The present invention provides a simpler method for sharpening a tip of an emitter. In addition, the present invention provides an emitter including a nanoneedle made of a single crystal material, an emitter including a nanowire made of a single crystal material such as hafnium carbide (HfC), both of which stably emit electrons with high efficiency, and an electron gun and an electronic device using any one of these emitters. A method for manufacturing the emitter according to an embodiment of the present invention comprises processing a single crystal material in a vacuum using a focused ion beam to form an end of the single crystal material, through which electrons are to be emitted, into a tapered shape, wherein the processing is performed in an environment in which a periphery of the single crystal material fixed to a support is opened.

In a writing process in a charged-particle multi-beam apparatus, a desired pattern is written onto a target wherein said desired pattern is provided as input pattern data (INPDAT) in a vector format and processed through a pattern data processing flow. A data preprocessing system receives the input pattern data (INPDAT) and preprocesses the input pattern data independently of the writing process, preferably in advance to it, using writing parameter data provided to the data preprocessing system, and writes the intermediate pattern data (IMDAT) thus obtained to a data storage. When a writing process is carried out using the apparatus, its writing control system reads the intermediate pattern data from the data storage, converts them into pattern streaming data (SBUF), and streams the pattern streaming data to the apparatus for writing the pattern to the target.

Beam intercept profiles are measured as a particle beam transversely scans across a probe. A current of beam particles, a detector intensity, or image pixel intensities can variously be measured to obtain the profiles. Multiple profiles are used to determine geometric parameters which in turn can be used to configure equipment. In one application, transverse beam intercept profiles are measured for different waist heights of the particle beam. Steepness of the several profiles can be used to determine a height of the probe as the height at which the profile is steepest. The known probe height enables placing the probe in contact with a substrate at another known height. In another application, transverse beam intercept profiles of orthogonal probe edges are used to position a beam waist, reduce spot size, or reduce astigmatism. Techniques are applicable to SEM, FIB, and nanoprobe systems. Methods and apparatus are disclosed, with variations.

Beam intercept profiles are measured as a particle beam transversely scans across a probe. A current of beam particles, a detector intensity, or image pixel intensities can variously be measured to obtain the profiles. Multiple profiles are used to determine geometric parameters which in turn can be used to configure equipment. In one application, transverse beam intercept profiles are measured for different waist heights of the particle beam. Steepness of the several profiles can be used to determine a height of the probe as the height at which the profile is steepest. The known probe height enables placing the probe in contact with a substrate at another known height. In another application, transverse beam intercept profiles of orthogonal probe edges are used to position a beam waist, reduce spot size, or reduce astigmatism. Techniques are applicable to SEM, FIB, and nanoprobe systems. Methods and apparatus are disclosed, with variations.

A system and method for extending the life of a cathode and repeller in an IHC ion source is disclosed. The system monitors the health of the cathode by operating using a known set of parameters and measuring the bias power used to generate the desired extracted beam current or the desired current from the arc voltage power supply. Based on the measured bias power, the system may determine whether the cathode is becoming too thin, and may take a corrective action. This corrective action may be to alert the operator; to operate the IHC ion source using a predetermined set of parameters; or to change the dilution used within the IHC source. By performing these actions, the life of the cathode may be more than doubled.

A method to compensate for drift while controlling a charged particle beam (CPB) system having at least one charged particle beam controllable in position. Sources of drift include mechanical variations in the stage supporting the sample, beam deflection shifts, and environmental impacts, such as temperature. The method includes positioning a sample supported by a stage in the CPB system, monitoring a reference fiducial on a surface of the sample from a start time to an end time, determining a drift compensation to compensate for a drift that causes an unintended change in the position of a first charged particle beam relative to the sample by a known amount over a period of time based on a change in the position of the reference fiducial between the start time and the end time, and adjusting positions of the first charged particle beam by applying the determined drift compensation during an operation of the CPB system.

The invention relates to a method for processing an object using a material processing device that has a particle beam apparatus. The method comprises the following steps: determining a region of interest of the object on or in a first material region of the object, ablating material from a second material region adjoining the first material region by means of an ablation device, recognizing a geometric shape of the first material region, the geometric shape having a center, ablating material from a second portion of the first material region adjoining a first portion by means of a particle beam, the first portion having a first subregion and a second subregion, the region of interest being arranged in the first subregion, recognizing a further geometric shape of the first material region, the further geometric shape having a further center at a second position, relative positioning of the object such that the first position corresponds to the second position, and ablating material from the second subregion by means of the particle beam.

An aperture diaphragm capable of varying the size of an aperture in two dimensions is disclosed. The aperture diaphragm may be utilized in an ion implantation system, such as between the mass analyzer and the acceleration column. In this way, the aperture diaphragm may be used to control at least one parameter of the ion beam. These parameters may include angular spread in the height direction, angular spread in the width direction, beam current or cross-sectional area. Various embodiments of the aperture diaphragm are shown. In certain embodiments, the size of the aperture in the height and width directions may be independently controlled, while in other embodiments, the ratio between height and width is constant.

A 3D imaging system and method for a nanostructure is provided. The 3D imaging system includes a master control center, a vacuum chamber, an electron gun, an imaging signal detector, a broad ion beam source device, and a laser rangefinder component. A sample loading device is arranged inside the vacuum chamber. A radial source of the broad ion beam source device is arranged in parallel with an etched surface of a sample. The laser rangefinder component includes a first laser rangefinder configured to measure a distance from a top surface of an ion beam shielding plate and a second laser rangefinder configured to measure a distance from a non-etched area of the sample, the first laser rangefinder and the second laser rangefinder are arranged side by side, and a laser traveling direction is perpendicular to a traveling direction of the broad ion beam source device.

A collimated electron beam is illuminated to a grounded metal mask such that patterns on the mask can be transferred to a substrate identically. In a preferred embodiment, a linear electron source can be provided for enhancing lithographic throughput. The metal mask is adjacent to the substrate, but does not contact with substrate.