The present invention is to generate a spatially phase modulated electron wave. A laser radiating apparatus, a spatial light phase modulator, and a photocathode are provided. The photocathode has a semiconductor film having an NEA film formed on a surface thereof, and a thickness of the semiconductor film is smaller than a value obtained by multiplying a coherent relaxation time of electrons in the semiconductor film by a moving speed of the electrons in the semiconductor film. According to the configuration, a spatial distribution of phase and a spatial distribution of intensity of spatial phase modulated light are transferred to an electron wave, and the electron wave emitted from an NEA film is modulated into the spatial distribution of phase and the spatial distribution of intensity of the light. Since the spatial distribution of phase of the light can be modulated as intended by a spatial phase modulation technique for light, it is possible to generate an electron wave having a spatial distribution of phase modulated as intended.

A scanning electron microscope having a spectrometer with a sensor having a plurality of pixels, wherein the spectrometer directs different wavelengths of collected light onto different pixels. An optical model is formed and an error function is minimized to find values for the model, such that wavelength detection may be corrected using the model. The model can correct for errors generated by effects such as the motion of the electron beam over the specimen, aberrations introduced by optical elements, and imperfections of the optical elements. A correction function may also be employed to account for effects not captured by the optical model.

Systems, methods, and programming are described for inspecting a substrate having a pattern imaged thereon, including obtaining a plurality of selected target locations on the substrate, the selected target locations dependent on characteristics of the pattern, scanning the substrate with a plurality of electron beamlets, wherein the scanning includes individually addressing the beamlets to impinge on the selected target locations independently, detecting a reflected or a transmitted portion of the beamlets, and generating images of the selected target locations.

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.

A charged particle beam apparatus for directing a charged particle beam to preselected locations of a sample surface is provided. The charged particle beam has a field of view of the sample surface. A charged-particle-optical arrangement is configured to direct a charged particle beam along a beam path towards the sample surface and to detect charged particles generated in the sample in response to the charged particle beam. A stage is configured to support and move the sample relative to the beam path. A controller is configured to control the charged particle beam apparatus so that the charged particle beam scans over a preselected location of the sample simultaneously with the stage moving the sample relative to the charged-particle-optical column along a route, the scan over the preselected location of the sample covering a part of an area of the field of view.

An object of the present disclosure is to provide a charged particle beam apparatus that can quickly find a correction condition for a new aberration that is generated in association with beam adjustment. In order to achieve the above object, the present disclosure proposes a charged particle beam apparatus configured to include an objective lens (7) configured to focus a beam emitted from a charged particle source and irradiate a specimen, a visual field movement deflector (5 and 6) configured to deflect an arrival position of the beam with respect to the specimen, and an aberration correction unit (3 and 4) disposed between the visual field movement deflector and the charged particle source, in which the aberration correction unit is configured to suppress a change in the arrival position of the beam irradiated under different beam irradiation conditions.

An object of the present disclosure is to provide a charged particle beam apparatus that can quickly find a correction condition for a new aberration that is generated in association with beam adjustment. In order to achieve the above object, the present disclosure proposes a charged particle beam apparatus configured to include an objective lens (7) configured to focus a beam emitted from a charged particle source and irradiate a specimen, a visual field movement deflector (5 and 6) configured to deflect an arrival position of the beam with respect to the specimen, and an aberration correction unit (3 and 4) disposed between the visual field movement deflector and the charged particle source, in which the aberration correction unit is configured to suppress a change in the arrival position of the beam irradiated under different beam irradiation conditions.

According to one aspect of the present invention, an aberration corrector includes a first electrode substrate provided with first passage holes through which multiple electron beams pass; a second electrode substrate disposed below the first electrode substrate and provided with second passage holes through which the multiple electron beams pass, first electrodes of four or more poles being disposed individually on each top surface region of top surface regions around some second passage holes among the second passage holes; and a third electrode substrate disposed below the second electrode substrate and provided with third passage holes through which the multiple electron beams pass, second electrodes of four or more poles being disposed individually on each of top surface region of top surface regions around some third passage holes corresponding to remaining second passage holes in which the first electrodes are not disposed, among the third passage holes.

When using a charged particle beam aperture having a ring shape in a charged particle beam device, the charged particle beam with the highest current density immediately above the optical axis, among the charged particle beams is blocked, so that it is difficult to dispose the charged particle beam aperture at the optimal mounting position. Therefore, in addition to the ring-shaped charged particle beam aperture, a hole-shaped charged particle beam aperture is provided, and it is possible to switch between the case where the ring-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam and the case where the hole-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam.

An electrostatic lens for transporting charged particles in an axial direction includes a first group of first electrodes configured to receive a first DC potential from a DC voltage source, and a second group of second electrodes configured to receive a second DC potential from the DC voltage source different from the first DC potential. The first electrodes are interdigitated with the second electrodes. The first group and/or the second group has a geometric feature that progressively varies along the axial direction. The lens generates an axial potential profile that progressively changes along the axial direction, and thereby reduces geometrical aberrations. The lens may be part of a charged particle processing apparatus such as, for example, a mass spectrometer or an electron microscope.