Rev. C 86, 054606 (2012)

O.Lalakulich, U.Mosel, K.Gallmeister

Neutrino energy reconstruction in quasielastic-like scattering in the MiniBooNE and T2K experiments

NUCLEAR REACTIONS C, 16O(ν, μ-p), E<2.5 GeV; analyzed quasielastic (QE) neutrino scattering cross sections, QE-like cross sections, reconstructed neutrino energies. Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU) transport model.

doi: 10.1103/PhysRevC.86.054606
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2012WE12      Eur.Phys.J. A 48, 111 (2012); Erratum Eur.Phys.J. A 48, 150 (2012)

J.Weil, H.van Hees, U.Mosel

Dilepton production in proton-induced reactions at SIS energies with the GiBUU transport model

doi: 10.1140/epja/i2012-12111-9
Citations: PlumX Metrics

2011GA04      Phys.Rev. C 83, 015201 (2011)

K.Gallmeister, M.Kaskulov, U.Mosel

Color transparency in hadronic attenuation of ρ0 mesons

doi: 10.1103/PhysRevC.83.015201
Citations: PlumX Metrics

2011KA39      Phys.Rev. C 84, 065206 (2011)

M.M.Kaskulov, U.Mosel

Primakoff production of π0, η, and η' in the Coulomb field of a nucleus

doi: 10.1103/PhysRevC.84.065206
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2010GA08      Phys.Rev. C 81, 054316 (2010)

T.Gaitanos, A.B.Larionov, H.Lenske, U.Mosel

Breathing mode in an improved transport approach

NUCLEAR STRUCTURE 12C, 100Sn; calculated rms radii, binding energies, neutron and proton density profiles, proton mean-field potentials. 12C, 56Ni, 96Ru, 124,136Sn, 208Pb; calculated rms radii. A=10-210; calculated excitation energies and widths of giant-monopole resonances (GMR).Improved relativistic Boltzmann-Uehling-Uhlenbeck (BUU) transport approach.

doi: 10.1103/PhysRevC.81.054316
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2010KA09      Phys.Rev. C 81, 045202 (2010)

M.M.Kaskulov, U.Mosel

Deep exclusive charged π electroproduction above the resonance region

doi: 10.1103/PhysRevC.81.045202
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2010LE08      Phys.Rev. C 81, 064614 (2010)

T.Leitner, U.Mosel

Neutrino-nucleus scattering reexamined: Quasielastic scattering and pion production entanglement and implications for neutrino energy reconstruction

NUCLEAR REACTIONS 12C(ν, ν), E=0.5-2 GeV; calculated quasielastic σ, dσ/dE(ν), influence of neutrino oscillations, effects of pion production using Giessen Boltzmann-Uehling-Uhlenbeck (GiBUU) theory.

doi: 10.1103/PhysRevC.81.064614
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2010LE17      Phys.Rev. C 82, 035503 (2010)

T.Leitner, U.Mosel

Neutrino-nucleus interactions in the T2K experiment

doi: 10.1103/PhysRevC.82.035503
Citations: PlumX Metrics

2010SH14      Phys.Rev. C 82, 015203 (2010)

V.Shklyar, H.Lenske, U.Mosel

Spin-5/2 fields in hadron physics

doi: 10.1103/PhysRevC.82.015203
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2010SH31      Phys.Rev. C 82, 062201 (2010)

R.Shyam, U.Mosel

Dilepton production in proton-proton and quasifree proton-neutron reactions at 1.25 GeV

doi: 10.1103/PhysRevC.82.062201
Citations: PlumX Metrics

2009GA10      Phys.Lett. B 675, 297 (2009)

T.Gaitanos, H.Lenske, U.Mosel

Formation of hypernuclei in high energy reactions within a covariant transport model

doi: 10.1016/j.physletb.2009.04.038
Citations: PlumX Metrics

2009GA25      Nucl.Phys. A826, 151 (2009)

K.Gallmeister, U.Mosel

Production of charged pions off nuclei with 3-30 GeV incident protons and pions

doi: 10.1016/j.nuclphysa.2009.05.104
Citations: PlumX Metrics

2009GA26      Nucl.Phys. A828, 9 (2009)

T.Gaitanos, M.Kaskulov, U.Mosel

Non-linear derivative interactions in relativistic hadrodynamics

doi: 10.1016/j.nuclphysa.2009.06.019
Citations: PlumX Metrics

2009KA02      Phys.Rev. C 79, 015207 (2009)

M.M.Kaskulov, K.Gallmeister, U.Mosel

Pionic transparency in semi-exclusive electroproduction off nuclei

NUCLEAR REACTIONS 1H(e, e'π+), E not given; calculated σ(θ). 12C, 27Al, 63Cu, 197Au(e, e'π+), E not given; calculated nuclear transparency of pions. Comparison with experimental data.

doi: 10.1103/PhysRevC.79.015207
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2009KA25      Phys.Rev. C 80, 028202 (2009)

M.M.Kaskulov, U.Mosel

Deep exclusive electroproduction of π+ from data measured with the HERMES detector at DESY

doi: 10.1103/PhysRevC.80.028202
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2009LE08      Phys.Rev. C 79, 034601 (2009)

T.Leitner, O.Buss, L.Alvarez-Ruso, U.Mosel

Electron- and neutrino-nucleus scattering from the quasielastic to the resonance region

NUCLEAR REACTIONS 1H(ν, μ), E=0.5-2 GeV; 16O(e, e), E=0.537, 0.7, 0.737, 0.88, 1.08, 1.2, 1.5 GeV; 16O(ν, μ-), E=0.5, 0.75, 1.0, 1.25, 1.5 GeV; 16O(ν, ν), E=1.0 GeV; 16O(ν, e), E=0-1.4 GeV; calculated cross sections as a function of energy transfer. 16O; calculated momentum density distribution of protons, probability distributions of nucleons. Giessen Boltzmann-Uehling-Uhlenbeck model.

doi: 10.1103/PhysRevC.79.034601
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2009LE09      Phys.Rev. C 79, 038501 (2009)

T.Leitner, O.Buss, U.Mosel, L.Alvarez-Ruso

Neutrino-induced pion production at energies relevant for the MiniBooNE and K2K experiments

NUCLEAR REACTIONS 12C, 16O(ν, π0), 12C(ν, π+), E=0.5-2.0 GeV; measured pion production as a function of kinetic energy, single π+ cross sections for charged current. Giessen Boltzmann-Uehling-Uhlenbeck model for neutrino induced reactions to charged current and neutral current pion production.

doi: 10.1103/PhysRevC.79.038501
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2009LE15      Phys.Rev. C 79, 057601 (2009)

T.Leitner, U.Mosel, S.Winkelmann

Neutrino-induced coherent pion production off nuclei reexamined

NUCLEAR REACTIONS 12C(ν, π+), E=500, 850, 1000 MeV; calculated σ(θ) and pion momentum distributions. Comparison between full calculations and local approximated calculations.

doi: 10.1103/PhysRevC.79.057601
Citations: PlumX Metrics

2009SH13      Phys.Rev. C 79, 035203 (2009)

R.Shyam, U.Mosel

Dilepton production in nucleon-nucleon collisions reexamined

doi: 10.1103/PhysRevC.79.035203
Citations: PlumX Metrics

2008GA05      Nucl.Phys. A801, 68 (2008)

K.Gallmeister, U.Mosel

Time dependent hadronization via HERMES and EMC data consistency

doi: 10.1016/j.nuclphysa.2007.12.009
Citations: PlumX Metrics

2008SH13      Phys.Rev. C 77, 052201 (2008)

R.Shyam, H.Lenske, U.Mosel

Hypernuclear production by the (γ, K+) reaction within a relativistic model

NUCLEAR REACTIONS 16O(γ, K+)16N, E<2 GeV; calculated momentum distributions, σ, levels, J, π for hypernuclei.

doi: 10.1103/PhysRevC.77.052201
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2007BU28      Phys.Rev. C 76, 035502 (2007)

O.Buss, T.Leitner, U.Mosel, L.Alvarez-Ruso

Influence of the nuclear medium on inclusive electron and neutrino scattering off nuclei

doi: 10.1103/PhysRevC.76.035502
Citations: PlumX Metrics

2007GA10      Nucl.Phys. A782, 166c (2007)

K.Gallmeister, T.Leitner, S.Leupold, U.Mosel, P.Muehlich, L.Alvarez-Ruso, V.Shklyar

In-medium Hadrons - Properties, Interaction and Formation

doi: 10.1016/j.nuclphysa.2006.10.040
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2007LA32      Phys.Rev. C 76, 044909 (2007)

A.B.Larionov, O.Buss, K.Gallmeister, U.Mosel

Three-body collisions in Boltzmann-Uehling-Uhlenbeck theory

doi: 10.1103/PhysRevC.76.044909
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2006BU15      Eur.Phys.J. A 29, 189 (2006)

O.Buss, L.Alvarez-Ruso, P.Muhlich, U.Mosel

Low-energy pions in nuclear matter and ππ photoproduction within a BUU transport model

NUCLEAR REACTIONS 1H(π+, π+), (π-, π-), (π-, π0), (π+, X), (π-, X), (π0, X), E(cm) ≈ 1-1.7 GeV; 1H(p, pπ0), (n, pπ-), (n, nπ0), (p, nπ+), E(cm) ≈ 2-2.5 GeV; calculated σ. C, Al, Cu, Sn, Au(π+, X), (π-, X), E ≈ 10-120 MeV; calculated absorption σ. 1n, 1H(γ, 2π0), (γ, π+π-), 1H(γ, π0π+), 1n(γ, π0π-), E=0.4-0.5 GeV; C, Ca, Pb(γ, 2π0X), (γ, π0π+X), (γ, π0π-X), E ≈ 0.25-0.5 GeV; calculated two-pion invariant mass spectra. Transport model, comparisons with data.

doi: 10.1140/epja/i2006-10075-y
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2006BU21      Phys.Rev. C 74, 044610 (2006)

O.Buss, L.Alvarez-Ruso, A.B.Larionov, U.Mosel

Pion-induced double-charge exchange reactions in the Δ resonance region

NUCLEAR REACTIONS 16O, 40Ca, 208Pb(π+, π-X), (π-, π+X), E=120, 150, 180 MeV; calculated σ(E, θ). Transport model, comparison with data.

doi: 10.1103/PhysRevC.74.044610
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2006LE15      Prog.Part.Nucl.Phys. 57, 395 (2006)

T.Leitner, L.Alvarez-Ruso, U.Mosel

Modelling nuclear effects in neutrino scattering

NUCLEAR REACTIONS 56Fe(ν, π+), (ν, π0), (ν, π-), E=0.7-1/5 GeV; calculated σ, nuclear medium and final-state interaction effects, pion momentum spectra.

doi: 10.1016/j.ppnp.2005.11.007
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2006LE25      Phys.Rev. C 73, 065502 (2006)

T.Leitner, L.Alvarez-Ruso, U.Mosel

Charged current neutrino-nucleus interactions at intermediate energies

NUCLEAR REACTIONS 56Fe(ν, μ-X), E=0.2-2 GeV; calculated inclusive σ, σ(E, θ), pion production and nucleon knockout σ, σ(E, θ); deduced nuclear medium and final-state interaction effects.

doi: 10.1103/PhysRevC.73.065502
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2006LE42      Phys.Rev.C 74, 065502 (2006)

T.Leitner, L.Alvarez-Ruso, U.Mosel

Neutral current neutrino-nucleus interactions at intermediate energies

NUCLEAR REACTIONS 1n, 1H(ν, ν'π0), E=0.2-2 GeV; 1H(ν, ν'π+), E=0.2-2 GeV; 1n(ν, ν'π-), E=0.2-2 GeV; calculated σ. 16O, 56Fe(ν, π0X), (ν, π+X), (ν, π-X), E=0.5-2 GeV; calculated pion production σ, σ(E); deduced in-medium modifications and final-state interaction effects.

doi: 10.1103/PhysRevC.74.065502
Citations: PlumX Metrics

2006MO16      Pramana 66, 709 (2006)


Hadrons in medium

doi: 10.1007/BF02704802
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2006MU01      Nucl.Phys. A765, 188 (2006)

P.Muhlich, U.Mosel

Attenuation of φ mesons in γA reactions

NUCLEAR REACTIONS 7Li, 12C, 27Al, 40Ca, 64Cu, 208Pb(γ, X), E ≈ 2 GeV; calculated φ production σ, mass-dependence and in-medium effects. Semi-classical transport approach, comparison with data.

doi: 10.1016/j.nuclphysa.2005.11.007
Citations: PlumX Metrics

2006MU12      Nucl.Phys. A773, 156 (2006)

P.Muhlich, U.Mosel

ω attenuation in nuclei

NUCLEAR REACTIONS 12C, 40Ca, 208Pb(γ, X), E=0.8-2.0 GeV; calculated ω production σ, mass-dependence and in-medium effects. Semi-classical transport approach, comparison with data.

doi: 10.1016/j.nuclphysa.2006.05.001
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2006MU16      Nucl.Phys. A780, 187 (2006)

P.Muehlich, V.Shklyar, S.Leupold, U.Mosel, M.Post

The spectral function of the ω meson in nuclear matter from a coupled-channel resonance model

doi: 10.1016/j.nuclphysa.2006.10.037
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2006SH03      Nucl.Phys. A764, 313 (2006)

R.Shyam, H.lenske, U.Mosel

A relativistic two-nucleon model for A(p, K+ΛB reaction

NUCLEAR REACTIONS 1H, 4He, 12C, 40Ca(p, K+), E=0.5-3.0 GeV; calculated hypernucleus production σ(E, θ), intermediate states contributions. Fully covariant two-nucleon model.

doi: 10.1016/j.nuclphysa.2005.09.015
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2005AL28      Prog.Part.Nucl.Phys. 55, 71 (2005)

L.Alvarez-Ruso, T.Falter, U.Mosel, P.Muehlich

In-medium properties of hadrons-observables II

doi: 10.1016/j.ppnp.2005.01.005
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2005KO19      Nucl.Phys. A756, 192 (2005)

P.Konrad, H.Lenske, U.Mosel

Short range correlations and spectral functions in asymmetric nuclear matter

doi: 10.1016/j.nuclphysa.2005.03.083
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2005LA20      Phys.Rev. C 72, 014901 (2005)

A.B.Larionov, U.Mosel

Kaon production and propagation at intermediate relativistic energies

NUCLEAR REACTIONS 197Au(197Au, K+X), E=0.96, 1.5 GeV/nucleon; C(C, K+X), E=2 GeV/nucleon; Ni(Ni, K+X), E=1.93 GeV/nucleon; calculated kaon production σ(E, θ), collective flow, related features. Transport model, comparison with data.

doi: 10.1103/PhysRevC.72.014901
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2005LI26      Prog.Part.Nucl.Phys. 55, 293 (2005)

O.Linnyk, S.Leupold, U.Mosel

Effect of quark off-shellness in DIS and the Drell-Yan process

NUCLEAR REACTIONS 1H(e, e'X), E=high; 1H(p, μ+μ-X), E=800 GeV; calculated Drell-Yan σ(E, θ), higher-twist corrections.

doi: 10.1016/j.ppnp.2005.01.006
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2005SH20      Phys.Rev. C 71, 055206 (2005); Erratum Phys.Rev. C 72, 019903 (2005)

V.Shklyar, H.Lenske, U.Mosel, G.Penner

Coupled-channel analysis of ω-meson production in πN and γN reactions for c.m. energies up to 2 GeV

NUCLEAR REACTIONS 1H(π-, X), (γ, X), E(cm) ≈ 1.7-2.1 GeV; analyzed ω-meson production σ, σ(θ); deduced resonance contributions. Coupled-channels effective Lagrangian approach.

doi: 10.1103/PhysRevC.71.055206
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2005SH30      Phys.Rev. C 72, 015210 (2005)

V.Shklyar, H.Lenske, U.Mosel

Coupled-channel analysis of KΛ production in the nucleon resonance region

NUCLEAR REACTIONS 1H(π-, K0X), (γ, K+X), E(cm) ≈ 1.6-2 GeV; analyzed hyperon production associated σ, σ(θ), polarization observables, related data; deduced final state resonance couplings. Unitary coupled-channels effective Lagrangian model.

doi: 10.1103/PhysRevC.72.015210
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2005WA08      Phys.Rev. C 71, 034910 (2005)

M.Wagner, A.B.Larionov, U.Mosel

Kaon and pion production in relativistic heavy-ion collisions

NUCLEAR REACTIONS 197Au(Si, X), (197Au, X), Pb(Pb, X), E=high; analyzed pion and kaon yields, transverse mass spectra; deduced reaction mechanism features. Transport model.

doi: 10.1103/PhysRevC.71.034910
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2004FA13      Prog.Part.Nucl.Phys. 53, 25 (2004)

T.Falter, J.Lehr, U.Mosel, P.Muehlich, M.Post

In-medium properties of hadrons -- observables

doi: 10.1016/j.ppnp.2004.02.012
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2004FA26      Phys.Lett. B 594, 61 (2004)

T.Falter, W.Cassing, K.Gallmeister, U.Mosel

Hadron formation and attenuation in deep inelastic lepton scattering off nuclei

NUCLEAR REACTIONS 14N, 84Kr, 131Xe(e, e'X), E=high; calculated charged hadron multiplicities. Comparisons with data.

doi: 10.1016/j.physletb.2004.04.089
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2004FA30      Phys.Rev. C 70, 054609 (2004)

T.Falter, W.Cassing, K.Gallmeister, U.Mosel

Hadron attenuation in deep inelastic lepton-nucleus scattering

NUCLEAR REACTIONS 14N, 20Ne, 63Cu, 84Kr, 131Xe(e, e'X), E=high; calculated hadron yields, multiplicity ratios, attenuation, related features; deduced role of final state interactions. Probabilistic coupled-channels transport model, comparison with data.

doi: 10.1103/PhysRevC.70.054609
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2004FA32      Fizika(Zagreb) B 13, 165 (2004)

Th.Falter, U.Mosel

Electroproduction of hadrons on nuclei at GeV energies

NUCLEAR REACTIONS 14N(e, e'X), E=high; calculated ρ0 production transparency ratio. 14N, 84Kr(e, e'X), E=high; calculated charged particles multiplicity ratios. Comparison with data.

2004KR16      Eur.Phys.J. A 22, 277 (2004)

B.Krusche, J.Lehr, J.Ahrens, J.R.M.Annand, R.Beck, F.Bloch, L.S.Fog, D.Hornidge, S.Janssen, M.Kotulla, J.C.McGeorge, I.J.D.MacGregor, J.Messchendorp, V.Metag, U.Mosel, R.Novotny, R.O.Owens, M.Pfeiffer, R.Sanderson, S.Schadmand, D.P.Watts

Photoproduction of π0-mesons from nuclei

NUCLEAR REACTIONS 12C, 40Ca, 93Nb, 208Pb(γ, π0X), E=200-800 MeV; measured missing-energy and missing-mass spectra, σ, σ(E, θ); deduced in-medium effects. Tagged photons, comparison with model predictions, previous results.

doi: 10.1140/epja/i2004-10033-9
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2004KR17      Eur.Phys.J. A 22, 347 (2004)

B.Krusche, J.Lehr, F.Bloch, M.Kotulla, V.Metag, U.Mosel, S.Schadmand

Surface and volume effects in the photoabsorption of nuclei

NUCLEAR REACTIONS 2H, C, Ca, Nb, Pb(γ, X), E=200-900 MeV; analyzed meson production σ; deduced surface and volume components, resonance effects.

doi: 10.1140/epja/i2004-10098-4
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2004LE08      Phys.Rev. C 69, 024603 (2004)

J.Lehr, U.Mosel

Influence of the nucleon spectral function in photon and electron induced reactions on nuclei

NUCLEAR REACTIONS 40Ca(γ, X), E=0.5-1 GeV; 40Ca(e, e'X), E=1.8-3.2 GeV; calculated η-meson production σ, medium effects. Transport model, comparison with data.

doi: 10.1103/PhysRevC.69.024603
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2004LI17      Eur.Phys.J. A 19, Supplement 1, 203 (2004)

O.Linnyk, S.Leupold, U.Mosel

Ground state correlations in deep inelastic scattering and the Drell-Yan process

doi: 10.1140/epjad/s2004-03-034-8
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2004MU15      Eur.Phys.J. A 20, 499 (2004)

P.Muhlich, T.Falter, U.Mosel

Inclusive ω photoproduction off nuclei

NUCLEAR REACTIONS 1H, 12C, 92Nb(γ, X), E=1.2, 2.5 GeV; calculated ω production σ, invariant mass spectra, in-medium effects.

doi: 10.1140/epja/i2003-10166-3
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2004MU17      Phys.Lett. B 595, 216 (2004)

P.Muhlich, L.Alvarez-Ruso, O.Buss, U.Mosel

Low-energy ππ photoproduction off nuclei

NUCLEAR REACTIONS 1H, 12C, 208Pb(γ, 2π0), (γ, π+π0), (γ, π-π0), E=400-460 MeV; calculated two-pion invariant mass distributions, final-state interaction effects. Semi-classical transport model, comparison with data.

doi: 10.1016/j.physletb.2004.05.054
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2004PO14      Nucl.Phys. A741, 81 (2004)

M.Post, S.Leupold, U.Mosel

Hadronic spectral functions in nuclear matter

doi: 10.1016/j.nuclphysa.2004.05.016
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2004SH23      Phys.Rev. C 69, 065205 (2004)

R.Shyam, H.Lenske, U.Mosel

Exclusive K+ production in proton-nucleus collisions

NUCLEAR REACTIONS 40Ca(p, K+), E=2.0 GeV; calculated hypernucleus production σ(E, θ), intermediate states contributions. Fully covariant two-nucleon model.

doi: 10.1103/PhysRevC.69.065205
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2004SH35      Eur.Phys.J. A 21, 445 (2004)

V.Shklyar, G.Penner, U.Mosel

Spin-5/2 resonance contributions to the pion-induced reactions for energies √ s ≤ 2.0 GeV

NUCLEAR REACTIONS 1H(π+, X), (π-, X), E(cm) ≈ 1.4-2 GeV; calculated kaon, meson, hyperon production σ, partial waves, resonance contributions. Coupled-channels effective Lagrangian model, comparison with data.

doi: 10.1140/epja/i2004-10003-3
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2003FA05      Phys.Rev. C 67, 054606 (2003); Erratum Phys.Rev. C 68, 019903 (2003)

T.Falter, K.Gallmeister, U.Mosel

Incoherent ρ0 electroproduction off nuclei

NUCLEAR REACTIONS 1H, 14N(e, X), E=high; calculated π0 production σ(E, θ). 14N, 84Kr(e, X), E=high; calculated π0 production nuclear transparency vs coherence length. Comparisons with data.

doi: 10.1103/PhysRevC.67.054606
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2003FR01      Phys.Rev. C 67, 015206 (2003)

F.Fromel, S.Leupold, U.Mosel

Spectral function of quarks in quark matter

doi: 10.1103/PhysRevC.67.015206
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2003FR16      Nucl.Phys. A723, 544 (2003)

F.Fromel, H.Lenske, U.Mosel

Short-range correlations in nuclear matter at finite temperatures and high densities

doi: 10.1016/S0375-9474(03)01364-2
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2003FR33      Eur.Phys.J. A 18, 265 (2003)

F.Fromel, S.Leupold, U.Mosel

Spectral functions of quarks in quark matter

doi: 10.1140/epja/i2002-10213-7
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2003LA19      Nucl.Phys. A728, 135 (2003)

A.B.Larionov, U.Mosel

The NN → NΔ cross section in nuclear matter

NUCLEAR REACTIONS 1H(p, nX), E=high; calculated Δ resonance production σ, medium corrections. 12C(12C, X), Ca(Ca, X), Ru(Ru, X), 197Au(197Au, X), E=high; calculated pion multiplicities, transverse momentum spectra. Comparisons with data.

doi: 10.1016/j.nuclphysa.2003.08.005
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2003LE22      Phys.Rev. C 68, 044601 (2003)

J.Lehr, M.Post, U.Mosel

In-medium modifications of the S11(1535) resonance and η photoproduction

NUCLEAR REACTIONS 1H, C, Al, Ca, Cu, Nb, Pb(γ, X), E ≈ 0.6-1 GeV; calculated η-meson production σ; deduced role of in-medium resonance modification. Transport model, comparison with data.

doi: 10.1103/PhysRevC.68.044601
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2003LE23      Phys.Rev. C 68, 044603 (2003)

J.Lehr, U.Mosel

η electroproduction on nuclei in the nucleon resonance region

NUCLEAR REACTIONS 40Ca(e, e'X), (e, e'π0X), E=3.2, 4 GeV; 40Ca(γ, X), E=0.6-1 GeV; calculated pion and η meson production σ, final state interaction effects. Transport model.

doi: 10.1103/PhysRevC.68.044603
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2003MA82      Eur.Phys.J. A 18, 223 (2003)

G.Martens, C.Greiner, S.Leupold, U.Mosel

Chromofields of strings and baryons

doi: 10.1140/epja/i2002-10303-6
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2003MU04      Phys.Rev. C 67, 024605 (2003)

P.Muhlich, T.Falter, C.Greiner, J.Lehr, M.Post, U.Mosel

Photoproduction of φ mesons from nuclei

NUCLEAR REACTIONS 1H(γ, X), E=2-6 GeV; calculated φ meson production σ, σ(θ). 40Ca(γ, K+K-X), E=2.4 GeV; calculated φ meson production associated σ, kaon pair invariant mass spectra, final state interaction and other medium effects. Semiclassical transport model.

doi: 10.1103/PhysRevC.67.024605
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2003SH16      Phys.Rev. C 67, 065202 (2003)

R.Shyam, U.Mosel

Role of baryonic resonances in the dilepton emission in nucleon-nucleon collisions

NUCLEAR REACTIONS 1n, 1H(p, X), E=1.04-4.88 GeV; calculated dilepton invariant mass distributions, total dilepton production σ. Effective Lagrangian model, comparisons with data.

doi: 10.1103/PhysRevC.67.065202
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2002FA08      Phys.Rev. C66, 024608 (2002)

T.Falter, U.Mosel

Hadron formation in high energy photonuclear reactions

NUCLEAR REACTIONS 208Pb(γ, π+π-X), E=7 GeV; calculated ρ meson production associated mass spectra, σ(θ). 208Pb(γ, K+X), E=1-7 GeV; calculated production σ. Realistic treatment of final state interactions.

doi: 10.1103/PhysRevC.66.024608
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2002LA21      Phys.Rev. C66, 034902 (2002)

A.B.Larionov, U.Mosel

Off-Shell Pions in Boltzmann-Uehling-Uhlenbeck Transport Theory

NUCLEAR REACTIONS 197Au(197Au, X), E=1.06 GeV/nucleon; calculated pion mass spectra vs time, transverse momentum spectra, contributions from off-shell pions. Δ-hole model.

doi: 10.1103/PhysRevC.66.034902
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2002LA32      Phys.Rev. C 66, 054604 (2002)

A.B.Larionov, M.Effenberger, S.Leupold, U.Mosel

Resonance lifetime in Boltzmann-Uehling-Uhlenbeck theory: Observable consequences

NUCLEAR REACTIONS C, Fe(π+, X), E ≈ 70-320 MeV; calculated absorption σ, dependence on resonance lifetime. 197Au(197Au, X), E=1 GeV/nucleon; calculated pion transverse momentum, invariant mass spectra, dependence on resonance lifetime. Transport model, comparisons with data.

doi: 10.1103/PhysRevC.66.054604
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2002LE06      Nucl.Phys. A699, 324c (2002)

J.Lehr, U.Mosel

Photon and Electron Induced Particle Production on Nuclei

doi: 10.1016/S0375-9474(01)01512-3
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2002LE14      Nucl.Phys. A703, 393 (2002)

J.Lehr, H.Lenske, S.Leupold, U.Mosel

Nuclear Matter Spectral Functions by Transport Theory

doi: 10.1016/S0375-9474(01)01534-2
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2002PE07      Phys.Rev. C65, 055202 (2002); Erratum Phys.Rev. C65, 059901 (2002)

G.Penner, U.Mosel

πN → ωN in a Coupled-Channel Approach

NUCLEAR REACTIONS 1H(π-, nX), E(cm)=1.7-2.0 GeV; calculated ω meson production σ; deduced role of rescattering and resonance excitations, partial wave contributions. Coupled-channels approach, comparisons with data.

doi: 10.1103/PhysRevC.65.055202
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2002PE20      Phys.Rev. C 66, 055211 (2002)

G.Penner, U.Mosel

Vector meson production and nucleon resonance analysis in a coupled-channel approach for energies mN<√s<2 GeV. I. Pion-induced results and hadronic parameters

NUCLEAR REACTIONS 1H(π+, X), (π-, X), E(cm) < 2 GeV; analyzed pion, kaon, η, and ω production σ(θ); deduced nucleon resonance features.

doi: 10.1103/PhysRevC.66.055211
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2002PE21      Phys.Rev. C 66, 055212 (2002)

G.Penner, U.Mosel

Vector meson production and nucleon resonance analysis in a coupled-channel approach for energies mN<√s<2 GeV. II. Photon-induced results

NUCLEAR REACTIONS 1H(γ, X), E(cm) < 2 GeV; analyzed pion, kaon, η, and ω production σ(θ); deduced nucleon resonance features.

doi: 10.1103/PhysRevC.66.055212
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2002PO01      Nucl.Phys. A699, 169c (2002)

M.Post, U.Mosel

Vector Mesons and Baryon Resonances in Nuclear Matter

doi: 10.1016/S0375-9474(01)01489-0
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2001BR04      Nucl.Phys. A681, 84c (2001)

E.L.Bratkovskaya, W.Cassing, C.Greiner, M.Effenberger, U.Mosel, A.Sibirtsev

Thermal and Chemical Equilibration of Hadronic Matter

doi: 10.1016/S0375-9474(00)00486-3
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2001BR13      Nucl.Phys. A686, 568 (2001)

E.L.Bratkovskaya, W.Cassing, U.Mosel

Perspectives of e+e- Production in pp, pd and pBe Reactions at SIS Energies

NUCLEAR REACTIONS 1,2H, Be(p, X), E=1-4.9 GeV; calculated dilepton invariant mass spectra, transverse momentum and rapidity distributions; deduced reaction mechanism features. Resonance-string approach, comparisons with data.

doi: 10.1016/S0375-9474(00)00557-1
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2001FA14      Phys.Rev. C64, 024608 (2001)

T.Falter, S.Leupold, U.Mosel

Nuclear Shadowing at Low Photon Energies

NUCLEAR REACTIONS C, 27Al, Cu, Sn, Pb(γ, X), E=1-3 GeV; calculated relative photoabsorption σ, nuclear shadowing effects. Multiple scattering approach, comparison with data.

doi: 10.1103/PhysRevC.64.024608
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2001KE07      Phys.Rev. C63, 045202 (2001)

M.Th.Keil, G.Penner, U.Mosel

Anti-Kaon Induced Reactions on the Nucleon

NUCLEAR REACTIONS 1H(K-, K-), (K-, K0), (K-, π+X), (K-, π0X), (K-, π-X), E(cm) ≈ 1.4-1.8 GeV; calculated σ, σ(θ). Comparisons with data.

doi: 10.1103/PhysRevC.63.045202
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2001LA29      Nucl.Phys. A696, 747 (2001)

A.B.Larionov, W.Cassing, S.Leupold, U.Mosel

Quenching of Resonance Production in Heavy-Ion Collisions at 1-2 A GeV

NUCLEAR REACTIONS 197Au(197Au, X), E=1 GeV/nucleon; Ni(Ni, X), E=1-2 GeV/nucleon; C(C, X), E=0.8-2 GeV/nucleon; calculated pion multiplicities, transverse momentum spectra, angular distributions; deduced in-medium quenching of resonance production. Transport model, comparisons with data.

doi: 10.1016/S0375-9474(01)01216-7
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2001LE33      Phys.Rev. C64, 042202 (2001)

J.Lehr, U.Mosel

In-Medium Broadening of Nucleon Resonances

NUCLEAR REACTIONS 40Ca(γ, π0X), E=0.4-0.9 GeV; calculated pion production σ; deduced role of in-medium nucleon resonance broadening. Comparisons with data.

doi: 10.1103/PhysRevC.64.042202
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2001PO12      Nucl.Phys. A688, 808 (2001)

M.Post, U.Mosel

Coupling of Baryon Resonances to the Nω Channel

NUCLEAR REACTIONS 1H(γ, X), (π-, X), E ≈ 1.1-2 GeV; calculated total σ. Baryon resonance coupling. Comparison with data.

doi: 10.1016/S0375-9474(00)00583-2
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2001PO14      Nucl.Phys. A689, 753 (2001)

M.Post, S.Leupold, U.Mosel

The ρ Spectral Function in a Relativistic Resonance Model

doi: 10.1016/S0375-9474(00)00613-8
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