Apparatuses, systems, and methods for beam array geometry optimization of a multi-beam inspection tool are disclosed. In some embodiments, a microelectromechanical system (MEMS) may include a first row of apertures; a second row of apertures positioned below the first row of apertures; a third row of apertures positioned below the second row of apertures; and a fourth row of apertures positioned below the third row of apertures; wherein the first, second, third, and fourth rows are parallel to each other in a first direction; the first and third rows are offset from the second and fourth rows in a second direction that is perpendicular to the first direction; the first and third rows have a first length; the second and fourth rows have a second length; and the first length is longer than the second length in the second direction.

Provided is a charged particle beam device for which deterioration in throughput in the event of abnormality of multiple beams can be prevented. The charged particle beam device includes: a stage 11 on which a sample is mounted; a charged particle optical system configured to irradiate the sample with multiple beams including multiple primary beams; a detector 15 configured to detect secondary beams generated by interactions between the primary beams and the sample and output detection signals; and a control unit 17 configured to control the stage and the charged particle optical system to generate image data based on the detection signals from the detector obtained by scanning the sample with the multiple beams using a first scanning method. The control unit changes, when the abnormality of the multiple beams is detected based on the image data, the multiple beams to scan the sample using a second scanning method, and a scanning width of the multiple beams for scanning the sample is greater in the second scanning method than in the first scanning method.

A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.

A multiple electron beam image acquisition method includes performing scanning with a representative secondary electron beam emitted, based on temporary secondary electron beam deflection conditions, for each of plural positions in a primary electron beam deflection range of a representative primary electron beam, acquiring plural coordinates corresponding to the plural positions, based on detected images of the representative secondary electron beam, each detected at any one of the plural positions in the primary electron beam deflection range of the representative primary electron beam, and calculating, using the plural coordinates acquired, secondary electron beam deflection conditions to cancel movement of the representative secondary electron beam due to movement of the representative primary electron beam in the primary electron beam deflection range of the representative primary electron beam and to fix the irradiation position of the representative secondary electron beam to the predetermined detection element.

When contamination or local electrification is generated during acquisition of a low-magnification image, if a high-magnification image contains both a portion in which the contamination or local electrification is generated and a portion in which the contamination or local electrification is not generated, a region whose image quality has changed due to the contamination or local electrification is erroneously recognized as a defect. Thus, defect detection fails or it may be impossible to correctly determine the feature quantity of a defect. The invention provides a defect observation system that acquires sample images at a low magnification and a high magnification, and sets the position or size of the field of view of the high-magnification image or the electron beam irradiation range during acquisition of the low-magnification image no that the image acquired at the high magnification does not contain the outer edge of the image acquired at the low magnification.

Systems and methods of enhancing imaging resolution by reducing crosstalk between detection elements of a secondary charged-particle detector in a multi-beam apparatus are disclosed. The multi-beam apparatus may comprise an electro-optical system comprising a beam-limit aperture plate having a surface substantially perpendicular to an optical axis, the beam-limit aperture plate comprising a first aperture at a first distance relative to the surface of the beam-limit aperture plate, and a second aperture at a second distance relative to the surface of the beam-limit aperture plate, the second distance being different from the first distance. The first aperture may be a part of a first set of apertures of the beam-limit aperture plate at the first distance, and the second aperture may be a part of a second set of apertures of the beam-limit aperture plate at the second distance.

In order to allow detecting backscattered electrons (BSEs) generated from the bottom of a hole for determining whether a hole with a super high aspect ratio is opened or for inspecting and measuring the ratio of the top diameter to the bottom diameter of a hole, which are typified in 3D-NAND processes of opening a hole, a primary electron beam accelerated at a high accelerating voltage is applied to a sample. Backscattered electrons (BSEs) at a low angle (e.g. a zenith angle of five degrees or more) are detected. Thus, the bottom of a hole is observed using “penetrating BSEs” having been emitted from the bottom of the hole and penetrated the side wall. Using the characteristics in which a penetrating distance is relatively prolonged through a deep hole and the amount of penetrating BSEs is decreased to cause a dark image, a calibration curve expressing the relationship between a hole depth and the brightness is given to measure the hole depth.

Provided are an inspection device that detects with high precision and classifies surface unevenness, step batching, penetrating blade-shaped dislocations, penetrating spiral dislocations, basal plane dislocations, and stacking defects formed in an SiC substrate and an epitaxial layer; and a system. In the inspection device using charged particle beams, a device is used that has an electrode provided between a sample and an objective lens, the device applies a positive or negative voltage to the electrode and obtains images. A secondary electron emission rate is measured and energy EL and EH for the charged particles are found. A first image is obtained using the EH and positive potential conditions. A second image is obtained using the EL and negative potential conditions. A third image is obtained at the same position as the second image, and by using the EL and positive potential conditions.

Proposed is a charged particle beam apparatus for the purpose of detecting a charged particle emitted from a sample in a specific direction by discriminating between the charged particle and a charged particle emitted in another direction. As one aspect of achieving the above purpose, proposed is a charged particle beam apparatus including an objective lens configured to focus a beam emitted from a charged particle source, a detector (8) configured to detect at least one of a first charged particle (23) emitted from a sample by irradiating the sample with the beam and a second charged particle emitted from a charged particle collided member by causing the first charged particle to collide with the charged particle collision member disposed on a trajectory of the first charged particle, and an electrostatic lens (12) including a plurality of electrodes disposed between the objective lens and the detector, in which the electrostatic lens is a Butler type.

A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.