The present invention relates to a method for measuring a sample with a microscope, the method comprising scanning the sample using a focusing plane having a first angle with respect to a top surface of the sample and computing a confidence distance based on the first angle. The method further comprises selecting at least one among a plurality of alignment markers on the sample for performing a lateral alignment of the scanning step and/or for performing a lateral alignment of an output of the scanning step. In particular, the at least one alignment marker selected at the selecting step is chosen among the alignment markers placed within the confidence distance from an intersection of the focusing plane with the top surface.

An electron-beam device includes upper-column electron optics and lower-column electron optics. The upper-column electron optics include an aperture array to divide an electron beam into a plurality of electron beamlets. The upper-column electron optics also include a lens array with a plurality of lenses to adjust the focus of the plurality of electron beamlets. Respective lenses of the plurality of lenses are to adjust the focus of respective electron beamlets of the plurality of electron beamlets. The upper-column electron optics further include a first global lens to adjust the focus of the plurality of electron beamlets in a manner opposite to the lens array.

An electron-beam device includes upper-column electron optics and lower-column electron optics. The upper-column electron optics include an aperture array to divide an electron beam into a plurality of electron beamlets. The upper-column electron optics also include a lens array with a plurality of lenses to adjust the focus of the plurality of electron beamlets. Respective lenses of the plurality of lenses are to adjust the focus of respective electron beamlets of the plurality of electron beamlets. The upper-column electron optics further include a first global lens to adjust the focus of the plurality of electron beamlets in a manner opposite to the lens array.

Provided is a sample milling apparatus capable of milling various samples efficiently. The sample milling apparatus includes an anode, a cathode for emitting electrons which are made to collide with gas molecules so that ions are generated, an extraction electrode for causing the generated ions to be extracted as an ion beam, and a focusing electrode disposed between the cathode and the extraction electrode and applied with a focusing voltage. The spatial profile of the ion beam is controlled by varying the focusing voltage applied to the focusing electrode.

Provided is a sample milling apparatus capable of milling various samples efficiently. The sample milling apparatus includes an anode, a cathode for emitting electrons which are made to collide with gas molecules so that ions are generated, an extraction electrode for causing the generated ions to be extracted as an ion beam, and a focusing electrode disposed between the cathode and the extraction electrode and applied with a focusing voltage. The spatial profile of the ion beam is controlled by varying the focusing voltage applied to the focusing electrode.

An optical system used in a charged particle beam inspection system. The optical system includes one or more optical lenses, and a compensation lens configured to compensate a drift of a focal length of a combination of the one or more optical lenses from a first medium to a second medium.

An electron source emits an electron beam. The electron beam is received by a beam limiting assembly. The beam limiting assembly has a first beam limiting aperture with a first diameter and a second beam limiting aperture with a second diameter larger than the first diameter. The first beam limiting aperture receives the electron beam. This beam limiting assembly reduces the influence of Coulomb interactions.

An electron source emits an electron beam. The electron beam is received by a beam limiting assembly. The beam limiting assembly has a first beam limiting aperture with a first diameter and a second beam limiting aperture with a second diameter larger than the first diameter. The first beam limiting aperture receives the electron beam. This beam limiting assembly reduces the influence of Coulomb interactions.

A multiple particle beam system with a mirror mode of operation, a method for operating a multiple particle beam system with a mirror mode of operation and an associated computer program product are disclosed. The multiple particle beam system can be operated in different mirror modes of operation which allow the multiple particle beam system to be inspected and recalibrated thoroughly. A detection system configured to operate in a first detection mode and/or in a second detection mode is used for the analysis.

Electron beam spot characteristics can be tuned in each x-ray tube by moving a focusing-ring along a longitudinal-axis of the x-ray tube. The focusing-ring can then be immovably fastened to the x-ray tube.

An x-ray source can include an x-ray tube and a focusing-ring. The focusing-ring can at least partially encircle an electron-emitter, a cathode, an evacuated-enclosure, or combinations thereof. The focusing-ring can be located outside of a vacuum of the evacuated enclosure. The focusing-ring can adjust an electron-beam spot on a target material of the x-ray tube when moved along a longitudinal-axis extending linearly from the electron-emitter to the target material.