A. Schüttauf
GSI Helmholtz Centre for Heavy Ion Research
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Featured researches published by A. Schüttauf.
Nuclear Physics | 1996
A. Schüttauf; W. D. Kunze; A. Wörner; M. Begemann-Blaich; Th. Blaich; D. R. Bowman; R. J. Charity; A. Cosmo; A. Ferrero; C. K. Gelbke; C. Groß; W. C. Hsi; J. Hubele; G. Imme; I. Iori; J. Kempter; P. Kreutz; G. J. Kunde; Volker Lindenstruth; M. A. Lisa; W. G. Lynch; U. Lynen; M. Mang; T. Möhlenkamp; A. Moroni; W. F. J. Müller; M. Neumann; B. Ocker; C.A. Ogilvie; Graham F. Peaslee
Abstract Multi-fragment decays of 129Xe, 197Au and 238U projectiles in collisions with Be, C, Al, Cu, In, Au and U targets at energies between E A = 400 and 1000 MeV have been studied with the ALADIN forward-spectrometer at SIS. By adding an array of 84 SiCsI(Tl) telescopes the solid-angle coverage of the setup was extended to θlab = 16°. This permitted the complete detection of fragments from the projectile-spectator source. The dominant feature of the systematic set of data is the Zbound universality that is obeyed by the fragment multiplicities and correlations. These observables are invariant with respect to the entrance channel if plotted as a function of Zbound, where Zbound is the sum of the atomic numbers Zi of all projectile fragments with Zi ⩾ 2. No significant dependence on the bombarding energy nor on the target mass is observed. The dependence of the fragment multiplicity on the projectile mass follows a linear scaling law. The reasons for and the limits of the observed universality of spectator fragmentation are explored within the realm of the available data and with model studies. It is found that the universal properties should persist up to much higher bombarding energies than explored in this work and that they are consistent with universal features exhibited by the intranuclear cascade and statistical multifragmentation models.
Nuclear Physics | 1995
A.S. Botvina; Igor Mishustin; M. Begemann-Blaich; J. Hubele; G. Imme; I. Iori; P. Kreutz; G. J. Kunde; W. D. Kunze; Volker Lindenstruth; U. Lynen; A. Moroni; W. F. J. Müller; C.A. Ogilvie; J. Pochodzalla; G. Raciti; Th. Rubehn; H. Sann; A. Schüttauf; W. Seidel; W. Trautmann; A. Wörner
Abstract Using the ALADIN forward-spectrometer at SIS we have studied multi-fragment decays of 197 Au projectiles after collisions with C, Al, Cu and Pb targets at a bombarding energy of E A = 600 MeV . The new data presented in this work comprise the measured cross sections of multifragment processes, the N Z ratios of the produced fragments, and the differential distributions of fragment multiplicities and of observables built on the charge correlations within the event. The 197 Au+Cu data are analyzed with the statistical multifragmentation model. It is shown that all observables can be simultaneously reproduced on an absolute scale, apart from an overall normalization constant which relates the number of model events to the measured cross section. A continuous distribution of excited residual nuclei, used as input for the calculations, was derived from the criterion of a best fit to the data. It exhibits a correlation between decreasing mass number A and increasing excitation energy E x A and a saturation of the excitation energy at E x A ≈ 8 MeV .
Nuclear Physics | 2010
W. Reisdorf; A. Andronic; Ralf Peter Averbeck; M. L. Benabderrahmane; O. N. Hartmann; N. Herrmann; K. D. Hildenbrand; T. I. Kang; Y. J. Kim; M. Kiš; P. Koczon; T. Kress; Y. Leifels; M. Merschmeyer; K. Piasecki; A. Schüttauf; M. R. Stockmeier; V. Barret; Z. Basrak; N. Bastid; R. Čaplar; P. Crochet; P. Dupieux; M. Dželalija; Z. Fodor; P. Gasik; Y. Grishkin; B. Hong; J. Kecskemeti; M. Kirejczyk
Using the large acceptance apparatus FOPI, we study central collisions in the reactions (energies in A GeV are given in parentheses): Ca-40 + Ca-40 (0.4, 0.6, 0.8, 1.0, 1.5, 1.93), Ni-58 + Ni-58 (0.15, 0.25, 0.4), Ru-96+Ru-96 (0.4, 1.0. 1.5), (96)zr+(96)zr 1.0, 1.5), Xe-129+CsI (0.15, 0.25, 0.4), Au-197 + Au-197 (0.09, 0.12, 0.15, 0.25, 0.4, 0.6, 0.8, 1.0, 1.2, 1.5). The observables include cluster multiplicities, longitudinal and transverse rapidity distributions and stopping, and radial flow. The data are compared to earlier data where possible and to transport model simulations
Nuclear Physics | 1993
P. Kreutz; J.C. Adioff; M. Begemann-Blaich; P. Bouissou; J. Hubele; G. Imme; I. Iori; G. J. Kunde; S. Leray; Volker Lindenstruth; Zhi Liu; U. Lynen; R.J. Meijer; U. Milkau; A. Moroni; W. F. J. Müller; C. Ngo; C.A. Ogilvie; J. Pochodzalla; G. Raciti; G. Rudolf; H. Sann; A. Schüttauf; W. Seidel; L. Stuttge; W. Trautmann; A. Tucholski
Abstract We have studied multi-fragment decays of Au projectiles after collisions with C, Al, Cu and Pb targets at a bombarding energy of 600 MeV/nucleon. We examine the correlations between the charges emitted in these reactions. These correlations are given as a function of the total charge in bound fragments, Z bound , at forward angles, which is a measure of the violence of the collision and can be related to the impact parameter. The charge distributions have been fitted by a power law and the extracted τ parameter exhibits a minimum as a function of Z bound . We observe a strong reduction in the maximum charge, Z max , of the event with decreasing Z bound . For those events where Z max is less than half Z bound , the relative sizes of the two largest charges within the event cover the full spectrum of possibilities. The charge-Dalitz plots indicate that the multi-fragmentation events are not an extension of symmetric fission reactions. The event-by-event charge moments are examined to measure the size of the charge fluctuations. All of the charge correlations are independent of the target when plotted as a function of Z bound . The results are compared to both nuclear statistical and percolation calculations. The model predictions differ from each other, establishing that the observables are sensitive to how the available phase space is populated. The sequential nuclear model predicts too asymmetric a decay, while the simultaneous model predicts too symmetric a break-up. The percolation model, which was adjusted to reproduce the size of Z max , correctly predicts the mean behaviour and the fluctuations of the lighter fragments.
Physical Review C | 2003
A. Andronic; W. Reisdorf; N. Herrmann; P. Crochet; J. P. Alard; V. Barret; Z. Basrak; N. Bastid; G. Berek; R. Čaplar; A. Devismes; P. Dupieux; M. Dželalija; C. Finck; Z. Fodor; A. Gobbi; Y. Grishkin; O. N. Hartmann; K. D. Hildenbrand; B. Hong; J. Kecskemeti; Y. J. Kim; M. Kirejczyk; P. Koczon; M. Korolija; R. Kotte; T. Kress; A. Lebedev; Y. Leifels; X. Lopez
We present new experimental data on directed flow in collisions of Au+Au, Xe+CsI and Ni+Ni at incident energies from 90 to 400A MeV. We study the centrality and system dependence of integral and differential directed flow for particles selected according to charge. All the features of the experimental data are compared with Isospin Quantum Molecular Dynamics (IQMD) model calculations in an attempt to extract information about the nuclear matter equation of state (EoS). We show that the combination of rapidity and transverse momentum analysis of directed flow allow to disentangle various parametrizations in the model. At 400A MeV, a soft EoS with momentum dependent interactions is best suited to explain the experimental data in Au+Au and Xe+CsI, but in case of Ni+Ni the model underpredicts flow for any EoS. At 90A MeV incident beam energy, none of the IQMD parametrizations studied here is able to consistently explain the experimental data.
European Physical Journal A | 1991
J. Hubele; P. Kreutz; J. C. Adloff; M. L. Begemann-Blaich; P. Bouissou; G. Imme; I. Iori; G. J. Kunde; S. Leray; Volker Lindenstruth; Z. Liu; U. Lynen; R. J. Meijer; U. Milkau; A. Moroni; W. F. J. Müller; C. Ngô; C. A. Ogilvie; J. Pochodzalla; G. Raciti; G. Rudolf; H. Sann; A. Schüttauf; W. Seidel; L. Stuttge; W. Trautmann; A. Tucholski
We have studied the fragmentation of Au projectiles interacting with targets of C, Al and Cu at an incident energy ofE/A=600 MeV. The employed inverse kinematics allowed a nearly complete detection of projectile fragments with chargeZ≧2. The recorded fragmentation events were sorted according to three observables, the multiplicityMlp of light charged particles, the largest atomic numberZmax within an event, and a new observable,Zbound, representing the sum of the atomic numbersZ of all fragments withZ≧2. Using these observables, the impact parameter dependence of the fragmentation process was investigated. For all three targets, a maximum mean multiplicity of 3 to 4 intermediate mass fragments (IMFs) is observed. The corresponding impact parameters range from central collisions for theC target to increasingly peripheral collisions for the heavier targets. It is found that the correlation between the IMF multiplicity andZbound, extending from evaporation type processes (largeZbound) to the total disassembly of the projectile (smallZbound), is independent of the target nucleus. This universal behaviour may suggest an — at least partial — equilibration of the projectile fragment prior to its decay.
Physical Review Letters | 2009
M. L. Benabderrahmane; N. Herrmann; K. Wiśniewski; J. Kecskemeti; A. Andronic; V. Barret; Z. Basrak; N. Bastid; P. Buehler; M. Cargnelli; R. Čaplar; E. Cordier; I. M. Deppner; P. Crochet; P. Dupieux; M. Dželalija; L. Fabbietti; Z. Fodor; P. Gasik; I. Gašparić; Y. Grishkin; O. N. Hartmann; K. D. Hildenbrand; B. Hong; T. I. Kang; P. Kienle; M. Kirejczyk; Y. J. Kim; M. Kiš; P. Koczon
The K0 meson production by pi(-) mesons of 1.15 GeV/c momentum on C, Al, Cu, Sn, and Pb nuclear targets was measured with the FOPI spectrometer at the Schwer-Ionen-Synchrotron accelerator of GSI. Inclusive production cross sections and the momentum distributions of K0 mesons are compared to scaled elementary production cross sections and to predictions of theoretical models describing the in-medium production of kaons. The data represent a new reference for those models, which are widely used for interpretation of the strangeness production in heavy-ion collisions. The presented results demonstrate the sensitivity of the kaon production to the reaction amplitudes inside nuclei and point to the existence of a repulsive KN potential of 20+/-5 MeV at normal nuclear matter density.
Physical Review C | 2007
M. Merschmeyer; X. Lopez; N. Bastid; P. Crochet; N. Herrmann; A. Andronic; V. Barret; Z. Basrak; M. L. Benabderrahmane; R. Čaplar; E. Cordier; P. Dupieux; M. Dželalija; Z. Fodor; I. Gašparić; Y. Grishkin; O. N. Hartmann; K. D. Hildenbrand; B. Hong; T. I. Kang; J. Kecskemeti; Y. J. Kim; M. Kirejczyk; M. Kiš; T. Matulewicz; P. Koczon; M. Korolija; R. Kotte; A. Lebedev; Y. Leifels
New results concerning the production of neutral strange particles, K{sup 0} and {lambda} in Ni+Ni collisions at 1.93A GeV, measured with the FOPI detector at GSI Darmstadt, are presented. Rapidity density distributions and Boltzmann slope parameter distributions are measured in nearly the full phase space of the reaction. The observables are compared to existing K{sup +} and proton data. While the K{sup 0} data agree with previously reported K{sup +} measurements, the {lambda} distributions show a different behavior relative to that of protons. The strangeness balance and the production yield per participating nucleon as a function of the centrality of the reaction are discussed, for the first time at GSI Schwerionen Synchrotron (SIS) energies.
European Physical Journal A | 2005
R. Kotte; J. P. Alard; A. Andronic; V. Barret; Z. Basrak; N. Bastid; M. L. Benabderrahmane; R. Čaplar; E. Cordier; Philippe Crochet; P. Dupieux; M. Dželalija; Z. Fodor; I. Gašparić; A. Gobbi; Y. Grishkin; O. N. Hartmann; N. Herrmann; K. D. Hildenbrand; B. Hong; J. Kecskemeti; Y. J. Kim; M. Kirejczyk; P. Koczon; M. Korolija; T. Kress; A. Lebedev; Y. Leifels; X. Lopez; M. Merschmeyer
Abstract.Small-angle correlations of pairs of protons emitted in central collisions of Ca + Ca, Ru + Ru and Au + Au at beam energies from 400 to 1500MeV per nucleon are investigated with the FOPI detector system at SIS/GSI Darmstadt. Dependences on system size and beam energy are presented which extend the experimental data basis of pp correlations in the SIS energy range substantially. The size of the proton-emitting source is estimated by comparing the experimental data with the output of a final-state interaction model which utilizes either static Gaussian sources or the one-body phase-space distribution of protons provided by the BUU transport approach. The trends in the experimental data, i.e. system size and beam energy dependences, are well reproduced by this hybrid model. However, the pp correlation function is found rather insensitive to the stiffness of the equation of state entering the transport model calculations.
Physical Review C | 2007
W. Trautmann; B. Zwieglinski; R. Bassini; A. Schüttauf; G. Verde; G. Riccobene; C. Sfienti; A. Moroni; J. Pochodzalla; A. Trzcinski; F. Petruzzelli; G. Raciti; I. Iori; B. Ocker; T. Möhlenkamp; V. Maddalena; C. Schwarz; G. Imme; F.P. Romano; S. Fritz; C. Nociforo; Th. Rubehn; A. Le Fèvre; J. Lukasik; U. Kleinevoss; W. F. J. Müller; H. Sann; U. Lynen; H. Orth; G. J. Kunde
Isotope temperatures from double ratios of hydrogen, helium, lithium, beryllium, and carbon isotopic yields, and excited-state temperatures from yield ratios of particle-unstable resonances in {sup 4}He, {sup 5}Li, and {sup 8}Be, were determined for spectator fragmentation, following collisions of {sup 197}Au with targets ranging from C to Au at incident energies of 600 and 1000 MeV per nucleon. A deviation of the isotopic from the excited-state temperatures is observed which coincides with the transition from residue formation to multi-fragment production, suggesting a chemical freeze-out prior to thermal freeze-out in bulk disintegrations.