Abstract: The present invention is directed to a gas line electron beam exciter, gas line electron beam excitation system and method for exciting a gas using an electron beam exciter. The electron beam exciter generally comprises a variable density electron source for generating a cloud of electrons in an electron chamber and a variable energy electron extractor for accelerating electrons from the electron chamber as an electron beam and into an effluent stream for fluorescing species in the effluent. The electron density of the electron beam is variably controlled by adjusting the excitation power applied to the variable density electron source. The electrons in the electron chamber reside at a reference electrical potential of the chamber, typically near ground electrical potential.

Abstract: The present invention is directed to a gas line electron beam exciter, gas line electron beam excitation system and method for exciting a gas using an electron beam exciter. The electron beam exciter generally comprises a variable density electron source for generating a cloud of electrons in an electron chamber and a variable energy electron extractor for accelerating electrons from the electron chamber as an electron beam and into an effluent stream for fluorescing species in the effluent. The electron density of the electron beam is variably controlled by adjusting the excitation power applied to the variable density electron source. The electrons in the electron chamber reside at a reference electrical potential of the chamber, typically near ground electrical potential.

Abstract: A pulsed plasma doping system separates the plasma ignition function from the ion implantation function. An ignition voltage pulse is supplied to an ionizable gas and an implantation voltage pulse is applied to the target. The implantation voltage pulse can be generated from the ignition voltage pulse or can be generated separately from the ignition voltage pulse. Ions may be implanted in the target at an energy level that is below the Paschen curve for the system.

Abstract: A plasma doping apparatus includes a hollow cathode to increase throughput and uniformity of ion implantations in a target. The hollow cathode is located adjacent an anode and a target cathode on which a target is placed. An ionizable gas is provided in a space between the anode and the target cathode. The space in which the ionizable gas is provided is surrounded by the hollow cathode. The hollow cathode has either a circular or rectangular cross-section.

Abstract: In a plasma processing system, displacement current is removed from a current measurement by providing a secondary capacitor connected in parallel with a primary capacitor defined by an anode and a cathode spaced from one another within the plasma doping chamber. The secondary capacitor is chosen or adjusted to have a same or nearly the same capacitance as the primary capacitor. When a voltage pulse is applied to both the primary and secondary capacitors, the respective currents through the capacitors are measured. In order to remove the effects of the displacement current that is present at the leading and falling edges of the voltage pulse, and in order to measure the ion current within the doping chamber, the secondary current through the secondary capacitor is subtracted from the primary current through the primary capacitor.

Abstract: A pulsed plasma doping system separates the plasma ignition function from the ion implantation function. An ignition voltage pulse is supplied to an ionizable gas and an implantation voltage pulse is applied to the target. The implantation voltage pulse can be generated from the ignition voltage pulse or can be generated separately from the ignition voltage pulse. Ions may be implanted in the target at an energy level that is below the Paschen curve for the system.

Abstract: A pulsed plasma doping system separates the plasma ignition function from the ion implantation function. An ignition voltage pulse is supplied to an ionizable gas and an implantation voltage pulse is applied to the target. The implantation voltage pulse can be generated from the ignition voltage pulse or can be generated separately from the ignition voltage pulse. Ions may be implanted in the target at an energy level that is below the Paschen curve for the system.

Abstract: A plasma doping apparatus includes a hollow cathode to increase throughput and uniformity of ion implantations in a target. The hollow cathode is located adjacent an anode and a target cathode on which a target is placed. An ionizable gas is provided in a space between the anode and the target cathode. The space in which the ionizable gas is provided is surrounded by the hollow cathode. The hollow cathode has either a circular or rectangular cross-section.