studies of exotic nuclei with electromagnetic and ligh hadronic probes (EXL) is part of the FAIR project . The aim of the EXL experiment is to study the structure of unstable exotic nuclei in light-ion scattering [...] light-ion reactions in inverse kinematics by using novel storage-ring techniques and a universal detector system providing high resolution and large solid angle coverage in kinematically complete measurements.

ty of the different detector systems and their associated DAQ sub-systems. To this goal, the data acquisition will be based on MBS – a distributed data acquisition system that provides a generalized m [...] being integrated into MBS by means of the GEMEX system board . The control, trigger and data flow are susequently interfaced to the common DAQ system. We provide the necessary trigger types, like data [...] individual detector system. As examples (see figures below), for Silicon Strip detectors the AMS front-end electronics has been made available through the locally developped Siderem module . The integrated

quasi-free scattering reactions are tracked with a dedicated tracking system surrounding the target. More details can be found here . [...] focussed in the forward direction and detected with high effciency in the NeuLAND neutron detector . The momenta of the neutrons are determined from the time-of-flight and position information. At the

the further development of the SAM2 module, the centerpiece of the GSI Heavy Ion Therapy Control system. Main improvements are increased memory buffers to handle larger event sizes and the addition of [...] SAM3 processor board (6U VME) is based on two Floating Point Digital Signal Processors TMS320C6711 . Features Two generic readout and control GTB interfaces per board. Up to 100m distances and up to 20Mbytes/s

Antiprotonic exotic atoms (pdf - MiB) Christoph Scheidenberger GSI Towards higher precision Eletron cooling in traps (pdf - 0.7MiB) Günther Zwicknagel Erlangen The TITAN-EBIT (pdf - 1.7MiB) Günther Sikler [...] Georg Bollen MSU HITRAP cooler trap, transport of HCI (pdf - 0.6MiB) Frank Herfurth GSI Sympathetic cooling of HCI Veli Kolhinen Munich Systematical studies and improvements of JYFLTRAP (pdf - 2.2MiB) Tommi [...] selectivity Non destructive electronic detection techniques and electronics for cryogenic trap systems (pdf - 1.3MiB) Stefan Stahl Laser spectroscopy and atom traps Atom trapping at KVI (pdf - 1.3MiB)

stored after each shot by the PCS . The PCS bases on the Control System Framework ( CS ) developed at GSI and used several groups worldwide. Described in key words the system uses the object oriented approach [...] The PHELIX Control System (PCS) technical contact: Stefan Götte PHELIX is controlled by use of the PCS . This serves when PHELIX is aligned as well as to control the sequence of a high energy laser shot [...] distributed, event driven and free available (GNU Public License). Programming language is LabVIEW ™ . With the PCS about 70 cameras, more than 170 motors, 25 power meter, about 30 end-switch controlled

during standard operation. The current status of the RF systems is available on our online monitoring page . Development Projects Cavity systems for the SIS100 (Acceleration, Bunch Compression, K.O.- [...] projects. Some of these projects are listed in the following. Operation of Ring-RF-Systems The operation of the RF systems requires continuous maintenance work, repair in case of failures, and stand-by service [...] Extraction, Barrier Bucket, and Longitudinal Feedback) Cavity systems for the CR Digital RF Control Bunch Phase Timing System BuTiS Fast semiconductor gap switches to temporarily short-circuit the ceramic

terawatt. PHELIX is a flashlamp-pumped Nd:glass system employing two frontends ( short pulse - and long pulse-frontend ), a pre-amplifier and a main amplifier . It was built in close cooperation with Lawrence

Pre-Amplifier Technical contact: Udo Eisenbarth The Pre-Amplifier system uses two flashlamp-pumped Nd:glass amplifiers with free apertures of 19 mm and 45 mm, operating in a double-pass mode. The input [...] aberrations are actively corrected by a deformable mirror, which operates in a closed-loop control system with a Shack-Hartmann sensor. Positioned at the end of the laser chain, this sensor allows the deformable [...] Key parameters are: Maximum output energy (fs pulses): 8J Maximum output energy (ns pulses): 15J Cool down between shots: 3 min Maximum gain (depending on spectral width): >600 (dep. on the spectral range

Nd:glass amplifier modules. Its design originates from the formet Nova and Phebus laser amplifier systems. With a beam diameter of up to 28 cm, it can produce output energies reaching one kilojoule. For [...] output energy (ns pulses): 1 kJ Maximum gain: 100 Maximum output beam diameter: 28 cm (tophat profile) Cool down between shots: 1.5h