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and do not absorb the RF power that is tuned to the m/q ratio of the electron The plasma can remove even the innermost electrons from second-row elements All of these ion sources emit beams of positive ions at relatively low velocities, the ions drift or are pulled out from the ionization region with relatively small electrostatic potentials (U 20 kV) These beams of charged particles can be focused and transported in vacuum to the main accelerating machines 1442 Electrostatic Machines An ion source that is held at a large and stable positive electrostatic potential, V, will accelerate positive ions to a kinetic energy of KE qV The maximum potential is limited by the ability to sustain the high voltage without breaking down the intervening dielectric material (sparking).

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Consideration of the formula for the electric eld E at the surface of a sphere with a radius r, carrying a total charge Q, surrounded by a medium with a dielectric constant 1, which is E Q/1r 2, leads to several common features of electrostatic accelerators The high-voltage terminal should be as large a sphere as possible without any sharp points (the ends of sharp points have small radii) and the terminal should be surrounded by a material with a large dielectric constant A large, carefully prepared terminal can be held at a maximum voltage of % 750 kV in dry air The kinetic energies of ions from such systems are (only) suf cient to induce nuclear reactions among the lightest elements and are often used to generate neutrons via the d t !a n reaction.

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The breakdown voltages of various gases were studied as a function of pressure in the 19th century by Paschen, and he showed, not surprisingly, that pure gases have higher breakdown potentials than air Thus, higher electrostatic potentials can be maintained by insulating the platform with an inert gas such as N2 or SF6 and by increasing the gas pressure An important distinguishing feature of electrostatic accelerators is that the beam is emitted continuously from the ion source and is literally a direct current (DC) beam of particles This feature can be good or bad depending on the application, but a DC beam can be chopped, switched, or pulsed to produce an alternating beam (AC) beam The underlying principle for production of high voltages is that the leakage current should be as small as possible, microamps or less, and thus the dissipated power remains low.

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Notice that a current of 1 mA from a 1 MV platform will have a power drain of 1 watt The techniques developed for the production of the very high voltages necessary for electrostatic accelerators fall into two categories: direct and mechanical production Direct production relies on electronic circuits, whereas mechanical production relies on the mechanical transportation of charge to the platform A voltage multiplication circuit for the direct production of very high voltages was developed by Cockcroft and Walton A schematic drawing of the circuit is shown in Figure 144 An alternating current is applied to the transformer at the bottom of the circuit, which is recti ed and multiplied by the stack to produce the high voltage The resulting voltage depends on the number of elements in the stack and on the input voltage.

The high voltage is not precisely constant in that it has a small variation or ripple in.

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