A negative ion source includes a plasma chamber, a microwave source, a negative ion converter, a magnetic filter and a beam formation mechanism. The plasma chamber contains gas to be ionized. The microwave source transmits microwaves to the plasma chamber to ionize the gas into atomic species including hyperthermal neutral atoms. The negative ion converter converts the hyperthermal neutral atoms to negative ions. The magnetic filter reduces a temperature of an electron density provided between the plasma chamber and the negative ion converter. The beam formation mechanism extract the negative ions.

A negative ion source includes a plasma chamber, a microwave source, a negative ion converter, a magnetic filter and a beam formation mechanism. The plasma chamber contains gas to be ionized. The microwave source transmits microwaves to the plasma chamber to ionize the gas into atomic species including hyperthermal neutral atoms. The negative ion converter converts the hyperthermal neutral atoms to negative ions. The magnetic filter reduces a temperature of an electron density provided between the plasma chamber and the negative ion converter. The beam formation mechanism extract the negative ions.

The invention relates to a novel ion source, which uses method for the production of highly charged ions in the local ion traps created by an axially symmetric electron beam in the thick magnetic lens. The highly charged ions are produced in the separate local ion traps, which are created as a sequence of the focuses (F.sub.1, F.sub.2, and F.sub.3) of the electron beam (EB) rippled in the magnetic field (B(z)). Since the most acute focus is called the main one, the ion source is classified as main magnetic focus ion source (MaMFIS/T), which can also operate in the trapping regime. The electron current density in the local ion traps can be much greater than that in the case of Brillouin flow. For the ion trap with length of about 1 mm, the average electron current density of up to the order of 100 kA/cm.sup.2 can be achieved. Thus it allows one to produce ions in any charge state for all elements of the Periodic Table. In order to extract the ions, geometry of the electron beam is changed to a relatively smooth electron beam by setting the potential of the focusing electrode (W) of the electron gun negative with respect to the potential of the cathode (C).

The invention relates to a novel ion source, which uses method for the production of highly charged ions in the local ion traps created by an axially symmetric electron beam in the thick magnetic lens. The highly charged ions are produced in the separate local ion traps, which are created as a sequence of the focuses (F.sub.1, F.sub.2, and F.sub.3) of the electron beam (EB) rippled in the magnetic field (B(z)). Since the most acute focus is called the main one, the ion source is classified as main magnetic focus ion source (MaMFIS/T), which can also operate in the trapping regime. The electron current density in the local ion traps can be much greater than that in the case of Brillouin flow. For the ion trap with length of about 1 mm, the average electron current density of up to the order of 100 kA/cm.sup.2 can be achieved. Thus it allows one to produce ions in any charge state for all elements of the Periodic Table. In order to extract the ions, geometry of the electron beam is changed to a relatively smooth electron beam by setting the potential of the focusing electrode (W) of the electron gun negative with respect to the potential of the cathode (C).

An ion generating device including a time-varying electromagnetic power source; and a multi-antenna ion source including a plurality of live antennas electrically coupled to the power source; and a grounded antenna. A neutron generator, including a time-varying electromagnetic power source; a hermetically-sealed tube; a multi-antenna ion source within tube, the multi-antenna ion source including a plurality of live antennas electrically coupled to the time-varying electromagnetic power source; and at most one grounded antenna; an extractor adjacent to an aperture of the multi-antenna ion source; at least one magnet generating a magnetic field substantially parallel to a longitudinal axis of the multi-antenna ion source; a target within the hermetically-sealed tube; and a plurality of electrodes for accelerating and/or decelerating ions toward the target, where the power source operates at a frequency corresponding to a cyclotron frequency defined by a value of the magnetic field within the multi-antenna ion source.

An ion generating device including a time-varying electromagnetic power source; and a multi-antenna ion source including a plurality of live antennas electrically coupled to the power source; and a grounded antenna. A neutron generator, including a time-varying electromagnetic power source; a hermetically-sealed tube; a multi-antenna ion source within tube, the multi-antenna ion source including a plurality of live antennas electrically coupled to the time-varying electromagnetic power source; and at most one grounded antenna; an extractor adjacent to an aperture of the multi-antenna ion source; at least one magnet generating a magnetic field substantially parallel to a longitudinal axis of the multi-antenna ion source; a target within the hermetically-sealed tube; and a plurality of electrodes for accelerating and/or decelerating ions toward the target, where the power source operates at a frequency corresponding to a cyclotron frequency defined by a value of the magnetic field within the multi-antenna ion source.

The presently disclosed ion sources include one or more electromagnets for changing the distribution of plasma within a discharge space of an ion source. At least one of the electromagnets is oriented about an outer periphery of a tubular sidewall of the ion source and changes a distribution of the plasma in a peripheral region of the discharge space.

The presently disclosed ion sources include one or more electromagnets for changing the distribution of plasma within a discharge space of an ion source. At least one of the electromagnets is oriented about an outer periphery of a tubular sidewall of the ion source and changes a distribution of the plasma in a peripheral region of the discharge space.

Embodiments include methods and apparatuses that include a plasma processing tool that includes a plurality of magnets. In one embodiment, a plasma processing tool may comprise a processing chamber and a plurality of modular microwave sources coupled to the processing chamber. In an embodiment, the plurality of modular microwave sources includes an array of applicators positioned over a dielectric that forms a portion of an outer wall of the processing chamber, and an array of microwave amplification modules. In an embodiment, each microwave amplification module is coupled to one or more of the applicators in the array of applicators. In an embodiment, the plasma processing tool may include a plurality of magnets. In an embodiment, the magnets are positioned around one or more of the applicators.

An apparatus may include a cyclotron to receive an ion beam as an incident ion beam at an initial energy, and output the ion beam as an accelerated ion beam at an accelerated ion energy. The apparatus may further include an RF source to output an RF power signal to the cyclotron chamber, the RF power source comprising a variable power amplifier, and a movable stripper, translatable to intercept the ion beam within the cyclotron at a continuum of different positions.