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 method of detecting a defect in a device using a charged particle beam includes inputting a charged particle beam condition, a light condition, and electronic device circuit information, controlling a charged particle beam applied to a sample based on the electron beam condition, controlling light applied to the sample based on the light condition, detecting second electrons emitted from the sample by the application of the charged particle beam and the light, and generating a calculation netlist based on the electronic device circuit information, generating a light irradiation netlist based on the calculation netlist and the light condition, estimating a first irradiation result when the charged particle beam and the light are applied to the sample based on the light irradiation netlist and the charged particle beam condition, and comparing the first irradiation result with a second irradiation result when the charged particle beam and the light are actually applied to the sample based on the electron beam condition.

A structure for grounding an extreme ultraviolet mask (EUV mask) is provided to discharge the EUV mask during the inspection by an electron beam inspection tool. The structure for grounding an EUV mask includes at least one grounding pin to contact conductive areas on the EUV mask, wherein the EUV mask may have further conductive layer on sidewalls or/and back side. The inspection quality of the EU mask is enhanced by using the electron beam inspection system because the accumulated charging on the EUV mask is grounded. The reflective surface of the EUV mask on a continuously moving stage is scanned by using the electron beam simultaneously. The moving direction of the stage is perpendicular to the scanning direction of the electron beam.

Systems and methods of observing a sample using an electron beam apparatus are disclosed. The electron beam apparatus comprises an electron source configured to generate a primary electron beam along a primary optical axis, and a first electron detector having a first detection layer substantially parallel to the primary optical axis and configured to detect a first portion of a plurality of signal electrons generated from a probe spot on a sample. The method may comprise generating a plurality of signal electrons and detecting the signal electrons using the first electron detector substantially parallel to the primary optical axis of the primary electron beam. A method of configuring an electrostatic element or a magnetic element to detect backscattered electrons may include disposing an electron detector on an inner surface of the electrostatic or magnetic element and depositing a conducting layer on the inner surface of the electron detector.

The present invention relates to a scanning electron microscope configured to scan a workpiece, such as a wafer, mask, panel, or substrate, with an electron beam to generate an image of the workpiece. The scanning electron microscope includes a deflector (17, 18) configured to deflect the electron beam to scan a target region (T) on the workpiece (W) with the electron beam, and a deflection controller (22) configured to apply to the deflectors (17, 18) a scanning voltage that causes the electron beam to scan the target region (T) and an offset voltage that shifts the electron beam from an optical axial center (O) to the target region (T).

The present invention has been made in view of the above problems, and an object thereof is to provide a charged particle beam device capable of improving the reproducibility of the magnetic field response of a magnetic field lens and realizing highly-accurate electron orbit control in a short time. A charged particle beam device according to the present invention generates an excitation current of a magnetic field lens by combining a direct current with an alternating current (see FIG. 6A).

Some embodiments are related to a method of or apparatus for forming an image of a buried structure that includes: emitting primary charged particles from a source; receiving a plurality of secondary charged particles from a sample; and forming an image based on received secondary charged particles that have an energy within a first range.

In one embodiment, an electron beam inspection apparatus includes an optical system irradiating a substrate with primary electron beams, a beam separator separating, from the primary electron beams, secondary electron beams emitted as a result of irradiating the substrate with the primary electron beams, a detector detecting the secondary electron beams separated, a movable stage on which the substrate is placed, a support base supporting the substrate on the stage, and an applying unit applying a first voltage to the substrate. The support base includes a plurality of support pins that support the substrate from below. The support pins each include a columnar insulator and a metal film disposed in the insulator. A second voltage is applied to the metal film.

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 for projecting a plurality of secondary charged-particle beams from a sample onto a charged-particle detector. The electro-optical system may include a first pre-limit aperture plate comprising a first aperture configured to block peripheral charged-particles of the plurality of secondary charged-particle beams, and a beam-limit aperture array comprising a second aperture configured to trim the plurality of secondary charged-particle beams. The charged-particle detector may include a plurality of detection elements, wherein a detection element of the plurality of detection elements is associated with a corresponding trimmed beam of the plurality of secondary charged-particle beams.

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.