highly energetic and/or highly charged ions up to naked uranium U 92+ and short-lived isotopes far off stability. Powerful accelerator devices such as the heavy-ion synchrotron and the experimental storage [...] be roughly split into the following topics: Spectroscopy of highly charged ions Dynamics and reactions of highly charged ions Determination of Ground state properties of atomic nuclei with atomic physics [...] the Atomic, Quantum & Fundamental Physics department at GSI is the ESR. In the ESR, highly-charged ions can be stored and investigated over a long period of time. Here, electron capture from an electron

in computer modeling and simulations which are validated by measurements on heavy ion beams. High intensity ion beams The focus of the department are on the hitherto existing GSI accelerator facility as [...] t and benchmarking of computer models for ion beams The members of the department contribute significantly to the understanding of the dynamics of intense ion beams by development and evaluation of computer [...] Department Accelerator physics Physics of high intensity ion beams The GSI accelerator physics department contributes to the optimization of the GSI and FAIR machines. The key aspect of the work is in

Structure of Atoms, Highly Charged Ions & Nuclei ESR Experiments @ ESR HITRAP: Ion Trap Experiments SPARC @ FAIR CRYRING @ ESR Plasma Physics Compressing Matter by Intensive Ion and Laser Beams PHELIX: the Petawatt [...] Materials Research Material Science with Accelerated Ions Biophysics & Medical Developments © David Sánchez Medina Calderón Biophysics & Tumor Therapy with Ion Beams Information Technology © Otto/GSI/FAIR R&D [...] Collaboration/GSI HADES @ SIS: The High Acceptance Di-electron Spectrometer ALICE @ CERN:LHC: A Large Ion Collider Experiment CBM @ FAIR:SIS100/300: The Compressed Baryonic Matter Experiment Former experiments

which enables direct imaging of surface modification induced by the ion beam. The sample can be rotated in-situ, switching from the ion beam into the electron beam of the microscope. This setup allows for [...] Time-of-Flight Secondary Ion/Neutral Mass Spectrometry (ToF-SIMS/SNMS). This technique is powerful for analyzing desorbed and sputtered species from a sample surface under swift heavy ion irradiation. M2 Beamline [...] on-line X-ray diffractometer, which allows ion irradiations and X-ray diffraction analysis at any angle of incidence. This setup is ideal for investigating ion-induced modifications of the crystallographic

of DR: the electron-ion collision energy is scanned in fine steps. For center-of-mass (CM) collision energies that match the resonance energies a higher count rate of recombined ions, X (q−1)+ , is recorded [...] with only a few hundred ions produced and injected every 10 minutes into the storage ring were successfully conducted. The list of physics questions studied with electron-ion collision spectroscopy at [...] storage-ring electron coolers or merged-beams free-electron targets, in particular at low electron-ion collision energies. DR is a two-step process: X q+ +e− → X (q−1)+ ∗∗ → X (q−1)+ ∗ +photons. In the

for research with photons neutrons and ions : 120 2014 all JCR publications to the Programe Large-scale facilities for research with photons neutrons and ions : 102 2014 all WOS not JCR publications to [...] for research with photons neutrons and ions : 3 2014 all other refereed publications to the Programe Large-scale facilities for research with photons neutrons and ions : 12 2014 all PhDs to the Programe [...] Large-scale facilities for research with photons neutrons and ions : 14 2014 all refereed publications to the Programe Cancer : 39 2014 all JCR publications to the Programe Cancer : 37 2014 all WOS not

current is defined to be 70mA. The ion source department is responsible for the proton ion source and the low energy beam transport section of the linac. Even tough the ion source is built at the partner institute [...] ng technical specifications and the interface for the later setup of the accelerator at FAIR. The ion source will be RF-driven and delivers 100mA of protons at an extraction voltage of 95kV. There is a

Heavy-ion synchrotron SIS18 with sections Circumference: 216 m Maximum magnetic rigidity: 18 Tm Accelerator ring - SIS ( German: S chwer I onen S ynchrotron ): The from UNILAC pre-accelerated ion beam, [...] is further accelerating in the heavy-ion synchrotron SIS up to 90 % of light speed (270.000 km/s) in a few hundred thousand revolutions. If you have any further questions or remarks, please send an email

Department head Ion Sources Group head of high current ion sources and PIG Radiation protection officer Machine coordinator high current injectors Safety officer R&D and operations of high current ion sources

Heavy-ion synchrotron SIS18 with sections Circumference: 216 m Maximum magnetic rigidity: 18 Tm Accelerator ring - SIS ( German: S chwer I onen S ynchrotron ): The from UNILAC pre-accelerated ion beam, [...] is further accelerating in the heavy-ion synchrotron SIS up to 90 % of light speed (270.000 km/s) in a few hundred thousand revolutions. If you have any further questions or remarks, please send an email