Abstract: An apparatus for plasma control is disclosed. The apparatus comprises: a plasma generator comprising two electrodes, an anode and a cathode, configured to produce a plasma between the two electrodes; a solenoid coil disposed to surround the plasma and configured to produce a magnetic field parallel to a longitudinal axis between the two electrodes; and circuitry configured for allowing independent timing of the magnetic field with respect to the production of the plasma. A method for plasma control in a spectroscopy system and an optical emission spectrometer using said method are also disclosed.

Abstract: Disclosed herein are various systems and methods for optical emission spectroscopy. In some examples a substrate can be formed from conductive layers separated by a dielectric layer, the substrate having at least one recess therein, and the recess having a aperture therethrough. A chamber then encloses the area over the recess, the chamber including chamber walls, a gas inlet and a gas outlet to allow a gas to fill the chamber. An arc is then created across the substrate using the conductive layers. The arc may form a plasma using the gas inside the chamber. The plasma then ablates a surface of a specimen generating photons that can then be analyzed by a spectrometer.

Abstract: Apparatuses and methods for an optical induced ion source are disclosed herein. An example apparatus at least includes an ionization volume arranged to receive a gas and first optical energy, the first optical energy to ionize the gas, and a channel formed between a first membrane and a second membrane, the first membrane having at least a transparent portion and the second membrane including an aperture, where the gas is provided to the ionization volume through the channel, the ionization volume formed inside the channel and adjacent to the aperture, and where the first optical energy ionizes the gas after passing through the at least transparent portion of the first membrane.

Abstract: A collision ionization source is disclosed herein. An example source includes an ionization region arranged to receive a gas and a charged particle beam, the charged particle beam to ionize at least some of the gas, and a supply duct arranged to provide the gas to the ionization region, the supply duct having a non-uniform height decreasing from an input orifice to an output orifice, the output orifice arranged adjacent to the ionization region.

Abstract: A collision ionization source is disclosed herein. An example source includes an ionization region arranged to receive a gas and a charged particle beam, the charged particle beam to ionize at least some of the gas, and a supply duct arranged to provide the gas to the ionization region, the supply duct having a non-uniform height decreasing from an input orifice to an output orifice, the output orifice arranged adjacent to the ionization region.

Abstract: A collision ionization ion source comprising: A pair of stacked plates, sandwiched about an intervening gap; An input zone (aperture), provided in a first of said plates, to admit an input beam of charged particles to said gap; An output zone (aperture), located opposite said input zone and provided in the second of said plates, to allow emission of a flux of ions from said gap; A gas space, between said input and output zones, in which gas can be ionized by said input beam so as to produce said ions; A supply duct in said gap, for supplying a flow of said gas to said gas space, and comprising: An emergence orifice, opening into said gas space; An entrance orifice, connectable to a gas supply, wherein said duct comprises at least one transition region between said entrance orifice and said emergence orifice in which an inner height of said duct, measured normal to the plates, decreases from a first height value to a second height value.

Abstract: Applicants have found that energetic neutral particles created by a charged exchange interaction between high energy ions and neutral gas molecules reach the sample in a ion beam system using a plasma source. The energetic neutral create secondary electrons away from the beam impact point. Methods to solve the problem include differentially pumped chambers below the plasma source to reduce the opportunity for the ions to interact with gas.

Abstract: An inductively-coupled plasma source for a focused charged particle beam system includes a plasma chamber and a fluid that is not actively pumped surrounding the plasma chamber for providing high voltage isolation between the plasma chamber and nearby parts which are at ground potential, such as a conductive shield. One or more cooling devices cool the plasma chamber by using evaporative cooling and heat pipes to dissipate the heat from the plasma chamber into a surrounding environment.

Abstract: An inductively coupled plasma charged particle source for focused ion beam systems includes a plasma reaction chamber with a removably attached source electrode. A fastening mechanism connects the source electrode with the plasma reaction chamber and allows for a heat-conductive, vacuum seal to form. With a removable source electrode, improved serviceability and reuse of the plasma source tube are now possible.

Abstract: Applicants have found that energetic neutral particles created by a charged exchange interaction between high energy ions and neutral gas molecules reach the sample in a ion beam system using a plasma source. The energetic neutral create secondary electrons away from the beam impact point. Methods to solve the problem include differentially pumped chambers below the plasma source to reduce the opportunity for the ions to interact with gas.

Abstract: An inductively coupled plasma charged particle source for focused ion beam systems includes a plasma reaction chamber with a removably attached source electrode. A fastening mechanism connects the source electrode with the plasma reaction chamber and allows for a heat-conductive, vacuum seal to form. With a removable source electrode, improved serviceability and reuse of the plasma source tube are now possible.

Abstract: An openable gas passage provides for rapid pumpout of process or bake out gases in an inductively coupled plasma source in a charged particle beam system. A valve, typically positioned in the source electrode or part of the gas inlet, increases the gas conductance when opened to pump out the plasma chamber and closes during operation of the plasma source.

Abstract: An improved method and apparatus for shutting down and restoring an ion beam in an ion beam system. Preferred embodiments provide a system for improved power control of a focused ion beam source, which utilizes an automatic detection of when a charged particle beam system is idle (the beam itself is not in use) and then automatically reducing the beam current to a degree where little or no ion milling occurs at any aperture plane in the ion column. Preferred embodiments include a controller operable to modify voltage to an extractor electrode and/or to reduce voltage to a source electrode when idle state of an ion source of the charged particle beam system is detected.

Abstract: Applicants have found that energetic neutral particles created by a charged exchange interaction between high energy ions and neutral gas molecules reach the sample in a ion beam system using a plasma source. The energetic neutral create secondary electrons away from the beam impact point. Methods to solve the problem include differentially pumped chambers below the plasma source to reduce the opportunity for the ions to interact with gas.

Abstract: An inductively coupled plasma charged particle source for focused ion beam systems includes a plasma reaction chamber with a removably attached source electrode. A fastening mechanism connects the source electrode with the plasma reaction chamber and allows for a heat-conductive, vacuum seal to form. With a removable source electrode, improved serviceability and reuse of the plasma source tube are now possible.

Abstract: An inductively-coupled plasma source for a focused charged particle beam system includes a plasma chamber and a fluid that is not actively pumped surrounding the plasma chamber for providing high voltage isolation between the plasma chamber and nearby parts which are at ground potential, such as a conductive shield. One or more cooling devices cool the plasma chamber by using evaporative cooling and heat pipes to dissipate the heat from the plasma chamber into a surrounding environment.

Abstract: An inductively-coupled plasma source for a focused charged particle beam system includes a conductive shield that provides improved electrical isolation and reduced capacitive RF coupling and a dielectric fluid that insulates and cools the plasma chamber. The conductive shield may be enclosed in a solid dielectric media. The dielectric fluid may be circulated by a pump or not circulated by a pump. A heat tube can be used to cool the dielectric fluid.

Abstract: An inductively coupled plasma charged particle source for focused ion beam systems includes a plasma reaction chamber with a removably attached source electrode. A fastening mechanism connects the source electrode with the plasma reaction chamber and allows for a heat-conductive, vacuum seal to form. With a removable source electrode, improved serviceability and reuse of the plasma source tube are now possible.

Abstract: An openable gas passage provides for rapid pumpout of process or bake out gases in an inductively coupled plasma source in a charged particle beam system. A valve, typically positioned in the source electrode or part of the gas inlet, increases the gas conductance when opened to pump out the plasma chamber and closes during operation of the plasma source.

Abstract: The state of an emitter can be determined by measurements of how the current changes with the extraction voltage. A field factor ? function is determined by series of relatively simple measurements of charged particles emitted at different conditions. The field factor can then be used to determine derived characteristics of the emission that, in the prior art, were difficult to determine without removing the source from the focusing column and mounting it in a specialized apparatus. The relations are determined by the source configuration and have been found to be independent of the emitter shape, and so emission character can be determined as the emitter shape changes over time, without having to determine the emitter shape and without having to redefine the relation between the field factor and the series of relatively simple measurements, and the relationships between the field factor and other emission parameters.