chemical physics of discharges - Argonne National Laboratory
chemical physics of discharges - Argonne National Laboratory chemical physics of discharges - Argonne National Laboratory
162 EXPERIMENTAL WORK Apparatus. The basic apparatus utilized for parametric studies employing a fixed substrate is shown in Fig. 1. The reaction vessel is a simple pyrex tube with the substrate filament suspended down the central axis and suitably sealed at each end. The reactant gases are admitted at one end of the tube and exit at the opposite end. Electrodes are simple con- centric copper strips which may be moved along the tube for optimum positioning. The glow discharge then forms between these electrodes. Both horizontal and vertical reactor configurations have been employed; the vertical system is preferred since dubstrate align- ment is better controlled. The vertical arrangement is also more amenable ,to moving filament systems for continuous filament preparation. Both air and water cooled reaction vessels have been evaluated. Water cooling was originally instituted to minimize sidewall deposition; later work demonstrated that this could be accomplished by regulation of gas composition and current input so as to confine the glow area to the central area of the reaction tube. A three compartment chamber was used so that these experiments could be performed before the system was opened for examination. The balance of the system is largely a gas flow system. Hydrogen is passed through a catalytic cartridge and a liquid nitrogen trap for removal of oxygen and water impurities. Boron trichloride is fed into the hydrogen stream. Both lines have appropriate flowmeter devices. The boron trichloride is controlled at the cylinder valve; satisfactory control with respect to potential condensation is obtained by bleeding the gas into a section of tubing at operating pressures and heated to 35°C. Hydrogen flow is regulated by a stainless steel steel needle valve just downstream from the flowmeter. The combined hydrogen-boron , trichloride stream then passes into the reaction chamber. Exit gases from the reactor pass successively through a trap for condensation of unused boron trichloride, past a manometer, through a Cartesian manostat, and thence to a mechanical vacuum pump. The power supply is a Lockheed-designed 3 Mc oscillator capable of about 30 W output; however, only a portion of this output is available as rf power, about 20 W at 1400-1500 V. The first 20 turns of the large coil (Fig. l), and the capacitance connected across them, act as the tank. The tank is a resonance combination wherein the energy is alternately stored in the condensers and in the field of the coil, with interchange occurring at a fre- quency determined by the coil inductance and capacitance of the condensers. A variable condenser included in the tank allows its frequency to be matched to that of the secondary. When such matching occurs, the coils are efficiently coupled, and rf power is drawn from the secondary. This power is fed into the primary by a 6146A transmitter tube activated at proper frequency by feedback from the tank. This is done through a condenser and a resistor wound with a coil, serving as a low-Q resonance circuit to suppress high frequency parasitic oscillation. A 47K resistor allows the grid to be self-biased. An rf choke pre- vents loss of power into the backup power supply. TWO 1OK resistors and a 7500 fl resis- tors serve as a voltage divider for the screen grid. Materials. The boron trichloride used was electronic grade supplied by American Potash and Chemical Co. Hydrogen was a high purity laboratory grade (BB-H-886) supplied by Air Reduction Co. Quartz monofilament utilized as a substrate for most of the work w88 obtained from the General Electric Co. Glass filaments were drawn from pyrex glass rods by the LMSC glass shop. General Procedure. Experiments were started by evacuating the assembled apparatus to 1 mm Hg pressure. The leak rate was determined by turning off the pump and noting the increase - in Dressure over extended time periods. A leak rate of less than 0.05 mm Hg/min is necessary to avoid boron oxide formation. When the system was determined to be essentially leak free, a flow of hydrogen was introduced and allowed to sweep through the apparatus for 15 to 30 min. The desired gas pressures and flow rates of hydrogen and boron trichloride were established, the power supply for the oscillator turned on, and the flow Was I initiated by adjusting the variable capacitor. At the end of the experiment, the flow discharge and the boron trichloride flow were turned off and hydrogen allowed to sweep through the
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Fig. 1 Process Apparatus<br />
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Fig. 2 Boron on Glass, Longitudinal Section (3000~)<br />
Boron<br />
B2°3<br />
oxygen<br />
Enriched<br />
or<br />
Oriented<br />
Material