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  • 1995-1999  (3)
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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 69 (1998), S. 1057-1059 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: For the first phase of the GSI high current project, an improvement of Penning ionization gauge (PIG) ion sources is necessary. Therefore, we carry out several PIG source development activities. A test bench for PIG ion sources was set up. It was equipped with the same source magnet, the same beam line, and the same computer control as at the accelerator injector. It has been partly operational since the beginning of 1997. Contrary to the UNILAC accelerator with a typical pulse width of up to 5 ms at a repetition rate of 50 Hz, the synchrotron injection requires a pulse length of about 200 μs at 0.3 Hz. Therefore, the use of lower repetition rates is possible. Thus, more power can be applied to the discharge and increased ion currents can be extracted. This mode requires higher cathode heating, which decreases the lifetime of the filament. The use of monocrystalline LaB6 cathodes drastically reduces the necessary heating power at the same electron current, which should increase the lifetime of the filament and the cathode. The yield of ions from solids was improved by the use of optimized combinations of target and sputtering gas. The use of xenon instead of argon as the sputtering gas for the uranium target yielded a current enhancement of 40%. To achieve a shift of the charge-state distribution to higher charge states, an optimized gas feeding is one option. In collaboration with JINR Dubna, we developed a pulsed gas feeding system. Two piezovalves directly mounted to the source allowed us to control the pressure in the source. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 69 (1998), S. 1079-1081 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: Different ion sources are used at GSI to match the requirements for specific tasks at the accelerator. At the standard injector a Penning ionization gauge ion source is used (design ion U10+, m/q〈24, 1 emA). Further development of this source is mainly aiming at an increase of the extractable currents and an increase of the lifetime of the source. The new injector produces the beam by means of an electron cyclotron resonance source (Caprice-type). Here the design ion is U28+, m/q〈8.5, 5 eμA. Clearly, the oven technology is our main development goal. In addition we are trying to improve the extraction flexibility by a moveable accel–decel system. For our high current project ion sources are required which are capable to deliver a beam of several mA even for heavy ions. Design ion here is U4+, m/q〈65, 15 emA. For that application two different types of ion source are used: the multicusp ion sources "cold or hot reflex discharge ion source" and "multicusp ion source" for gaseous ions and the MEVVA source for metal beams. © 1998 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 67 (1996), S. 1331-1333 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The pulsed magnetic field (PuMa)-electron cyclotron resonance (ECR) ion source uses a pulsed coil to improve the peak current by opening the magnetic bottle along the beam axis. After demonstration of the principle of the pulsed magnetic extraction, the ion source was tested with different gases. We received promising results from helium to krypton. The influence of the current in the pulsed coil on the analyzed ion current was measured. With increased current levels within the pulsed coil not only the pulse height of the PuMa pulse, but the pulse length can also be controlled. By using the pulsed coil the maximum of the charge state distribution can be shifted to higher charge states. © 1996 American Institute of Physics.
    Type of Medium: Electronic Resource
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