09.2012 06:00- 07:00 U 73+ 300 1E9 HHD SE Grundeinstellung Schicht 07:00- 17:00 U 73+ 300 1E9 HTP SE Zweiharmonischenbetrieb M. Mehler / HF Abt. 17:00- 19:00 U 73+ 300 1E9 HHD SE Einfluss Sextupol D. Ondreka

Physik Journal 3 (1), 31 - 37 (2004) V.P. Shevelko, O. Rosmej, H. Tawara, I.Y. Tolstikhina The target-density effect in electron-capture processes J. Phys. B.: At. Mol. Opt. Phys. 37 (1), 201 - 213 (2004) [...] compression of solid matter by intense heavy-ion-beam-generated pressure waves Laser Particle Beams 22 (1), 59 - 63 (2004) T. E. Cowan, J. Fuchs, et.al., M. Roth, A. Blazevic, E. Brambrink, M. Geissel Ultralow [...] electron transferred to slow highly charged ions interacting with a metal surface Phys. Rev. A 70 (1), 012902 (2004) Neumayer, P.; Seelig, W.; Cassou, K.; Klisnick, A.; Ros, D.; Ursescu, D.; Kuehl, T.;

RELEASE MBS reference, version 6.3, (pdf), (Nov 2017) MBS reference, version 5.1, (pdf), (Aug 2010) MBS-DABC GUI, version 5.1, (pdf), (Mar 2009) MBS reference, version 4.3, (pdf), (Oct 2003) MBS reference [...] PRODUCTION RELEASE MBS version 6.3 (pdf), (Nov-2017) MBS version 6.2 (pdf), (Apr-2013) MBS version 5.1 (pdf), (May 2010) MBS version 5.0 (pdf), (Oct 2006) MBS version 4.3 (pdf), (Jan 2004) MBS version 3 [...] multi-event time stamper, (pdf), (2008) MBS Note 2, requirements for SIS S3xxx, (pdf), (2008) MBS Note 1, multi-event VME readout, (pdf), (2008)

obtain a horizontal kick. Figure 1 shows this process schematically as a top view of the SIS100. © Graphic: GSI Helmholtzzentrum für Schwerionenforschung GmbH Figure 1: Injection-kick The basic circuit [...] identical to the SIS18 kicker . The electrical parameters of the I-kicker can be found in Table 1 Table 1: Electrical data I-Kicker The injection kicker consists of six single magnets, which are located

stabilisieren. In der Elektronenkanone des Elektronenkühlers wird ein Elektronenstrahl von typisch 0.1 bis 1 A aus einer thermischen Kathode von 5 cm Durchmesser in einem longitudinalen Magnetfeld extrahiert [...] darunter und Durchmessern im Bereich von Millimeter, entsprechend Strahlemittanzen von weniger als 1 µm. Die Methode der Elektronenkühlung kommt bei nahezu allen Experimenten am ESR zum Einsatz. Sie erlaubt

pes. 1st Meeting of the International Biophysics Collaboration (Password protected) © [Translate to English:] Photo:G. Otto GSI Helmholtzzentrum für Schwerionenforschung GmbH Group photo of the 1st In [...] Patera Spokesperson Vincenzo Patera , Sapienza University of Rome, Italy vincenzo.patera(at)uniroma1.it © [Translate to English:] J. Prezado Deputy Yolanda Prezado , Centre National de la Recherche Sc

topolgies Based on Linux (Debian, Sugarhat, IPV) (v.2.6) from MBS version V6.1 onwards Based on Real-time system LynxOS (v2.5, 3.1, 4.0) Supports VME, VXI, FASTBUS, CAMAC, PCI Express standards GSI Trigger [...] V7.0 activate at gsi with "prod", "mbslogin prod" or "mbslogin v70" Current development version: V7.1 activate at gsi with "deve", "mbslogin deve" or "mbslogin v7x" Current "old" version: V6.3 activate

irregularity of Hamiltonian systems J. Struckmeier, A. Redelbach Physical Review E 74 (2006) 026209/1-026209/12 Energy-second-moment map: A new means for the regularity analysis of Hamiltonian systems (2005) [...] time-dependent Hamilton-Lagrange systems J. Struckmeier, C. Riedel Physical Review E 66 (2002) 066605/1-066605/12 Hamiltonian systems of charged particles in discrete and continuous description Habilitat [...] for time-dependent Hamiltonian systems J. Struckmeier, C. Riedel Physical Review E 64 (2001) 026503/1-026503/9 Invarianten für zeitabhängige Hamilton-Systeme (2001) Analytical approaches for the dynamics

tracks in the detectors. Two such decays, also from a nickel-nickel reaction at 1.93 GeV per nucleon, are visible in Figure 1. It can be seen that not all of the tracks originate from the same point. The [...] detector systems, the total assembly achieves its goal of covering the complete range of beam energies (0.1 - 2 GeV per nucleon) made available by GSI's SIS heavy ion synchrotron. The target is located within [...] The energy loss is dependent on the type of particle and its momentum in a characteristic way. Figure 1 gives an impression of the available information. This shows the signals ("hits") as squares in a plane

Balß Phone: +49-6159-71-1376 Room: BR1 3.011 Deputy © Copyright: GSI Helmholtzzentrum für Schwerionenforschung GmbH Thomas Winnefeld Phone: +49-6159-71-2014 Room: BR1 3.001 The assignment of the group members