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 charged particle assessment tool includes: an objective lens configured to project a plurality of charged particle beams onto a sample, the objective lens having a sample-facing surface defining a plurality of beam apertures through which respective ones of the charged particle beams are emitted toward the sample; and a plurality of capture electrodes adjacent respective ones of the beam apertures and configured to capture charged particles emitted from the sample.

A particle beam system includes: a particle source to generate a beam of charged particles; a first multi-lens array including a first multiplicity of individually adjustable and focusing particle lenses so that at least some of the particles pass through openings in the multi-lens array in the form of a plurality of individual particle beams; a second multi-aperture plate including a multiplicity of second openings downstream of the first multi-lens array so that some of the particles which pass the first multi-lens array impinge on the second multi-aperture plate and some of the particles which pass the first multi-lens array pass through the openings in the second multi-aperture plate; and a controller configured to supply an individually adjustable voltage to the particle lenses of the first multi-lens array and thus individually adjust the focusing of the associated particle lens for each individual particle beam.

Charged particle beam systems and methods, such as a multi beam charged particle beam system and related methods, can compensate sample charging.

Provided herein are approaches for reducing particles in an ion implanter. In some embodiments, an electrostatic filter of the ion implanter may include a housing and a plurality of conductive beam optics within the housing, the plurality of conductive beam optics arranged around an ion beam-line. At least one conductive beam optic of the plurality of conductive beam optics may include a conductive core element, a resistive material disposed around the conductive core, and a conductive layer disposed around the resistive material.

Provided herein are approaches for reducing particles in an ion implanter. In some embodiments, an electrostatic filter of the ion implanter may include a housing and a plurality of conductive beam optics within the housing, the plurality of conductive beam optics arranged around an ion beam-line. At least one conductive beam optic of the plurality of conductive beam optics may include a conductive core element, a resistive material disposed around the conductive core, and a conductive layer disposed around the resistive material.

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 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 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 charged particle multi-beam device includes a charged particle source, a collimator lens, a multi-light-source forming unit, and a reduction projection optical system. The multi-light-source forming unit has first to third porous electrodes disposed side by side in an optical axis direction. A plurality of holes for causing the multi-beams to pass is formed in each of the first to third porous electrodes. The first porous electrode and the third porous electrode have the same potential and the second porous electrode has potential different from the potential of the first porous electrode and the third porous electrode. A diameter of the holes on the second porous electrode is formed larger further away from an optical axis such that a surface on which the multi-light sources are located is formed in a shape convex to the charged particle source side.