The present invention relates to a monochromator device. The monochromator device includes a first radiofrequency cavity positioned to receive an output beam from an electron source. A second radiofrequency cavity is positioned to receive the output beam from the first radiofrequency cavity. The first radiofrequency cavity and the second radiofrequency cavity are configured to, in combination, in combination, correct one or more energy deviations in time and space of the output beam.

The present invention relates to a monochromator device. The monochromator device includes a first radiofrequency cavity positioned to receive an output beam from an electron source. A second radiofrequency cavity is positioned to receive the output beam from the first radiofrequency cavity. The first radiofrequency cavity and the second radiofrequency cavity are configured to, in combination, in combination, correct one or more energy deviations in time and space of the output beam.

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.

In one embodiment, a multi charged particle beam writing method includes forming a multi charged particle beam with which a substrate serving as a writing target is irradiated, deflecting the multi charged particle beam to a position with a predetermined deflection offset added so that deflection voltages respectively applied to a plurality of electrodes of an electrostatic positioning deflector does not include a state where all the deflection voltages are zero, and irradiating the substrate with the multi charged particle beam. A positive common voltage is added to the deflection voltages which are applied to the respective electrodes of the electrostatic positioning deflector.

A difference between a calculated amount of drift and an actual amount of drift is reduced. According to one aspect of the present invention, a charged particle beam writing apparatus includes a deflector adjusting an irradiation position of the charged particle beam with respect to a substrate placed on a stage, a shot data generator generating shot data from writing data, the shot data including a shot position and beam ON and OFF times for each shot, a drift corrector referring to a plurality of pieces of the generated shot data, calculating an amount of drift of the irradiation position of the charged particle beam with which the substrate is irradiated, and generating correction information for correcting an irradiation position deviation based on the amount of drift, a deflection controller controlling a deflection amount achieved by the deflector based on the shot data and the correction information, and a dummy irradiation instructor instructing execution of dummy irradiation in a writing process to irradiate with the charged particle beam in a predetermined irradiation amount at a position different from the substrate on the stage.

A multi-beam apparatus for observing a sample with high resolution and high throughput is proposed. In the apparatus, a source-conversion unit forms plural and parallel images of one single electron source by deflecting plural beamlets of a parallel primary-electron beam therefrom, and one objective lens focuses the plural deflected beamlets onto a sample surface and forms plural probe spots thereon. A movable condenser lens is used to collimate the primary-electron beam and vary the currents of the plural probe spots, a pre-beamlet-forming means weakens the Coulomb effect of the primary-electron beam, and the source-conversion unit minimizes the sizes of the plural probe spots by minimizing and compensating the off-axis aberrations of the objective lens and condenser lens.

The invention relates to a method for electron microscopy. The method comprises providing an electron microscope, generating an electron beam and an image beam, adjusting one of the beam and of the beam and the image beam to reduce off-axial aberrations and correcting a diffraction pattern of the resulting modified beam. The invention also relates to a method for reducing throughput time in a sample image acquisition session in transmission electron microscopy. The method comprises providing an electron microscope, generating a beam and an image beam, adjusting one of the two to reduce off-axial aberrations and filtering the resulting modified image beam. The invention further relates to an electron microscope and to a non-transient computer-readable medium with a computer program for carrying out the methods.

The invention relates to a method for electron microscopy. The method comprises providing an electron microscope, generating an electron beam and an image beam, adjusting one of the beam and of the beam and the image beam to reduce off-axial aberrations and correcting a diffraction pattern of the resulting modified beam. The invention also relates to a method for reducing throughput time in a sample image acquisition session in transmission electron microscopy. The method comprises providing an electron microscope, generating a beam and an image beam, adjusting one of the two to reduce off-axial aberrations and filtering the resulting modified image beam. The invention further relates to an electron microscope and to a non-transient computer-readable medium with a computer program for carrying out the methods.

The invention relates to a particle beam device (100) for imaging, analyzing and/or processing an object (114). The particle beam device (100) comprises a first particle beam generator (300) for generating a first particle beam, wherein the first particle beam generator (300) has a first generator beam axis (301), wherein an optical axis (OA) of the particle beam device (100) and the first generator beam axis (301) are identical; a second particle beam generator (400) for generating a second particle beam, wherein the second particle beam generator (400) has a second generator beam axis (401), wherein the optical axis (OA) and the second generator beam axis (401) are arranged at an angle being different from 0° and 180°; a deflection unit (500) for deflecting the second particle beam from the second generator beam axis (401) to the optical axis (OA) and along the optical axis (OA), wherein the deflection unit (500) has a first opening (501) and a second opening (502) being different from the first opening (501), wherein the optical axis (OA) runs through the first opening (501), wherein the second generator beam axis (401) runs through the second opening (502); an objective lens (107) for focusing the first particle beam or the second particle beam onto the object (114), wherein the optical axis (OA) runs through the objective lens (107); and at least one detector (116, 121, 122) for detecting interaction particles and/or interaction radiation.

The invention provides a charged particle beam device capable of reducing a positional shift between secondary beams generated in a beam separator. The charged particle beam device includes a charged particle beam source configured to irradiate a sample with a plurality of primary beams, a plurality of detectors configured to detect secondary beams emitted from the sample in correspondence to the primary beams, and a beam separator configured to deflect the secondary beams in a direction different from that of the primary beams. The charged particle beam device further includes a deflector provided between the beam separator and the detector to correct a positional shift between the secondary beams generated in the beam separator.