The purpose of the present invention is to provide a charged-particle beam device capable of stable performance of processes such as a measurement or test, independent of fluctuations in sample electric electric potential or the like. To this end, this charged-particle beam device comprises an energy filter for filtering the energy of charged particles released from the sample and a deflector for deflecting the charged particles released from the sample toward the energy filter. A control device generates a first image on the basis of the output of a detector, adjusts the voltage applied to the energy filter so that the first image reaches a prescribed state, and calculates deflection conditions for the deflector on the basis of the post-adjustment voltage applied to the energy filter.

A charged particle system may include a first charged particle beam source provided on a first axis, and a second charged particle beam source provided on a second axis. There may also be provided a deflector arranged on the first axis. The deflector may be configured to deflect a beam generated from the second charged particle beam source toward a sample. A method of operating a charged particle beam system may include switching between a first state and a second state of operating a deflector. In the first state, a first charged particle beam generated from a first charged particle beam source may be blanked and a second charged particle beam generated from a second charged particle beam source may be directed toward a sample. In the second state, the second charged particle beam may be blanked and the first charged particle beam may be directed toward the sample.

Systems and methods for conducting charged particle beam modulation are disclosed. According to certain embodiments, a charged particle beam apparatus generates a plurality of charged particle beams. A modulator may be configured to receive the plurality of charged particle beams and generate a plurality of modulated charged particle beams. A detector may be configured to receive the plurality of modulated charged particle beams.

A scanning transmission electron microscope is adapted to acquire high quality precession electron diffraction (PED) patterns by means of separated scanning deflectors and precession deflectors. Magnetic or electrostatic deflectors may be used for scanning and for precession. This enables independent optimization of parameters for each deflection system to achieve a broad operating range simultaneously for both deflection systems.

An electron microscope system and a method of measuring an aberration of the electron microscope system are disclosed. A method of controlling an aberration of an electron microscope includes obtaining a dispersed energy distribution for electrons at a diffraction plane of the electron microscope and placing an aperture at a selected location of the dispersed energy distribution in the diffraction plane. The method measures displacement of an image of the aperture in an image plane of the electron microscope for the selected location of the aperture. The method determines an aberration coefficient of the electron microscope from the measured displacement and the selected location of the aperture and alters a parameter of an element of the electron microscope to control the aberration of the electron microscope based at least in part on the determined aberration coefficient.

The present invention enlarges a range of movement of field of view by beam deflection with a simple deflector configuration and suppresses deterioration of a signal electron detection rate caused by the beam deflection. A scanning electron microscope according to the present invention is provided with a first deflection field setting module that sets plural deflectors to move a scanning area on a specimen by a primary electron beam to a position deviated from an axis extended from an electron source toward the center of an objective lens and a second deflection field setting module that sets the plural deflectors so that trajectories of signal electrons are corrected without changing the scanning area set by the first deflection field setting module. The control unit controls the plural deflectors by adding a setting value set by the second deflection field setting module to a setting value set by the first deflection field setting module.

A charged particle beam device includes a deflection unit that deflects a charged particle beam released from a charged particle source to irradiate a sample, a reflection plate that reflects secondary electrons generated from the sample, and a control unit that controls the deflection unit based on an image generated by detecting the secondary electrons reflected from the reflection plate. The deflection unit includes an electromagnetic deflection unit that electromagnetically scans with the charged particle beam by a magnetic field and an electrostatic deflection unit that electrostatically scans with the charged particle beam by an electric field. The control unit controls the electromagnetic deflection unit and the electrostatic deflection unit, superimposes an electromagnetic deflection vector generated by the electromagnetic scanning and an electrostatic deflection vector generated by the electrostatic scanning, and controls at least a trajectory of the charged particle beam.

A multi-electron beam image acquiring apparatus includes a stage configured to mount thereon a substrate, an illumination optical system configured to apply multiple primary electron beams to the substrate, a plurality of multipole lenses including at least two stages of multipole lenses, arranged at positions common to a trajectory of the multiple primary electron beams and a trajectory of multiple secondary electron beams which are emitted because the substrate is irradiated with the multiple primary electron beams and each configured to include at least four electrodes and at least four magnetic poles, and a multi-detector configured to detect the multiple secondary electron beams separated from the trajectory of the multiple primary electron beams, wherein one of the plurality of multipole lenses separates the multiple secondary electron beams from the trajectory of the multiple primary electron beams.

Apparatus and methods for directing a beam of primary electrons along a primary beam path onto a sample are disclosed. In one arrangement, a beam separator diverts away from the primary beam path a beam of secondary electrons emitted from the sample along the primary beam path. A dispersion device is upbeam from the beam separator. The dispersion device compensates for dispersion induced in the primary beam by the beam separator. One or more common power supplies drive both the beam separator and the dispersion device.

In a first cross section along an electron ray that passes between an inner curved surface and an outer curved surface of a beam bender, the curvature of the surfaces are fixed, and the center of the curvature of the surfaces are set so as to match each other. In a second cross section perpendicular to the electron ray, the curvature of the surfaces are fixed, and the center of curvature of the surfaces are set so as to match each other. The radius of the curvature of the surface in the second cross section is set to be larger than that of the surface in the first cross section. The radius of curvature of the surface in the second cross section is set to be larger than that of the surface in the first cross section.