A scanning electron microscope includes: a retarding power source configured to apply a retarding voltage to a specimen; a combined objective lens configured to focus the primary beam on a surface of the specimen; an electrostatic deflection system configured to deflect the primary beam to direct the primary beam to each point in a field of view on the surface of the specimen; a first scintillation detector having a first scintillator configured to emit light upon incidence of secondary electrons which have been emitted from the specimen; a Wien filter configured to deflect the secondary electrons in one direction without deflecting the primary beam; and a second scintillation detector having a second scintillator configured to detect the secondary electrons deflected by the Wien filter. The second scintillator has a distal end located away from the axis of the primary beam.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.

Embodiments consistent with the disclosure herein include methods and a multi-beam apparatus configured to emit charged-particle beams for imaging a top and side of a structure of a sample, including: a deflector array including a first deflector and configured to receive a first charged-particle beam and a second charged-particle beam; a blocking plate configured to block one of the first charged-particle beam and the second charged-particle beam; and a controller having circuitry and configured to change the configuration of the apparatus to transition between a first mode and a second mode. In the first mode, the deflector array directs the second charged-particle beam to the top of the structure, and the blocking plate blocks the first charged-particle beam. And in the second mode, the first deflector deflects the first charged-particle beam to the side of the structure, and the blocking plate blocks the second charged-particle beam.

A fine-adjustable charged particle lens comprises a magnetic circuit assembly including permanent magnets, a yoke body, and a shunting device comprising a shunting component, and this assembly surrounds a beam passage extending along the longitudinal axis (cx). The shunting device is placed in the yoke body besides the permanent magnets and may be composed of several sector components, comprising different high magnetically permeable materials. The permanent magnet and the yoke body form a magnetic circuit having at least two gaps, in order to generate a magnetic field reaching inwards into the beam passage, into which a sleeve insert having electrostatic electrodes can be inserted, which may also generate an electric field spatially overlapping said magnetic field. The shunting device partially bypasses the magnetic flux of said circuit assembly and thus reduces the magnetic field to a desired value.

A method of forming a plasma processing apparatus comprises providing a chamber, the chamber including a wall defining an interior, and a viewport extending through the wall. An analysis apparatus connected to the viewport may be formed. The analysis apparatus includes an analyzer adjacent to the chamber, a probe connected to the analyzer and aligned with the viewport, and a first window aligned with the probe, the first window having a first surface, and a second surface at an opposite side relative to the first surface, the second surface being exposed to the interior of the chamber, and the second surface of the first window has a scattering surface.

An electron-beam device includes a laser and a photocathode film. The photocathode film has a front side and a back side and emits a plurality of electron beamlets when illuminated from the back side using the laser. The electron-beam device also includes electrodes to extract the plurality of electron beamlets from the front side of the photocathode film and to control shapes of the plurality of electron beamlets.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.

A scanning electron microscope objective lens system is disclosed, which includes: a magnetic lens, a deflection device, a deflection control electrode, specimen to be observed, and a detection device; in which, The opening of the pole piece of the magnetic lens faces to the specimen; the deflection device is located in the magnetic lens, which includes at least one sub-deflector; the deflection control electrode is located between the detection device and the specimen, and the deflection control electrode is used to change the direction of the primary electron beam and the signal electrons generating from the specimen; the detection device comprises the first sub-detector for detecting the back-scattered electrons and the second sub-detector for detecting the second electrons. A specimen detection method is also disclosed.

A multi-beam charged particle system includes: a vacuum enclosure having an opening covered by a door; a particle source configured to generate charged particles, wherein the particle source is arranged within the vacuum enclosure; at least one multi-aperture plate module including at least one multi-aperture plate and a base; and a transfer box having an opening covered by a door. The at least one multi-aperture plate includes a plurality of apertures. The base is configured to hold the at least one multi-aperture plate. The base is configured to be fixed relative to the vacuum enclosure such that the multi-aperture plate module is arranged in an interior of the vacuum enclosure such that, during operation of the particle beam system, particles traverse the plural multi-aperture plates through the apertures of the plates.

A transmission electron microscope includes an electron beam source emitting an electron beam and an illumination optical system for directing the emitted electron beam at a sample. The illumination optical system has a first condenser lens, a second condenser lens, a third condenser lens, a fourth condenser lens, an objective lens, and a condenser aperture disposed at the position of the second condenser lens. The third condenser lens and the fourth condenser lens cooperate to make the position of the condenser aperture and a sample plane conjugate to each other. The first condenser lens and the second condenser lens cooperate to make the electron beam source and a front focal plane of the objective lens conjugate to each other while the conjugate relationship between the position of the condenser aperture and the sample plane is maintained by the third and fourth condenser lenses.