Abstract: This inspection system 100 comprises: an electron source 102 which irradiates a sample 200 with an inspection beam; a detector 105 which detects secondary electrons obtained by irradiating the sample 200 with the inspection beam and outputs a detection signal; a laser device 107 which emits an action laser that changes the amount of secondary electrons; an electron gun 106 which emits an action electron beam that changes the amount of secondary electrons; and a computer system 140 which generates an image of the sample 200 on the basis of the detection signal.

Abstract: A charged particle beam device includes: a charged particle source configured to emit a charged particle beam to be emitted onto a sample; a deflector configured to deflect trajectories of a secondary electron and a reflected electron emitted from the sample; a reflected electron detector configured to detect the reflected electron; a control unit configured to acquire an observation image based on a detection signal output from the reflected electron detector and configured to control an operation of each unit; and an absorbing plate disposed between the deflector and the reflected electron detector and including a concave portion.

Abstract: Roughness measurement corrects a machine difference utilizing first PSD data indicating power spectral density of a line pattern measured for a line pattern formed on a wafer for machine difference management by a reference machine in roughness index calculation and second PSD data indicating power spectral density of a line pattern measured for the line pattern formed on the wafer for machine difference management by a correction target machine are used to obtain a correction method for correcting the power spectral density of the second PSD data to the power spectral density of the first PSD data, power spectral density of a line pattern is measured as third PSD data from a scanning image of the line pattern, and corrected power spectral density obtained by correcting the power spectral density of the third PSD data by the obtained correction method is calculated.

Abstract: The present disclosure pertains to a method, a system, and a computer-readable medium for highly precisely measuring the depth of a recess formed in a sample even when, inter alia, the material or pattern density of the sample differs. The method, system, and computer-readable medium involve: using a measurement tool to acquire an image or a brightness distribution of a region including a recess formed in a sample; extracting a first characteristic of the interior of the recess, and a second characteristic pertaining to the dimensions or area of the recess, from the acquired image or brightness distribution; and inputting the extracted first characteristic and second characteristic to a model that indicates the relationship between the first characteristic, the second characteristic, and a depth index of the recess to thereby derive the depth index of the recess.

Abstract: A charged particle optical system scans a sample with a pulsed charged particle beam and detects secondary charged particles; and a scan image is formed. Control is carried out so that a deflection signal for deflecting the charged particle beam in a first direction, a first timing for pulsed irradiation, a second timing for pulsed irradiation, and a third timing for detection of the secondary charged particles are synchronized. When the deflection amount of the charged particle beam in the time period of the first timing corresponds to the coordinates of n pixels in the scan image, the same line is scanned m times (m<n) while shifting the first timing with respect to the deflection signal so that a location irradiated with the charged particle beam by each scanning has different pixel coordinates. The pixel values at pixel coordinates where a signal is defective are restored.

Abstract: A multipole lens includes a hollow cylindrical non-magnetic bobbin provided with a plurality of slits, and a metal wire. The plurality of slits are disposed such that a central angle between adjacent slits is (360/12N)°, N being a natural number. Winding numbers of the metal wire in the plurality of slits are equal. When a cross section of the non-magnetic bobbin orthogonal to a longitudinal direction of the slits is divided into an even number of regions having an equal central angle and including two or more of the slits, directions in which the metal wire passes through the slits provided in the region are same, and a direction in which the metal wire passes through the slits provided in the adjacent region is reversed.

Abstract: The present disclosure provides a technique enabling accurate ascertaining of a charged state of a resist pattern resulting from irradiation of a charged particle beam. The present disclosure provides a charged particle beam system provided with: a charged particle device provided with a charged particle source, deflectors for causing a primary charged particle beam emitted from the charged particle source to be scanned over a sample, an energy discriminator for performing energy discrimination for secondary electrons emitted when the primary charged particle beam has reached the sample, and a detector for detecting secondary electrons which have passed the energy discriminator; and a computer system for generating a scan image on the basis of signal amounts detected by the detector, which fluctuate during scanning of primary charged particles by the deflectors, and storing the scan image into an image storage unit.

Abstract: A control device controls a contact probe in synchronization with a pulse-controlled light having a predetermined wavelength, a measurement instrument measures a characteristic of a sample to be inspected or an analysis sample, and a circuit constant or a defect structure of the sample to be inspected is estimated based on a circuit model created by an electric characteristic analysis device configured to generate the circuit model based on a value measured by the measurement instrument and a detection signal of secondary electrons detected by the charged particle beam device.

Abstract: An object of the invention is to provide a charged particle beam apparatus capable of acquiring an observation image having a high contrast in a sample whose light absorption characteristic depends on a light wavelength. The charged particle beam apparatus according to the invention irradiates the sample with light, generates an observation image of the sample, changes an irradiation intensity per unit time of the light, and then generates a plurality of the observation images having different contrasts.

Abstract: To provide a sample image observation device and a method that restore an image based on a sparsely sampled image and that can improve observation throughput and usability by maintaining a restored image quality constant regardless of a change in an observation condition. In a sample image observation device that irradiates a part of an observation area of the sample 19 with an electron beam and restores an image including a pixel not irradiated with the electron beam, the control system 22 includes a storage unit configured to store a correlation between an irradiation condition of irradiating the observation area of the sample with the electron beam and an observation condition of the sample, a control unit configured to synchronize an irradiation proportion of the electron beam with the observation condition based on the correlation, and an input unit configured to input sample information on the sample.

Abstract: This inspection system 100 comprises: an electron source 102 which irradiates a sample 200 with an inspection beam; a detector 105 which detects secondary electrons obtained by irradiating the sample 200 with the inspection beam and outputs a detection signal; a laser device 107 which emits an action laser that changes the amount of secondary electrons; an electron gun 106 which emits an action electron beam that changes the amount of secondary electrons; and a computer system 140 which generates an image of the sample 200 on the basis of the detection signal.

Abstract: An object of the invention is to provide a charged particle beam device capable of increasing the contrast of an observation image of a sample as much as possible in accordance with light absorption characteristics that change for each optical parameter. The charged particle beam device according to the invention changes an optical parameter such as a polarization plane of light emitted to the sample, and generates the observation image having a contrast corresponding to the changed optical parameter. An optical parameter that maximizes a light absorption coefficient of the sample is specified according to a feature amount of a shape pattern of the sample (refer to FIG. 5).

Abstract: A control device controls a contact probe in synchronization with a pulse-controlled light having a predetermined wavelength, a measurement instrument measures a characteristic of a sample to be inspected or an analysis sample, and a circuit constant or a defect structure of the sample to be inspected is estimated based on a circuit model created by an electric characteristic analysis device configured to generate the circuit model based on a value measured by the measurement instrument and a detection signal of secondary electrons detected by the charged particle beam device.

Abstract: A charged particle optical system scans a sample with a pulsed charged particle beam and detects secondary charged particles; and a scan image is formed. Control is carried out so that a deflection signal for deflecting the charged particle beam in a first direction, a first timing for pulsed irradiation, a second timing for pulsed irradiation, and a third timing for detection of the secondary charged particles are synchronized. When the deflection amount of the charged particle beam in the time period of the first timing corresponds to the coordinates of n pixels in the scan image, the same line is scanned m times (m < n) while shifting the first timing with respect to the deflection signal so that a location irradiated with the charged particle beam by each scanning has different pixel coordinates. The pixel values at pixel coordinates where a signal is defective are restored.

Abstract: Roughness measurement corrects a machine difference utilizing first PSD data indicating power spectral density of a line pattern measured for a line pattern formed on a wafer for machine difference management by a reference machine in roughness index calculation and second PSD data indicating power spectral density of a line pattern measured for the line pattern formed on the wafer for machine difference management by a correction target machine are used to obtain a correction method for correcting the power spectral density of the second PSD data to the power spectral density of the first PSD data, power spectral density of a line pattern is measured as third PSD data from a scanning image of the line pattern, and corrected power spectral density obtained by correcting the power spectral density of the third PSD data by the obtained correction method is calculated.

Abstract: A charged particle beam apparatus acquires an image that is not affected by movement of a stage at a high speed. The apparatus includes: a charged particle source for irradiating a sample with a charged particle beam; a stage on which the sample is placed; a measurement unit for measuring a movement amount of the stage; a deflector; a deflector offset control unit, which is a feedback control unit for adjusting a deflection amount of the deflector according to the movement amount of the stage; a plurality of detectors for detecting secondary charged particles emitted from the sample by irradiation of the charged particle beam; a composition ratio calculation unit that calculates composition ratios of signals output from the detectors based on the deflection amount adjusted by the feedback control unit; and an image generation unit for generating a composite image by compositing the signals using the composition ratio.

Abstract: A charged particle beam device capable of generating an image having uniform image quality in a field of view is provided.

Abstract: The present disclosure provides a technique enabling accurate ascertaining of a charged state of a resist pattern resulting from irradiation of a charged particle beam. The present disclosure provides a charged particle beam system provided with: a charged particle device provided with a charged particle source, deflectors for causing a primary charged particle beam emitted from the charged particle source to be scanned over a sample, an energy discriminator for performing energy discrimination for secondary electrons emitted when the primary charged particle beam has reached the sample, and a detector for detecting secondary electrons which have passed the energy discriminator; and a computer system for generating a scan image on the basis of signal amounts detected by the detector, which fluctuate during scanning of primary charged particles by the deflectors, and storing the scan image into an image storage unit.

Abstract: An object of the invention is to provide a charged particle beam apparatus capable of acquiring an observation image having a high contrast in a sample whose light absorption characteristic depends on a light wavelength. The charged particle beam apparatus according to the invention irradiates the sample with light, generates an observation image of the sample, changes an irradiation intensity per unit time of the light, and then generates a plurality of the observation images having different contrasts (see FIG. 4).

Abstract: An object of the invention is to provide a charged particle beam device capable of increasing the contrast of an observation image of a sample as much as possible in accordance with light absorption characteristics that change for each optical parameter. The charged particle beam device according to the invention changes an optical parameter such as a polarization plane of light emitted to the sample, and generates the observation image having a contrast corresponding to the changed optical parameter. An optical parameter that maximizes a light absorption coefficient of the sample is specified according to a feature amount of a shape pattern of the sample (refer to FIG. 5).