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To Meet the FAIR science requirements higher beam intensity has to be achieved in the present GSI-accelerator complex. An advanced upgrade program for the UNILAC aimed to meet the FAIR requirements is ongoing. Stripping is a key technology for all heavy ion accelerators. For this an extensive research and development program was carried out to optimize for high brilliance heavy ion operation. After upgrade of the supersonic N2-gas jet (2007), implementation of high current foil stripping (2010 and 2011) and preliminary investigation of H2-gas jet operation (2012), a new H2-gas cell using a pulsed gas regime synchronized with arrival of the beam pulse was recently developed. An obviously enhanced stripper gas density at a simultaneously reduced gas load result in an increased stripping efficiency, while the beam emittance remains the same. A new record intensity (7.8 emA) for U beams at 1.4 MeV/u has been achieved applying the pulsed high density H2 stripper target, exploiting a high intensity U beam from the VARIS ion source with a newly developed extraction system. The experimental results will be presented in detail. STRIPPING OF HEAVY ION BEAMS Suitable charge stripper technologies [1] are crucial to meet the challenging demands of state of the art heavy ion accelerator facilities. At FAIR presently under construction at GSI the existing linear accelerator UNILAC and the synchrotron SIS18 will serve as injector chain for the FAIR SIS100 synchrotron. Different approaches are investigated to increase the stripping efficiency of the heavy ion beam at 1.4 MeV/u and to generate higher charge states [2–5]. The stripper target at 1.4 MeV/u has to cope with a very high ion beam power of up to 1.5 MW for 18 emA U beams during short beam pulses (100 μs) at low duty cycle (2.7 Hz rep. rate). Though for high beam powers gas or liquid strippers have clear advantages compared to foil strippers concerning durability and operational reliability, gas strippers lead to much lower equilibrium charge states due to the strongly reduced influence of the density effect [6–8] compared to solid strippers. Since electron capture cross sections of the heavy ions especially in the low-Z gases are considerably suppressed [8, 9], in particular hydrogen promises higher equilibrium charge states as compared to e.g. nitrogen, which is routinely used at the UNILAC gas stripper [10]. Thus a new setup, suitable for H2 operation has been constructed. To enhance the gas density a pulsed gas injection [11] was implemented. This allows an increase of the maximum gas pressure and creates a high-pressure interaction zone for the stripping process. The time between two pulses is used to remove most of the gaseous particles from the system before injection of the next pulse. UNILAC STRIPPER SECTION Figure 1: Layout of the 1.4 MeV/u stripper section; 14.0 m total length. For the UNILAC a stripper section [12] was redesigned and installed in 1999 (Fig. 1). Charge separation and beam transport under highest space charge conditions and multi beam operation with pulsed magnets was established. A supersonic N2-gas jet produced by a Laval nozzle crosses the ion beam in the central interaction region of the gas stripper chamber. Two sections of differential pumping upstream and downstream of the central region are pumped by four powerful turbo pumps (pumping speed 1200 l/s). The charge separator Proceedings of IPAC2015, Richmond, VA, USA THPF008 4: Hadron Accelerators A08 Linear Accelerators ISBN 978-3-95450-168-7 3693 Co py rig ht © 20 15 CC -B Y3. 0 an d by th er es pe ct iv ea ut ho rs comprises three bending magnets, operating in pulsed mode, based on a 50 Hz repetition frequency. In the following transport line the transversal and longitudinal matching to the poststripper accelerator is accomplished. BEAM EXPERIMENTS WITH A PULSED GAS STRIPPER CELL Characterizing the stripping performance, the absolute stripping efficiency into the desired charge state is a key indicator. A sufficient charge state resolution is required to enable highest intensities in the desired charge state. To compare the performance of the modified stripper setup with that of the existing gas-jet stripper, uranium beam measurements in both setups were conducted with a N2-target. It could be shown in [11] with Bi-beam that the measured relative charge state spectrum for jet operation as well as for the pulsed gas cell is the same inside the error limits, if the equilibrium charge state is reached. Figure 2: N2-gas jet (top) and H2-pulsed gas cell (bottom) charge spectra for max. available target density [13]. As shown in Fig. 2, the measured charge stripping distribution using the maximum target thickness available for N2-jet operation shows a relatively broad distribution (FHWM 7 charge states), but well separated peaks. The same level of separation purity was observed for H2-gas cell operation. But the width of distribution is much narrower (FHWM 4.5 charge states) and the shape of distribution is obviously more symmetric. As a result the relative maximum is significantly increased, while the peripheral areas are diminished. Besides, the maximum of the distribution is shifted by one charge state. The evaluation of charge spectra resulted in a 59% higher stripping efficiency for U as the most interesting uranium charge state for FAIR injector operation. Assuming an increased stripping efficiency for thicker targets, high current uranium operation for post stripper acceleration with even higher charge states appears possible [13]. Table 1: Measured Beam Parameters [13] N2-gas jet H2pulsed gas Stripper-(pre-)pressure 0.4 MPa 12.0 MPa U-current (HSI) 6.0 emA Max.U-current 4.5 emA 7.8 emA Total current (stripped) 24 emA 34 emA Stripping efficiency 12.70% 20.14% Energy loss 30 keV/u 22 keV/u x (90%, tot.) norm. 0.76 μm 0.70 μm y (90%, tot.) norm. 0.84 μm 0.93 μm Hor. beam brilliance 5.32 mA/μm 10.03 mA/μm

physical review special topics. accelerators and beams

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U28+-intensity record applying aH2