A method of operating a charged particle beam device is disclosed, including passing each of a plurality of beamlets through a deflector and a scanner, in that order. Each of the beamlets is focused with an objective lens on a sample to form a plurality of focal spots, forming an array. A first beamlet is focused on a first spot and a second beamlet is focused on a second spot. In a centered configuration of the device, each of the plurality of beamlets is directed by the deflector toward a coma free point. In a beamlet-displaced configuration of the device, the scanner is scanned such that the first beamlet passes through an acceptable aberrations point, the first beamlet scanning a displaced first field of view; and the first spot is displaced from the regular first focal spot to a displaced first focal spot.

A method of operating a charged particle beam device is disclosed, including passing each of a plurality of beamlets through a deflector and a scanner, in that order. Each of the beamlets is focused with an objective lens on a sample to form a plurality of focal spots, forming an array. A first beamlet is focused on a first spot and a second beamlet is focused on a second spot. In a centered configuration of the device, each of the plurality of beamlets is directed by the deflector toward a coma free point. In a beamlet-displaced configuration of the device, the scanner is scanned such that the first beamlet passes through an acceptable aberrations point, the first beamlet scanning a displaced first field of view; and the first spot is displaced from the regular first focal spot to a displaced first focal spot.

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 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 low voltage scanning electron microscope is disclosed, which includes: an electron source configured to generate an electron beam; an electron beam accelerator configured to accelerate the electron beam; a compound objective lens configured to converge the electron beams accelerated by the electron beam accelerator; a deflection device arranged between the inner wall of the magnetic lens and the optical axis of the electron beam and configured to deflect the electron beam; a detection device comprising a first sub-detection device for receiving secondary and backscattered electrons from the specimen, a second sub-detection device for receiving backscattered electrons, and a control device for changing the trajectories of the secondary electrons and the backscattered electrons; an electrostatic lens comprising the second sub-detection device, a specimen stage, and a control electrode for reducing the moving speed of the electron beam and changing the moving directions of the secondary and the backscattered electrons.

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.

The present invention relates to a charged particle beam apparatus enabling a selection of a charged particle beam in a specified energy range by symmetrically arranging cylindrical electrostatic lenses deflecting a path of the charged particle beam and disposing an energy selection aperture between the cylindrical electrostatic lenses. Since an integral structure in which a central electrode and a plurality of electrodes that are arranged at a front portion and a rear portion in relation to the central electrode of a monochromator are fixed to each other through insulator, is applied, a mechanism for adjusting an offset with respect to an optical axis is simplified as compared to the case of separately providing the lenses at the front portion and the rear portion, respectively, and a secondary aberration is canceled in an exit plane due to symmetry of an optical system.

In one embodiment, a charged particle beam writing apparatus includes a writer writing a pattern on a substrate on a stage with a charged particle beam, a mark substrate disposed on the stage and having a mark, an irradiation position detector detecting an irradiation position of the charged particle beam on a mark surface, a height detector detecting a surface height of the substrate and the mark substrate, a drift correction unit calculating an amount of drift correction, and a writing control unit correcting the irradiation position of the charged particle beam by using the amount of drift correction. The mark substrate has a pattern region with a plurality of marks and a non-pattern region with no pattern therein, and at least part of the non-pattern region is disposed between different portions of the pattern region. The height detector detects a height of a detection point in the non-pattern region.

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 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.