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Pulsed beam current can be achieved by regulating the bias voltage on the control grid electrode of electron gun.
High output ion beam current can be extracted axially in a direction normal to the discharge region without using extraction system.
For some clusters, the ion beam current can be increased by 1 to 2 orders of magnitude by adjusting the source parameters.
The electron energy can be tuned in the range from 200 MeV up to 600 MeV and the electron beam current can be adjusted from 1 pA (single electron) up to 200 mA.
It is found that the optimum gap distance between the anode and the cathode is equal to 3.5 mm, where stable discharge current and maximum output ion beam current can be obtained.
The system is similar to the one in Lawrence Berkeley Laboratory, which was first built and developed by Brown et al. The broad-beam ion source can be repetitively pulsed at rates up to ∼50 pulses per second and the extracted ion beam current can be up to ∼1 A peak or ∼10 mA time averaged.
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Combined with the use of gate control to pulse the X-ray source, high beam currents can be very advantageous to system designers.
Ion currents of a few specially positioned ion pumps were slight high in the high beam current, which can be explained as an effect of electron multiplying.
The base value, peak value and frequency of pulsed beam current all can be adjusted conveniently.
These calculations are very time consuming and in many cases, in particular for high beam current accelerators, can be sensibly only done using parallel computing.
According to our present results, such high current beams can be dissipated in a liquid-lithium target, hence the target design is readily applicable for accelerator-based BNCT.
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