A method includes moving a plurality of sensors along a translation path with respect to an ion beam, acquiring sensor signals produced by the plurality of sensors, converting the acquired sensor signals into a data set representative of a two-dimensional (2D) profile of the ion beam, generating a plurality of first one-dimensional (1D) profiles of the ion beam from the data set, generating a plurality of second 1D profiles of the ion beam by spatially inverting each of the plurality of first 1D profiles, generating a plurality of third 1D profiles of the ion beam by superposing first current density values of each of the plurality of first 1D profiles with second current density values of a corresponding one of the plurality of second 1D profiles and determining whether to continue an implantation process with the ion beam in accordance with the plurality of third 1D profiles.

Systems and methods of profiling a charged-particle beam are disclosed. The method of profiling a charged-particle beam may comprise activating a charged-particle source to generate the charged-particle beam along a primary optical axis, modifying the charged-particle beam by adjusting an interaction between the charged-particle beam and a standing optical wave, detecting charged particles from the modified charged-particle beam after the interaction with the standing optical wave, and determining a profile of the charged-particle beam based on the detected charged particles. Alternatively, the method may include activating an optical source, modifying the optical beam by adjusting an interaction between the optical beam and a charged-particle beam, detecting an optical signal from the modified optical beam, and determining a characteristic of the charged-particle beam based on the detected optical signal.

Provided is an ion milling device capable of improving the reproducibility of an ion distribution. An ion milling device includes: an ion source (1); a sample stage (2) on which a sample (4) to be processed by being irradiated with an unfocused ion beam from the ion source (1) is placed; and a drive unit (8) configured to be arranged between the ion source (1) and the sample stage (2), and to move a linear ion beam measuring member (7) extending in a first direction to a second direction orthogonal to the first direction, in which the drive unit (8) moves the ion beam measuring member (7) within an emission range of the ion beam in a state where the ion beam is outputted from the ion source (1) under a first emission condition, and an ion beam current flowing through the ion beam measuring member (7) is measured by irradiating the ion beam measuring member (7) with the ion beam.

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 method includes receiving a spot beam profile is received for a spot ion beam; receiving a linear scanned beam profile for the spot ion beam; generating a calculated calibration spot profile, based upon the spot beam profile and the linear scanned beam profile; and implementing an adjusted scanned profile for the spot ion beam, based upon the calculated calibration spot profile.

The present disclosure addresses the problem of providing an electron gun that can directly monitor an intensity of an electron beam emitted from a photocathode using only the configuration provided to the electron gun, an electron beam applicator equipped with an electron gun, and a method for controlling an electron gun.

The aforementioned problem can be solved by an electron gun comprising a light source, a photocathode that emits an electron beam in response to receiving light from the light source, an anode, an electron-beam-shielding member with which it is possible to shield part of the electron beam, and a measurement unit that measures the intensity of the electron beam emitted from the photocathode using a measurement electron beam shielded by the electron-beam-shielding member.

An ion beam profiling system include a beam profiling element, an ion sensitive element electrically isolated from the beam profiling element, an ion source configured to emit an ion beam at the beam profiling element and the ion sensitive element, and a current measuring device coupled to the ion sensitive element. The beam profiling element includes a plate of material having two parallel major surfaces, a first slit aperture extending through the plate of material and having a first longitudinal length extending in a direction parallel to the two parallel major surfaces, and a second slit aperture extending through the plate of material and having a second longitudinal length extending in a direction parallel to the two parallel major surfaces, wherein the first longitudinal length of the first slit aperture is perpendicular to the second longitudinal length of the second slit aperture.

A particle beam column generates a particle beam of charged particles, for example electrons or ions, and direct it onto a sample. The particle beam column comprises a multi-aperture stop and a deflection system for selectively steering the particle beam through one of a plurality of apertures provided in the multi-aperture stop. The apertures have different sizes in order to limit the current strength of the particle beam to different values. The particle beam column furthermore comprises a lens for changing the divergence angle of the particle beam upstream of a first stop. The lens can comprise a magnetic lens, which comprises a magnetic core with a plurality of parts, which are electrically insulated from one another and can have substantially different electrical potentials during operation. Some of the parts of the magnetic core can have the same electrical potential as the first stop during operation.

In one embodiment, a multi charged-particle beam writing apparatus includes a plurality of blankers switching between ON and OFF state of a corresponding beam among multiple beams, a main deflector deflecting beams having been subjected to blanking deflection to a writing position of the beams in accordance with movement of a stage, a detector scanning a mark on the stage with each of the beams having been deflected by the main deflector and detecting a beam position from a change in intensity of reflected charged particles and a position of the stage, and a beam shape calculator switching an ON beam, scanning the mark with the ON beam, and calculating a shape of the multiple beams from a beam position. A shape of a deflection field of the main deflector is corrected by using a polynomial representing an amount of beam position shift that is dependent on a beam deflection position of the main deflector and then the mark is scanned with the ON beam. The polynomial is different for each ON beam.

An apparatus includes a beam scanner applying, during a non-uniform scanning mode, a plurality of different waveforms generating a scan of an ion beam along a scan direction, wherein a given waveform comprises a plurality of scan segments, wherein a first scan segment comprises a first scan rate and a second scan segment comprises a second scan rate different from the first scan rate; a current detector intercepting the ion beam outside of a substrate region and recording a measured integrated current of the ion beam for a given waveform; and a scan adjustment component coupled to the beam scanner and comprising logic to determine: when a beam width of the ion beam along the scan direction exceeds a threshold; and a plurality of current ratios based on the measured integrated current of the ion beam for at least two different waveforms of the plurality of waveforms.