Provided is a charged particle beam device that enables, even if a visual field includes therein a plurality of regions having different secondary electron emission conditions, the setting of appropriate energy filter conditions adapted to each of these regions. The charged particle beam device is equipped with a detector for detecting charged particles obtained on the basis of scanning, over a sample, a charged particle beam emitted from a charged particle source, and an energy filter for filtering by energy the charged particles emitted from the sample. Index values are determined for the plurality of regions contained within the scanning region of the charged particle beam, and, for each of a plurality of energy filter conditions, differences are calculated between the plurality of index values and the reference index values that have been set for each of the plurality of regions.

In an electron beam device provided with two columns including an irradiation optical system and an imaging optical system, a photoelectron image for use in adjusting the irradiation optical system is made sharper. The electron beam device includes: an irradiation optical system which irradiates a sample placed on a stage with an electron beam; a light irradiation unit 50 which irradiates the sample with light containing ultraviolet rays; a sample voltage control unit 44 which applies a negative voltage to the sample so that, before the electron beam reaches the sample, the electron orbit inverts; and an imaging optical system which acquires a mirror electron image by forming an image of mirror electrons reflected by application of the negative voltage. In the electron beam device, the imaging optical system includes a sensor 32 which obtains a mirror electron image and a stray light suppression part 27 which is provided between the sensor and the stage 31 and which suppresses reaching the sensor of the light emitted from the light irradiation unit.

In an electron beam device provided with two columns including an irradiation optical system and an imaging optical system, a photoelectron image for use in adjusting the irradiation optical system is made sharper. The electron beam device includes: an irradiation optical system which irradiates a sample placed on a stage with an electron beam; a light irradiation unit 50 which irradiates the sample with light containing ultraviolet rays; a sample voltage control unit 44 which applies a negative voltage to the sample so that, before the electron beam reaches the sample, the electron orbit inverts; and an imaging optical system which acquires a mirror electron image by forming an image of mirror electrons reflected by application of the negative voltage. In the electron beam device, the imaging optical system includes a sensor 32 which obtains a mirror electron image and a stray light suppression part 27 which is provided between the sensor and the stage 31 and which suppresses reaching the sensor of the light emitted from the light irradiation unit.

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.

A device may include an electron source, a detector, and a deflector. The electron source may be directed toward a sample area. The detector may receive an electron signal or an electron-induced signal. A deflector may be positioned between the electron source and the sample. The deflector may modulate an intensity of the electron source directed to the sample area according to an electron dose waveform having a continuously variable temporal profile.

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.

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.

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.

An analysis system, an analysis method and a sample holder make it possible to analyse a battery via a particle beam system, for example to record images of the battery via the particle beam system, while the battery is arranged in a vacuum chamber of the particle beam system and is manipulated according to a multiplicity of different parameter value sets in the vacuum chamber. By way of example, the battery is kept at a predefined temperature, a predefined pressure is exerted on the battery, and the battery is electrically charged and discharged according to a loading scheme and at the same time images of the battery are recorded via the particle beam system.

A system for performing surface analysis on a material, includes a pulsed electron source that forms a monochromatic beam of incident electrons; means for conveying the incident electrons to the surface of a sample of material, so as to form backscattered electrons, and the backscattered electrons to detecting means, the conveying means comprising at least one electron optical system; means for detecting the backscattered electrons; the pulsed electron source comprising: a source of atoms; a continuous-wave laser beam configured to form a laser excitation zone able to excite the atoms to Rydberg states; a pulsed electric field on either side of the laser excitation zone, the pulsed electric field being configured to ionize at least the excited atoms and to form a monochromatic beam of electrons.