The present disclosure relates to a system and a non-transitory computer-readable medium for estimating the height of foreign matter, etc. adhering to a sample. In order to achieve the abovementioned purpose, proposed is a system, etc. in which data acquired by a charged particle beam device or features extracted from the data are input to a learning model, which is provided with, in an intermediate layer thereof, a parameter learned using teacher data having data acquired by the charged particle beam device or features extracted from the data as inputs and having the heights or depths of the structures of samples or of foreign matter on the samples as outputs, and height or depth information is output.

A method for calibrating a scanning charged particle microscope, such as a scanning electron microscope (SEM), is provided. The method includes dividing a wafer into a plurality of regions; preparing, on each of the plurality of regions, a pattern including a first periodic structure interleaved with a second periodic structure, the first and second periodic structures having an induced offset; determining an actual pitch the first and second periodic structures and thereby determining actual induced offset on each of the plurality of regions; selecting a plurality of regions from among the plurality of regions; measuring, by the SEM, a pitch of first and second periodic structures on each of the plurality of regions; and performing linearity calibration on the SEM based on the determining and the measuring.

Systems and methods for controlling a plasma sheath characteristic are described. One of the methods includes determining a first value of the plasma sheath characteristic of a plasma sheath formed within a plasma chamber. The method further includes determining whether the first value of the plasma sheath characteristic is within a predetermined range from a preset value of the plasma sheath characteristic. The method also includes modifying a variable of a radio frequency (RF) generator coupled to the plasma chamber via an impedance matching circuit upon determining that the first value is not within the predetermined range from the preset value. The operation of modifying the variable of the RF generator is performed until it is determined that the first value of the plasma sheath characteristic is within the predetermined range from the preset value.

A charged particle beam apparatus that forms a probe with a charged particle beam and scans a specimen with the probe to acquire a scanning image. The charged particle beam apparatus includes an optical system for scanning the specimen with the probe; a detector that detects a signal generated from the specimen through the scanning of the specimen with the probe; and a control unit that controls the optical system. The control unit performs correction processing of acquiring a reference image obtained by the scanning of the specimen with the probe, comparing the reference image to a criterion image to determine a drift amount, and correcting a displacement of an irradiation position with the probe on the specimen based on the drift amount; and processing of setting a frequency with which the correction processing is to be performed based on the drift amount.

A sample may be inspected by making particles traverse the sample. The particles that have traversed the sample hit a detector one-by-one. In response thereto, the detector provides a sequence of respective detection outputs. The sequence of respective detection outputs is processed so as to identify respective locations where respective incident particles have hit the detector. An image is generated on the basis of the respective locations that have been identified. In order to determine a location where an incident particle has hit the detector, an evaluation is made with regard to pre-established respective associations between, on the one hand, respective locations where incident particles have hit the detector and, on the other hand, respective detection outputs.

The efficiency of operation in a semiconductor processing apparatus is improved. In order to search an input parameter value to be set in a semiconductor processing apparatus for processing into a target processed shape, a predictive model indicating a relationship between an input parameter value and an output parameter value is generated based on the input parameter value and the output parameter value which is a measured value of a processing result processed by setting the input parameter value in the semiconductor processing apparatus. In this case, when the measured value of the processing result processed by the semiconductor processing apparatus is the defective data, the predictive model is generated based on the input parameter value causing defective data and defective substitute data obtained by substituting the measured value which is the defective data.

Apparatus and methods are disclosed for particle beam focusing, suitable for use in sample preparation or test environments, including SEM-based nanoprobing platforms. With a particle beam incident on a sample surface, stage current is used as an indicator of spot size. By scanning or searching settings of a working distance control, a control value having maximum (or minimum) stage current is used to set the beam waist at the sample surface. Alternatively, minima (or maxima) of reflected current can be used. Stigmator controls can be adjusted similarly to reduce astigmatism. The scan of control settings can be performed concurrently with sweeping the beam across a region of interest on the sample. Curved sweep patterns can be used. Energy measurements can be used as an alternative to current measurement. Applications to a nanoprobing workflow are disclosed.

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.

A method for measuring a height difference between lift pins includes receiving a first center position being a position of the center of a substrate with respect to a reference position that is measured before a transfer robot loads the substrate onto a support unit provided in a process chamber, the support unit including a plurality of lift pins, receiving a second center position being a position of the center of the substrate with respect to the reference position that is measured after the transfer robot picks up the substrate unloaded from the support unit, and deriving a difference in height between at least one of the plurality of lift pins and the other lift pins from a vector difference between the first center position and the second center position.

An overlay target includes a grating-over-grating structure with a bottom grating structure disposed on a specimen and a top grating structure disposed on the bottom grating structure. The overlay target further includes a calibration scan location including the bottom grating structure but not the top grating structure and an overlay scan location including the top grating structure and the bottom grating structure.