FIELD: electricity.
SUBSTANCE: intense pulse flow of heavy ions in this method is developed by multiple ionisation of heave ions in a rotary electronic ring, electrons in which are of high density and are retained for a long period of time along radius with a combination of a homogeneous Hz=560 Gs and multiple Hm=830 Gs magnetic fields. Retention of electrons in a trap in longitudinal direction is carried out by a field of two turns with current arranged at the ends of the trap, which develop a radial magnetic field Hr with intensity Hr=300 Gs. Injection of electrons with energy We=105 keV is carried out to an equilibrium radius ra=2 cm. in the area of the left turn. Longitudinal speed of electrons in injection is Vz=3*109 cm/s, capture of electrons into the trap is carried out by quick (for the time less than half-cycle of electron oscillations in z direction) "disconnection" of the longitudinal electric field, which moderates electrons. Electron current injected into a trap is Ic=300 A, time of moderating electric field disconnection is τcapt. =5 ns, so that the total number of electrons captured into a trap makes Ne= 1013 electrons, the retained electronic density is equal to ne=2*1010 electrons/cm3, the volume occupied with electrons is Ve=500 cm3. Time of electrons retention in the trap makes τret=10 sec, which makes it possible to produce the total number of multiple-charge ions at 10% probability of ionisation equal to around NU+90-+82=2*10 ions. The number of ions with charge of U+90 will be less by another factor: NU+90=2*109 ions at the frequency of source actuation F=0.1 Hz. Ions are discharged from the ionisation area for the time τrel=1 mcs due to their exposure to a longitudinal electric field, accelerated to the speed of βz=0.01 in the electrostatic field Uel.st.=130 kV, transformed into a beam parallel to the axis z, with a pair of magnetic lenses having Hφ field: Hφ≈800 Gs, and separated by charges with a magnetic field of a rotary magnet having a vertical component Hvert, equal to Hvert=4 kGs. Afterwards the ion beam may be accelerated to the required energy in a linear or a cyclic accelerator.
EFFECT: generation of an ion beam of the required time duration.
2 dwg
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Authors
Dates
2012-04-20—Published
2010-03-29—Filed