0000000000289176

AUTHOR

W. Trautmann

showing 21 related works from this author

ASY-EOS experiment at GSI

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich Heavy-Ion at intermediate energies has been recently proposed as an observable sensitive to the strength of the symmetry term in the nuclear equation of state (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for 197Au+197Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI laboratory b…

PhysicssezelePhysicsQC1-999Nuclear Theorysymmetry energyObservableNuclear equation of state[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nuclear equation of stateSymmetry (physics)Term (time)Nuclear physicsPhysics and Astronomy (all)nucleus-nucleus collisionsNeutronNucleonNuclear ExperimentEPJ Web of Conferences
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Onset of nuclear vaporization inAu197+197Au collisions

1993

Multifragmentation has been measured for [sup 197]Au+[sup 197]Au collisions at [ital E]/[ital A]=100, 250, and 400 MeV. The mean fragment multiplicity increases monotonically with the charged particle multiplicity at [ital E]/[ital A]=100 MeV, but decreases for central collisions with incident energy, consistent with the onset of nuclear vaporization. Molecular dynamics calculations follow some trends but underpredict the observed fragment multiplicities. Including the statistical decay of excited residues improves the agreement for peripheral collisions but worsens it for central collisions.

PhysicsNuclear physicsNuclear reactionComputer Science::Information RetrievalExcited stateVaporizationGeneral Physics and AstronomyIncident energyMultiplicity (mathematics)Nuclear ExperimentCharged particlePhysical Review Letters
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Fragment Flow and the Multifragmentation Phase Space

1995

Fragment distributions have been measured for Au+Au collisions at [ital E]/[ital A]=100 and 1000 MeV. A high detection efficiency for fragments was obtained by combining the ALADIN spectrometer and the MSU-Miniball/WU-Miniwall array. At both energies the maximum multiplicity of intermediate mass fragments (IMF) normalized to the size of the decaying system is about one IMF per 30 nucleons but the element distributions show significant differences. Within a coalescence picture the suppression of heavy fragments in central collisions at [ital E]/[ital A]=100 MeV may be related to a reduction of the density in momentum space which is caused by the collective expansion.

Nuclear reactionCoalescence (physics)PhysicsSpectrometer[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Computer Science::Information RetrievalGeneral Physics and AstronomyPosition and momentum space[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Space (mathematics)Nuclear physicsPhase spaceMultiplicity (chemistry)Atomic physicsNuclear ExperimentNucleonPhysical Review Letters
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Scintillating fiber detectors for the HypHI project at GSI

2009

WOS: 000270326800009

PhysicsNuclear and High Energy PhysicsHydrogenProjectileDetectorPhase (waves)chemistry.chemical_elementTracking (particle physics)Charged particleHypernuclear spectroscopyNuclear physicsTracking detectorschemistryScintillating fiber detectorsDeposition (phase transition)InstrumentationImage resolution
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Light Charged Particle Identification by Means of Digital Pulse Shape Acquisition in the CHIMERACsI(Tl) Detectors at GSI Energies

2011

We report the results obtained by applying digital pulse shape acquisition and digital signal processing to the signals from CsI(Tl) scintillators read out by photodiodes at high incident energy (400 MeV/u). The digitized signals allows the discrimination of light charged particles by computing the Fast and Slow components and the Rise Time of the output pulses of the CsI(Tl). When the energies of the light charged particles exceed those corresponding to their ranges in CsI(Tl), the points related to the punching-through particles gather in the corresponding scatter plots giving rise to a cusp. The punching-through points are used as energy calibration points for the reaction products stopp…

PhysicsRadiology Nuclear Medicine and ImagingRadiationsezelePhysics::Instrumentation and Detectorsbusiness.industryDetectorScintillatorRadiationCharged particlePhotodiodelaw.inventionOpticslawRise timebusinessBeam (structure)Digital signal processingNuclear and High Energy Physic
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The HypHI Phase 0 experiment

2010

10th International Conference on Hypernuclear and Strange Particle Physics -- SEP 14-18, 2009 -- Tokai, JAPAN

PhysicsNuclear and High Energy PhysicsCarbon graphiteProjectilehypernuclear spectroscopyPhase (waves)LambdaNuclear physicsheavy ion induced reactioninvariant massHeavy ionENERGY NUCLEAR COLLISIONSAtomic physicsSpectroscopyNuclear Physics A
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Probing the Merits of Different Event Parameters for the Identification of Light Charged Particles in CHIMERA CsI(Tl Detectors With Digital Pulse Sha…

2013

We investigated the merits of different event parameters in the identification of Light Charged Particles (LCPs) with CsI(Tl) scintillators read out by photodiodes at high incident energy (400 MeV/u). This investigation is made possible by digital signal processing the output signals. As in the conventional analogue case, the digitized signals allow the discrimination of light charged particles by computing the fast and slow components. In addition other identification parameters as the rise time of the output pulses of the CsI(Tl) come out nearly for free. Aim of this paper is the investigation of novel identification plots and the probe of their merits, in particular at relativistic energ…

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectorsintermediate energy nuclear physicpulse shape analysiScintillatorParticle identificationlaw.inventionOpticslawElectrical and Electronic EngineeringDigital signal processingPhysicsonline digital signal processingSignal processingsezeleCsI(Tl) scintillatorsbusiness.industrypulse shape analysisDetectorCsI(Tl) scintillatorCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysisCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysis; Electrical and Electronic Engineering; Nuclear Energy and Engineering; Nuclear and High Energy PhysicsCharged particlePhotodiodeintermediate energy nuclear physicsNuclear Energy and EngineeringRise timeparticle identificationbusinessnuclear physics; heavy-ions; digital signal processing; scintillation detectors
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Hypernuclear production cross section in the reaction of 6Li + 12C at 2 A GeV

2015

WOS: 000358624800021

Particle physicsNuclear and High Energy PhysicsPopulationH-4(LAMBDA)BEAMLIFETIMEStrangenessHEAVY-ION COLLISIONSLambdaParticle identificationNuclear physicsHypernucleiInvariant massRapidityeducationNuclear ExperimentPhysicseducation.field_of_studyHeavy ion collisionHyperonRelativistic energyHypernucleuslcsh:QC1-999STATEProduction cross sectionQUANTUM MOLECULAR-DYNAMICSLIGHT HYPERNUCLEIYield ratioDECAYlcsh:PhysicsRELATIVISTIC HYPERNUCLEIPhysics Letters B
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Hypernuclear spectroscopy of products from Li-6 projectiles on a carbon target at 2 A GeV

2013

WOS: 000322848900009

Nuclear reaction(Li-6E=2 GeV/nucleonNuclear and High Energy PhysicsMaximum likelihoodWEAK DECAYFOS: Physical sciencesLIFETIMET-1/2. Compared with other datadeduced Lambda massC-12(LAMBDA)H-4)T-1/2measured Lambda H-3H-4 Lambda-hypernuclei invariant mass distribution T-1/2measured LambdaInvariant massNuclear Experiment (nucl-ex)LIGHT HYPERFRAGMENTSSpectroscopyNuclear ExperimentX)PhysicsH-4 Lambda-hypernuclei invariant mass distributionH-3ProjectileSignificance valueslifetime measurementdeduced Lambda mass H-3H-4 Lambda-hypernuclei mass T-1/2. Compared with other data lifetime measurementNUCLEAR REACTIONS C(Li-6Decay timeLAMBDA-HYPERNUCLEIAtomic physicst)NUCLEAR REACTIONS C(Li-6 X) (Li-6 t) (Li-6 H-4) E=2 GeV/nucleonH-4 Lambda-hypernuclei massHypertritonRELATIVISTIC HYPERNUCLEINuclear Physics A
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Present status of the caloric curve of nuclei

1998

Abstract Spectator decay was studied for the system Au + Au at an energy of 1000 A·MeV and the decay of the interaction region at energies between 50 and 200 A·MeV. In both cases temperatures were derived from several double-ratios of neighboring isotopes and from the population of excited states in 5 Li and 4 He. Agreement was found among the different isotope temperatures and also among the two excited state temperatures. The comparison of isotope and excited state temperatures, however, reveals large differences, which cannot be explained by feeding corrections. At incident energies between 600 and 1000 A·MeV the energy spectra of fragments and also neutrons of the decaying projectile sp…

PhysicsNuclear and High Energy Physicseducation.field_of_studyIsotopeProjectileNuclear TheoryPopulationSpectral lineCaloric curveExcited stateIncident energyNeutronAtomic physicsNuclear ExperimenteducationNuclear Physics A
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Production of hypernuclei in peripheral HI collisions: The HypHI project at GSI

2012

ECT Workshop on Strange Hadronic Matter -- SEP 26-30, 2011 -- Trento, ITALY

PhysicsNuclear and High Energy PhysicsPhase (waves)chemistry.chemical_elementInvariant massLIFETIMEHeavy ion induced reactionHypernuclear spectroscopyNuclear physicschemistryMass spectrumLithiumHeavy ionInvariant massENERGY NUCLEAR COLLISIONSAtomic physicsSpectroscopyRELATIVISTIC HYPERNUCLEI
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The HypHI project: Hypernuclear spectroscopy with stable heavy ion beams and rare isotope beams at GSI and FAIR

2009

The HypHI collaboration aims to perform a precise hypernuclear spectroscopy with stable heavy ion beams and rare isotope beams at GSI and fAIR in order to study hypernuclei at extreme isospin, especially neutron rich hypernuclei to look insight hyperon-nucleon interactions in the neutron rich medium, and hypernuclear magnetic moments to investigate baryon properties in the nuclei. We are currently preparing for the first experiment with $^6$Li and $^{12}$C beams at 2 AGeV to demonstrate the feasibility of a precise hypernuclear spectroscopy by identifying $^{3}_{\Lambda}$H, $^{4}_{\Lambda}$H and $^{5}_{\Lambda}$He. The first physics experiment on these hypernuclei is planned for 2009. In th…

PhysicsNuclear and High Energy PhysicsIsotopeMagnetic momentNuclear TheoryGeneral Physics and AstronomyOrder (ring theory)FOS: Physical sciencesLambdaBaryonNuclear physicsIsospinNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentSpectroscopyNuclear Experiment
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Study of the Unstable NucleusL10iin Stripping Reactions of the Radioactive ProjectilesB11eandL11i

1995

Reactions of the halo systems Be-11 and Li-11 (at 460 and 280 MeV/nucleon) with a carbon target demonstrate that (n + Li-9) has an (unbound) l = 0 ground state very close to the threshold. The neutron halo of Li-11 has appreciable (1s(1/2))(2) and (0p(1/2))(2) components.

PhysicsStripping (chemistry)ProjectileAnalytical chemistryGeneral Physics and Astronomychemistry.chemical_elementmedicine.anatomical_structurechemistrymedicineNeutronHaloAtomic physicsNucleonGround stateNucleusCarbonPhysical Review Letters
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Event reconstruction methods for the HypHI Phase 0 experiment at GSI

2010

WOS: 000282530300034

PhysicsNuclear and High Energy PhysicsEvent reconstructionPhase (waves)Kalman filterHypHICollisionHough transformlaw.inventionHypernuclear spectroscopyNuclear physicsHough transformlawHeavy ionKalman filterSpectroscopyInstrumentationEvent reconstruction
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The percolation phase transition and statistical multifragmentation in finite systems

2020

The cumulant ratios up to fourth order of the $Z$ distributions of the largest fragment in spectator fragmentation following $^{107,124}$Sn+Sn and $^{124}$La+Sn collisions at 600 MeV/nucleon have been investigated. They are found to exhibit the signatures of a second-order phase transition established with cubic bond percolation and previously observed in the ALADIN experimental data for fragmentation of $^{197}$Au projectiles at similar energies. The deduced pseudocritical points are found to be only weakly dependent on the $A/Z$ ratio of the fragmenting spectator source. The same holds for the corresponding chemical freeze-out temperatures of close to 6 MeV. The experimental cumulant dist…

Nuclear and High Energy PhysicsPhase transitionheavy ion collisionsNuclear TheoryFOS: Physical sciences53001 natural sciencesHeat capacitypercolation theoryNuclear physicsstatistical multifragmentation modelsPercolation theory0103 physical sciencesHeavy ion collisionsddc:530Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsObservableStatistical modelPercolation theorylcsh:QC1-999SkewnessStatistical multifragmentation modelsKurtosisNucleonlcsh:Physics
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Hypernuclear spectroscopy with heavy ion beams: The HypHI project at GSI and fair

2010

The HypHI experiment for precise hypernuclear spectroscopy with induced reactions of stable heavy ion beams and rare isotope beams is currently under preparation at GSI. The main goal of the HypHI project is to study neutron and proton rich hypernuclei and to measure directly hypernuclear magnetic moments at GSI and FAIR. In the first HypHI experiment (Phase 0) planned in 2009, the feasibility of precise hypernuclear spectroscopy with heavy ion beams will be demonstrated by observing π- decay channels of [Formula: see text], [Formula: see text] and [Formula: see text] with 6 Li projectiles at 2 A GeV impinging on a 12 C target. An overview of the HypHI project and the details of the Phase …

PhysicsNuclear and High Energy PhysicsRI-beamsProtonNuclear TheoryGeneral Physics and AstronomyHypernuclear spectroscopyNuclear physicsmagnetic momentsexotic hypernucleiPhysics::Accelerator PhysicsHeavy ionNeutronheavy ion beamsENERGY NUCLEAR COLLISIONSSpectroscopyNuclear Experiment
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Electromagnetic fission of $^{238}$U at 600 and 1000 MeV per nucleon

1995

Electromagnetic fission of238U projectiles at E/A =600 and 1000 MeV was studied with the ALADIN spectrometer at the heavy-ion synchrotron SIS. Seven different targets (Be, C, Al, Cu, In, Au and U) were used. By considering only those fission events where the two charges added up to 92, most of the nuclear interactions were excluded. The nuclear contributions to the measured fission cross sections were determined by extrapolating from beryllium to the heavier targets with the concept of factorization. The obtained cross sections for electromagnetic fission are well reproduced by extended Weizsacker-Williams calculations which include E1 and E2 excitations. The asymmetry of the fission fragme…

PhysicsNuclear and High Energy PhysicsCold fissionCluster decayFissionNuclear Theorychemistry.chemical_elementUraniumResonance (particle physics)Nuclear physicschemistryNuclear fusionAtomic physicsBerylliumNuclear ExperimentNucleonNuclear Physics
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Longitudinal and transverse momentum distributions of 9Li fragments from break-up of 11Li

1995

7 pages, 3 figures, 1 table.

PhysicsNuclear and High Energy PhysicsTransverse planeFull width at half maximumMomentum (technical analysis)Break-UpSignificant differenceTransverse momentumSigmaHaloAtomic physicsNuclear Physics
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The ASY-EOS experiment at GSI: Investigating the symmetry energy at supra-saturation densities

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich heavy-ions systems at intermediate energies has been proposed as an observable sensitive to the strength of the symmetry term in the nuclear Equation Of State (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for $^{197}$Au+$^{197}$Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI la…

Particle physicsHistoryQC1-999Nuclear TheoryFOS: Physical sciencesand isobaric spin 24.10.Pa Thermal and statistical models[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]EducationNuclear physicsPhysics and Astronomy (all)nuclear physics; heavy-ions; symmetry energy; Au+Au collisionsNeutronNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentComputingMilieux_MISCELLANEOUSPhysicssezelePhysicsOrder (ring theory)Nuclear equation of stateObservableNuclear Experiment; Nuclear Experiment21.65.-f Nuclear matter 27.80.+w 190(less-than-or-equal-to)A(less-than-or-equal-to)219 24.60.-k Statistical theory and fluctuations 25.75.Gz Particle correlations and fluctuations 21.10.Hw SpinSymmetry (physics)Term (time)Computer Science ApplicationsparityNuclear reactionsSaturation (chemistry)NucleonEnergy (signal processing)
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Dissociation of 8He into 6He + n + X at 240 MeV/u

1995

4 pages, 3 figures, 2 tables.

PhysicsNuclear and High Energy PhysicsPhysical chemistryDissociation (chemistry)
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"Table 1" of "Electromagnetic fission of U-238 at 600-MeV and 1000-MeV per nucleon"

1997

Electromagnetic fission.

Nuclear TheoryIntegrated Cross SectionU238 U --> 2FRAGB XU238 C --> 2FRAGB XU238 AU --> 2FRAGB XCross SectionPhysics::Classical PhysicsSIGU238 AL --> 2FRAGB XU238 IN --> 2FRAGB XInclusiveU238 CU --> 2FRAGB XPhysics::Atomic and Molecular ClustersNUCLEUS NUCLEUS --> 2FRAGB XNuclear Experiment
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