A charged particle detector with high detection efficiency is presented in this patent. This charged particle detector contains a grid electrode used for attracting charged particles, a convertor with the shape of particle entrance area smaller than the particle exit area, which is used for converging charged particles and converting ions into electrons in the ion detection mode, an electron detection unit used for detecting secondary electrons and amplifying the signal detected, and a metal shielding. This optimized detector has a simple construction, is easy to assemble and has a low manufacturing cost.

According to various embodiments, an inspection device may include a chamber, a stage provided within the chamber, an electron emitter, a laser emitter, and a conductive probe. The stage may be configured to hold a sample. The electron emitter may be configured to emit an electron beam towards the stage, to generate a first electrical signal in the sample. The laser emitter may be configured to emit a laser beam towards the stage, to generate a second electrical signal in the sample. The conductive probe may be configured to receive from the conductive structure, at least one of the first electrical signal and the second electrical signal.

The present invention relates to a sensor for electron detection emitted from an object to be used with a charged particle beam column being operated at a certain column and wafer voltage. The sensor is configured and operable to at least reduce interaction of negative ions with the active area of the sensor while minimizing electrons energy loss. The sensor is also configured and operable to minimize both gradual degradation of a cathodoluminescence efficiency of the active area and dynamic change of cathodoluminescence generated during operation of the sensor and evolving throughout the scintillator's lifetime.

Disclosed herein are CPM support systems, as well as related apparatuses, methods, computing devices, and computer-readable media. For example, in some embodiments, a charged particle microscope computational support apparatus may include: first logic to, for each angle of a plurality of angles, receive an associated image of a specimen at the angle, and generate an associated scan mask based on one or more regions-of-interest in the associated image; second logic to, for each angle of the plurality of angles, generate an associated data set of the specimen by processing data from a scan, in accordance with the associated scan mask, by a charged particle microscope of the specimen at the angle; and third logic to provide, for each angle of the plurality of angles, the associated data set of the specimen to reconstruction logic to generate a three-dimensional reconstruction of the specimen.

A method of measuring a critical dimension (CD) includes forming a plurality of patterns in a substrate, creating first to n-th images, where n is a natural number greater than 1, for first to n-th areas in the substrate, respectively, where the first to n-th areas do not overlap with each other, where each of the first to n-th areas comprising at least some of the plurality of patterns, creating a merged image for the first to n-th images, and measuring a CD for a measurement object from the plurality of patterns using the merged image. The merged image has a higher resolution than each of the first to n-th images.

The scanning charged particle beam microscope according to the present application is characterized in that, in acquiring an image of the FOV (field of view), interspaced beam irradiation points are set, and then, a deflector is controlled so that a charged particle beam scan is performed faster when the charged particle beam irradiates a position on the sample between each of the irradiation points than when the charged particle beam irradiates a position on the sample corresponding to each of the irradiation points (a position on the sample corresponding to each pixel detecting a signal). This allows the effects from a micro-domain electrification occurring within the FOV to be mitigated or controlled.

The objective of the present invention is to use brightness images acquired under different energy conditions to estimate the size of a defect in the depth direction in a simple manner. A charged-particle beam device according to the present invention determines the brightness ratio for each irradiation position on a brightness image while changing parameters varying the signal amount, estimates the position of the defect in the depth direction on the basis of the parameters at which the brightness ratio is at a minimum, and estimates the size of the defect in the depth direction on the basis of the magnitude of the brightness ratio (see FIG. 5).

The purpose of the present disclosure is to propose a charged particle beam device capable of allowing specifying of a distance between irradiation points for a pulsed beam and a time between irradiation points. Proposed is a charged particle beam device equipped with a beam column which has a scanning deflector for sweeping a beam and directs the beam swept by the scanning deflector onto a sample in pulses, wherein: the distance between irradiation points of the pulsed beam is set such that feature quantities of one or more specific regions of an image obtained on the basis of an output of a detector satisfy a predetermined state; the duration of time between irradiation points for the pulsed beam is changed when in a state in which the set distance between irradiation points is set or in a state in which multiple distances between irradiation points determined on the basis of the specified distance between irradiation points are set; and the beam emission is carried out according to the duration of time between irradiation points whereby the feature quantities of the multiple specific regions of the image obtained on the basis of the output of the detector satisfy the predetermined state.

We describe a super-resolution optical microscopy technique in which a sample is located on or adjacent to the planar surface of an aplanatic solid immersion lens and placed in a cryogenic environment.

A charged particle beam apparatus includes: an electromagnetic wave generation source 16 that generates an electromagnetic wave with which a sample is irradiated; a charged particle optical system that includes a pulsing mechanism 3 and irradiates the sample with a focused charged particle beam; a detector 10 that detects an emitted electron emitted by an interaction between the charged particle beam and the sample; a first irradiation control unit 15 that controls the electromagnetic wave generation source and irradiates the sample with a pulsed electromagnetic wave to generate an excited carrier; a second irradiation control unit 14 that controls the pulsing mechanism and irradiates an electromagnetic wave irradiation region of the sample with a pulsed charged particle beam; and a timing control unit 13. While the emitted electrons are detected by the detector in synchronization with irradiation of the pulsed charged particle beam, the timing control unit controls the first irradiation control unit and the second irradiation control unit, and controls an interval time between the pulsed electromagnetic wave and the pulsed charged particle beam to the electromagnetic wave irradiation region. As a result, based on a transient change in an electron emission amount, it is possible to detect sample information with nano spatial resolution.