The invention is a unique and substantive improvement in ion source assemblies which is able to produce a ribbon-shaped ion beam having an arbitrarily chosen breadth dimension which is at least ten times greater [and often more than thirty times greater] than its thickness dimension, the breadth and thickness dimensions of the beam being normal (i.e., perpendicular) to the Z-axis direction of travel for the ion beam. In all its embodiments, the improved ion source will comprise not less than two discrete component parts: (i) A closed, solid wall, prism-shaped arc discharge chamber having limited width and depth dimensions, and which concurrently has an arbitrarily chosen and predetermined length dimension which can be as small as 80 millimeters and alternatively exceed 3,000 millimeters in size; and (ii) A primary electron trap assembly which comprises at least an adjacently located magnetic field generating yoke subassembly able to provide a discernible quadrupole magnetic field internally within a confined cavity volume existing within the measurable dimensions of the arc discharge chamber walls.

A high brightness ion source with a gas chamber includes multiple channels, wherein the multiple channels each have a different gas. An electron beam is passed through one of the channels to provide ions of a certain species for processing a sample. The ion species can be rapidly changed by directing the electrons into another channel with a different gas species and processing a sample with ions of a second species. Deflection plates are used to align the electron beam into the gas chamber, thereby allowing the gas species in the focused ion beam to be switched quickly.

An ion generator includes an arc chamber defining a plasma generation space, and a cathode which emits thermoelectrons toward the plasma generation space. The arc chamber includes a box-shaped main body having an opening, and a slit member mounted to cover the opening and provided with a front slit. An inner surface of the main body is exposed to the plasma generation space made of a refractory metal material. The slit member includes an inner member made of graphite and an outer member made of another refractory metal material. The outer member includes an outer surface exposed to an outside of the arc chamber. The inner member includes an inner surface exposed to the plasma generation space, and an opening portion which forms the front slit extending from the inner surface of the inner member to the outer surface of the outer member.

An apparatus to generate negative hydrogen ions. The apparatus may include an ion source chamber having a gas inlet to receive H.sub.2 gas; a light source directing radiation into the ion source chamber to generate excited H.sub.2 molecules having an excited vibrational state from at least some of the H.sub.2 gas; a low energy electron source directing low energy electrons into the ion source chamber, wherein H.sup. ions are generated from at least some of the excited H.sub.2 molecules; and an extraction assembly arranged to extract the H.sup. ions from the ion source chamber.

An ion source chamber for ion implantation system includes a housing that at least partially bounds an ionization region through which high energy electrons move from a cathode to ionize gas molecules injected into an interior of the housing; a liner section defining one or more interior walls of the housing interior, wherein each liner section includes a interiorly facing surface exposed to the ionization region during operation the ion implantation system; a cathode shield disposed about the cathode; a repeller spaced apart from the cathode; a plate including a source aperture for discharging ions from the ion source chamber; wherein at least one of the repeller, the liner section, the cathode shield; the plate, or an insert in the plate defining the source aperture comprise silicon carbide, wherein the silicon carbide is a non-stoichiometric sintered material having excess carbon.

An ion generator includes an arc chamber defining a plasma generation space, and a cathode which emits thermoelectrons toward the plasma generation space. The arc chamber includes a box-shaped main body having an opening, and a slit member mounted to cover the opening and provided with a front slit. An inner surface of the main body is exposed to the plasma generation space made of a refractory metal material. The slit member includes an inner member made of graphite and an outer member made of another refractory metal material. The outer member includes an outer surface exposed to an outside of the arc chamber. The inner member includes an inner surface exposed to the plasma generation space, and an opening portion which forms the front slit extending from the inner surface of the inner member to the outer surface of the outer member.

A cathode apparatus for an ion source has a cathode with a positioning feature and a blind hole. A cathode holder has an aperture defined by a thru-hole and a locating feature defined along an aperture axis. The thru-hole receives the cathode along the aperture axis in first and second alignment positions based on a rotational orientation of the positioning feature with respect to the locating feature. The first alignment position locates the cathode at a first axial position along the aperture axis. The second alignment position locates the cathode at a second axial position along the axial axis. A filament device has a filament clamp, a filament rod defining a filament axis, and a filament coupled to the filament rod. The filament clamp is in selective engagement with the filament rod to selectively position the filament along the filament axis within the blind hole.

An ion source with a target holder for holding a solid dopant material is disclosed. The ion source comprises a thermocouple disposed proximate the target holder to monitor the temperature of the solid dopant material. In certain embodiments, a controller uses this temperature information to vary one or more parameters of the ion source, such as arc voltage, cathode bias voltage, extracted beam current, or the position of the target holder within the arc chamber. Various embodiments showing the connections between the controller and the thermocouple are shown. Further, embodiments showing various placement of the thermocouple on the target holder are also presented.

An ion source is disclosed, in which the compression force applied to the faceplate on the two sides of the extraction aperture may be varied independently. Modifying the compression force between the faceplate and arc chamber can enable temperature control of the ion source by modifying the thermal contact resistance between the two components. This may allow more control of the temperature of the faceplate, and more specifically, the temperature profile across the entire faceplate due to precise control of the thermal contact gradient along the length of the faceplate. The ion implantation system includes two adjustable tension systems, each of which includes an actuator. A controller is used to provide a command signal to each adjustable tension system. In some embodiments, a feedback signal is generated by each adjustable tension system, which is representative of the torque or force experienced by the actuator.

An ion source is provided which can operate in a monomer mode or a cluster mode without experiencing losses. According to embodiments, an ion source can include a cathode that emits electrons. A plasma generation chamber can have an opening region through which the electrons pass. An electrode can be disposed between the cathode and the opening region, the electrode including a cylindrical portion through which the electrons pass. The electrode can be set to a negative potential with respect to the plasma generation chamber or a positive potential with respect to the plasma generation chamber. An exemplary method can include setting the electrode to a negative potential with respect to the plasma generation chamber if the ion species is a monoatomic ion, or setting the electrode to a positive potential with respect to the plasma generation chamber if the ion species is a molecular ion.