When a charged particle beam aperture having an annular shape is used, since a charged particle beam directly above the optical axis having the highest current density in the charged particle beam is blocked, it is difficult to dispose the charged particle beam aperture at an optimal mounting position. An charged particle beam apparatus includes a charged particle beam source that generates a charged particle beam, a charged particle beam aperture, a charged particle beam aperture power supply that applies a voltage to the charged particle beam aperture, an objective lens for focusing the charged particle beam on a sample, a detector that detects secondary charged particles emitted by irradiating the sample with the charged particle beam, a computer that forms a charged particle beam image based on the secondary charged particles detected by the detector, in which the position of the charged particle beam aperture is set so that the charged particle beam image does not move and changes concentrically in synchronization with the AC voltage, in a state where an AC voltage is applied to the charged particle beam aperture by the charged particle beam aperture power supply.

When using a charged particle beam aperture having a ring shape in a charged particle beam device, the charged particle beam with the highest current density immediately above the optical axis, among the charged particle beams is blocked, so that it is difficult to dispose the charged particle beam aperture at the optimal mounting position. Therefore, in addition to the ring-shaped charged particle beam aperture, a hole-shaped charged particle beam aperture is provided, and it is possible to switch between the case where the ring-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam and the case where the hole-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam.

As a device for correcting positive spherical aberration of an electromagnetic lens for a charged particle beam, a spherical aberration correction device combining a hole electrode and a ring electrode is known. In this spherical aberration correction device, when a voltage is applied between the hole electrode and the ring electrode, the focus of the charged particle beam device changes due to the convex lens effect generated in the hole electrode. Therefore, in a charged particle beam device including a charged particle beam source which generates a charged particle beam, a charged particle beam aperture having a ring shape, and a charged particle beam aperture power supply which applies a voltage to the charged particle beam aperture, the charged particle beam aperture power supply is configured to apply, to the charged particle beam aperture, a voltage having a polarity opposite to a polarity of charges of the charged particle beam.

The invention relates to a multi-beam pattern definition device for use in a particle-beam processing or inspection apparatus, said device being adapted to be irradiated with a beam of electrically charged particles and allow passage of the beam through a plurality of apertures thus forming a corresponding number of beamlets, said device comprising an aperture array device in which at least two sets of apertures are realized, an opening array device located downstream of the aperture array device having a plurality of openings configured for the passage of beamlets, said opening array device comprises impact regions, wherein charged impinge upon said impact regions.

Systems and methods of providing a probe spot in multiple modes of operation of a charged-particle beam apparatus are disclosed. The method may comprise activating a charged-particle source to generate a primary charged-particle beam and selecting between a first mode and a second mode of operation of the charged-particle beam apparatus. In the flooding mode, the condenser lens may focus at least a first portion of the primary charged-particle beam passing through an aperture of the aperture plate to form a second portion of the primary charged-particle beam, and substantially all of the second portion is used to flood a surface of a sample. In the inspection mode, the condenser lens may focus a first portion of the primary charged-particle beam such that the aperture of the aperture plate blocks off peripheral charged-particles to form the second portion of the primary charged-particle beam used to inspect the sample surface.

The present disclosure relates to a collimator. The collimator may include a motor, a transmission unit having a first end and a second end, and a leaf unit having a leaf. The first end of the transmission unit may be connected to the motor and the second end of the transmission unit may be connected to the leaf. The present disclosure also relates to a collimator system. The collimator system may include a leaf module having a leaf, a driving module having a motor configured to drive the leaf, and a processing module to generate a movement profile of the leaf. The movement profile of the leaf may include a first speed during a first stage, a second speed of the leaf during a second stage, and a third speed of the leaf during a third stage.

As a device for correcting positive spherical aberration of an electromagnetic lens for a charged particle beam, a spherical aberration correction device combining a hole electrode and a ring electrode is known. In this spherical aberration correction device, when a voltage is applied between the hole electrode and the ring electrode, the focus of the charged particle beam device changes due to the convex lens effect generated in the hole electrode. Therefore, in a charged particle beam device including a charged particle beam source which generates a charged particle beam, a charged particle beam aperture having a ring shape, and a charged particle beam aperture power supply which applies a voltage to the charged particle beam aperture, the charged particle beam aperture power supply is configured to apply, to the charged particle beam aperture, a voltage having a polarity opposite to a polarity of charges of the charged particle beam.

Provided is a transmission electron microscope capable of obtaining a hollow-cone dark-field image and visually displaying irradiation conditions thereof. The transmission electron microscope is provided with an irradiation unit for irradiating a specimen with an electron beam, an objective lens for causing the electron beam transmitted through the specimen to form an image, beam deflectors for deflecting the electron beam, said beam deflectors being positioned higher than a position where the specimen is to be placed, an objective movable aperture for passing only a portion of the electron beam transmitted through the specimen, and a deflection coil control unit. The deflection coil control unit controls a deflection angle of the electron beam using the beam deflectors such that the specimen is irradiated with the electron beam at a predetermined angle with respect to an optical axis while the electron beam is moving in a precessional manner and such that only a diffracted wave and/or a scattered wave having a desired angle among diffracted waves and/or scattered waves generated when the electron beam is transmitted through the specimen passes through the objective movable aperture.

A multiple-charged particle-beam irradiation apparatus includes a shaping aperture array substrate that causes a charged particle beam to pass through a plurality of first apertures to form multi-beams, a plurality of blanking aperture array substrates each provided with a plurality of second apertures, which enable corresponding beams to pass, and including a blanker arranged at each of the second apertures, a movable table on which the blanking aperture array substrates are mounted so as to be spaced apart from each other in a second direction, which is orthogonal to a first direction along an optical axis, and that moves in the second direction to position one of the blanking aperture array substrates on the optical axis, and an alignment mechanism that performs an alignment adjustment between the blanking aperture array substrate on the optical axis and the shaping aperture array substrate.

Disclosed herein are approaches for adjusting extraction slits of an extraction plate using a set of adjustable beam blockers. In one approach, an ion extraction optics may include an extraction plate including a first opening and a second opening, and a first beam blocker extending over the first opening and a second beam blocker extending over the second opening. Each of the first and second beam blockers may include an inner slit defined by a first distance between an inner edge and the extraction plate, and an outer slit defined by a second distance between an outer edge and the extraction plate, wherein the first and second beam blockers are movable to vary at least one of the first distance and the second distance. As a result, extraction through the inner and outer slits of ion beamlets characterized by similar mean angles may be achieved.