Apparatus and methods for adjusting beam condition of charged particles are disclosed. According to certain embodiments, the apparatus includes one or more first multipole lenses displaced above an aperture, the one or more first multipole lenses being configured to adjust a beam current of a charged-particle beam passing through the aperture. The apparatus also includes one or more second multipole lenses displaced below the aperture, the one or more second multipole lenses being configured to adjust at least one of a spot size and a spot shape of the beam.

A multiple electron beam irradiation apparatus includes a shaping aperture array substrate to form multiple primary electron beams, a plurality of electrode array substrates stacked each to dispose thereon a plurality of electrodes each arranged at a passage position of each of the multiple primary electron beams, each of the multiple primary electron beams surrounded by an electrode of the plurality of electrodes when each of the multiple primary electron beams passes through the passage position, the first wiring and the second wiring applied with one of different electric potentials, and a stage to mount thereon a target object to be irradiated with the multiple primary electron beams having passed through the plurality of electrode array substrates, wherein, in each of the plurality of electrode array substrates, each of the plurality of electrodes is electrically connected to either one of the first wiring and the second wiring.

The present disclosure relates to an apparatus and method that manipulate the voltage at an edge ring relative to a substrate located on a substrate support located within a processing chamber. The apparatus includes a substrate support assembly that has a body having a substrate support portion having a substrate electrode embedded therein for applying a substrate voltage to a substrate. The body of the substrate support assembly further has an edge ring portion disposed adjacent to the substrate support portion. The edge ring portion has an edge ring electrode embedded therein for applying an edge ring voltage to an edge ring. The apparatus further includes an edge ring voltage control circuit coupled to the edge ring electrode. A substrate voltage control circuit is coupled to the substrate electrode. The edge ring voltage control circuit and the substrate voltage control circuit are independently tunable to generate a difference in voltage between the edge ring voltage and the substrate voltage.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit changes a single electron source into a virtual multi-source array, a primary projection imaging system projects the array to form plural probe spots on the sample, and a condenser lens adjusts the currents of the plural probe spots. In the source-conversion unit, the image-forming means is on the upstream of the beamlet-limit means, and thereby generating less scattered electrons. The image-forming means not only forms the virtual multi-source array, but also compensates the off-axis aberrations of the plurality of probe spots.

A charged particle beam device is described, which includes: a beam source configured to generate a charged particle beam propagating along an optical axis (A); an aperture device with a plurality of apertures configured to create a plurality of beamlets from the charged particle beam; and a field curvature corrector. The field curvature corrector includes: a first multi-aperture electrode with a first plurality of openings having diameters that vary as a function of a distance from the optical axis (A); a second multi-aperture electrode with a second plurality of openings; and an adjustment device configured to adjust at least one of a first electrical potential (U1) of the first multi-aperture electrode and a second electrical potential (U2) of the second multi-aperture electrode. Further, a field curvature corrector and methods of operating a charged particle beam device are described.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

Systems for reducing the generation of thermal magnetic field noise in optical elements of microscope systems, are disclosed. Example microscopy optical elements having reduced Johnson noise generation according to the present disclosure comprises an inner core composed of an electrically isolating material, and an outer coating composed of an electrically conductive material. The product of the thickness of the outer coating and the electrical conductivity is less than 0.01?.sup.?1. The outer coating causes a reduction in Johnson noise generated by the optical element of greater than 2?, 3?, or an order of magnitude or greater. In a specific example embodiment, the optical element is a corrector system having reduced Johnson noise generation. Such a corrector system comprises an outer magnetic multipole, and an inner electrostatic multipole. The inner electrostatic multipole comprises an inner core composed of an electrically isolating material and an outer coating composed of an electrically conductive material.

A charged particle beam writing method includes forming an aperture image by making a charged particle beam pass through an aperture substrate, changing, in the state where a plurality of crossover positions of the charged particle beam and positions of all of one or more intermediate images of the aperture image are adjusted to matching positions with respect to the aperture image with the first magnification, magnification of the aperture image from the first magnification to the second magnification by using a plurality of lenses while maintaining the last crossover position of the charged particle beam and the position of the last intermediate image of the aperture image to be fixed, and forming, using an objective lens, the aperture image whose magnification has been changed to the second magnification on the surface of the target object, and writing the aperture image.

An ion implantation apparatus includes: a multistage linear acceleration unit including a plurality of stages of high-frequency resonators and a plurality of stages of focusing lenses; a first beam measuring unit disposed in the middle of the multistage linear acceleration unit and configured to allow passage of a beam portion adjacent to a center of a beam trajectory and measure a current intensity of another beam portion blocked by an electrode body outside a vicinity of the center of the beam trajectory; a second beam measuring unit disposed downstream of the multistage linear acceleration unit and configured to measure a current intensity of an ion beam exiting from the multistage linear acceleration unit; and a control device configured to adjust a control parameter of the plurality of stages of focusing lenses based on measurement results of the first and second beam measuring units.