An apparatus for analyzing and/or processing a sample with a particle beam, comprising: a sample stage for holding the sample; a providing unit for providing the particle beam comprising: an opening for guiding the particle beam to a processing position on the sample; and a shielding element for shielding an electric field generated by charges accumulated on the sample; wherein the shielding element covers the opening, is embodied in sheetlike fashion and comprises an electrically conductive material; wherein the shielding element comprises a convex section, this section being convex in relation to the sample stage; and wherein the convex section has a through opening for the particle beam to pass through to the sample.

The present invention quickly calculates values of optimal excitation parameters which are set in lenses in multiple stages. A multi charged particle beam adjustment method includes forming a multi charged particle beam, calculating, for each of lenses in two or more stages disposed corresponding to object lenses in two or more stages, a first rate of change and a second rate of change in response to change in at least an excitation parameter, the first rate of change being a rate of change in a demagnification level of a beam image of the multi charged particle beam, the second rate of change being a rate of change in a rotation level of the beam image, and calculating a first amount of correction to the excitation parameter of each of the lenses based on an amount of correction to the demagnification level and the rotation level of the beam image, the first rate of change, and the second rate of change.

An ion source for an ion implantation system is configured to form an ion beam from a predetermined species along a beamline, where the ion beam is at an initial energy. A deceleration component is configured to decelerate the ion beam to a final energy that is less than the initial energy. A workpiece support is configured to support a workpiece along a workpiece plane downstream of the deceleration component along the beamline. A beamline component is positioned downstream of the deceleration component along the beamline. The beamline component has a feature that is at least partially impinged by the ion beam, and where the feature has a surface having a predetermined angle of incidence with respect to the ion beam. The predetermined angle of incidence provides a predetermined sputter yield of the ion beam at the final energy that mitigates deposition of the ion species on the beamline component.

A method for irradiating a target with a beam of energetic electrically charged particles, wherein the target comprises an exposure region where an exposure by said beam is to be performed, and the exposure of a desired pattern is done employing a multitude of exposure positions on the target. Each exposure position represents the location of one of a multitude of exposure spots of uniform size and shape, with each exposure spot covering at least one pattern pixel of the desired pattern. The exposure positions are located within a number of mutually separate cluster areas which are defined at respective fixed locations on the target. In each cluster area the exposure position are within a given neighboring distance to a next neighboring exposure position, while the cluster areas are separated from each other by spaces free of exposure positions, which space has a width, which is at least the double of the neighboring distance.

An ion implanter includes: a plurality of devices which are disposed along a beamline along which an ion beam is transported; a plurality of neutron ray measuring instruments which are disposed at a plurality of positions in the vicinity of the beamline and measure neutron rays which are generated at a plurality of locations of the beamline due to collision of a high-energy ion beam; and a control device which monitors at least one of the plurality of devices, based on a measurement value in at least one of the plurality of neutron ray measuring instruments.

An ion implantation system includes an ion implanter containing an ion source unit and a dopant source gas supply system. The system includes a dopant source gas storage tank inside a gas box container located remotely to the ion implanter and a dopant source gas supply pipe configured to supply a dopant source gas from the dopant source gas storage tank to the ion source unit. The dopant source gas supply pipe includes an inner pipe, an outer pipe enclosing the inner pipe, a first pipe adaptor coupled to first end of respective inner and outer pipes, and a second pipe adaptor coupled to seconds end of respective inner and outer pipes opposite the first end. The first pipe adaptor connects the inner pipe to the dopant source gas storage tank and the second pipe adaptor connects the inner pipe to the ion source unit.

A system and method for controlling an amount of outgassing caused by implanting ions into a photoresist disposed on a workpiece. The amount of outgassing is based on the species being implanted, the type of photoresist, the energy of the implant, and the amount of dose that has already been implanted, among other effects. By controlling the effective beam current, the amount of outgassing may be maintained below a predetermined threshold. By developing and utilizing the relationship between effective beam current, dose completed and rate of outgassing, the effective beam current may be controlled more precisely to implant the workpiece in the most efficient manner while remaining below the predetermined outgassing threshold.

A heater assembly that that is effective at maintaining heating lamps at acceptable temperatures is disclosed. The heater assembly utilizes radiative heat transfer to transfer unwanted heat buildup in the heating lamps to a cooling base. One or more high emissivity films are disposed between the heating lamps and the cooling base to facilitate heat transfer. Further, a reflective coating is applied to a portion of the heating lamps to reflect heat away from the cooling base. The heater assembly may be utilized in a high vacuum environment as it does not rely on convective cooling.

A method of depositing material over a sample in a deposition region of the sample with a charged particle beam column, the method comprising: positioning a sample within a vacuum chamber such that the deposition region is under a field of view of the charged particle beam column; cooling the deposition region by contacting the sample with a cyro-nanomanipulator tool in an area adjacent to the deposition region; injecting a deposition precursor gas into the vacuum chamber at a location adjacent to the deposition region; generating a charged particle beam with a charged particle beam column and focusing the charged particle beam on the sample; and scanning the focused electron beam across the localized region of the sample to activate molecules of the deposition gas that have adhered to the sample surface in the deposition region and deposit material on the sample within the deposition region

An aperture diaphragm capable of varying the size of an aperture in two dimensions is disclosed. The aperture diaphragm may be utilized in an ion implantation system, such as between the mass analyzer and the acceleration column. In this way, the aperture diaphragm may be used to control at least one parameter of the ion beam. These parameters may include angular spread in the height direction, angular spread in the width direction, beam current or cross-sectional area. Various embodiments of the aperture diaphragm are shown. In certain embodiments, the size of the aperture in the height and width directions may be independently controlled, while in other embodiments, the ratio between height and width is constant.