Techniques for acquiring an electron energy loss spectrum in two dimensions are disclosed herein. The technique at least includes exposing an electron sensor to an electron spectrum projected in two dimensions, wherein one of the two dimensions corresponds to a dispersive axis, and the other of the two dimensions corresponds to a non-dispersive axis, receiving an electron sensor readout frame from the electron sensor, where the electron sensor readout frame comprises a plurality of values representative of the electron spectrum in each of the two dimensions, and reducing a resolution of the electron sensor readout frame in at least one of the two dimensions, where reducing the resolution includes reducing the number of values in the at least one of the two dimensions, where the electron sensor readout frame comprises a plurality of values in each of the two dimensions after the reduction in resolution.

A method of influencing a charged particle beam (11) propagating along an optical axis (A) is described. The method includes: guiding the charged particle beam (11) through at least one opening (102) of a multipole device (100, 200) that comprises a first multipole (110, 210) with four or more first electrodes (111, 211) and a second multipole (120, 220) with four or more second electrodes (121, 221) arranged in the same sectional plane, the first electrodes and the second electrodes being arranged alternately around the at least one opening (102); and at least one of exciting the first multipole to provide a first field distribution for influencing the charged particle beam in a first manner, and exciting the second multipole to provide a second field distribution for influencing the charged particle beam in a second manner. Further, a multipole device (100, 200) with a first multipole (110, 210) and a second multipole (120, 220) provided on the same substrate as well as a charged particle beam apparatus (500) with a multipole device (100, 200) are provided.

A blanking device for multi-beams includes arrayed plural separate blanking systems, each performing blanking control switching a corresponding beam of multi charged particle beams between a beam ON state and a beam OFF state and each including a first electrode, a first potential applying mechanism applying two different potentials selectively to the first electrode for the blanking control, and a second electrode performing blanking deflection of the corresponding beam, the second electrode being grounded and paired with the first electrode, and a potential change mechanism changing a potential of the second electrode from a ground potential to another potential, wherein when a potential of the first electrode included in one of the separate blanking systems is fixed to the ground potential, the potential change mechanism changes the potential of the second electrode corresponding to the first electrode fixed to the ground potential, from the ground potential to the another potential.

There is provided a beam alignment method capable of easily aligning an electron beam with a coma-free axis in an electron microscope. The method starts with tilting the electron beam (EB) in a first direction (+X) relative to a reference axis (A) and obtaining a first TEM (transmission electron microscope) image. Then, the beam is tilted in a second direction (−X) relative to the reference axis, the second direction (−X) being on the opposite side of the reference axis (A) from the first direction (+X), and a second TEM image is obtained. The reference axis is incrementally varied so as to reduce the brightness of the differential image between a power spectrum of the first TEM image and a power spectrum of the second TEM image.

A field emission device comprises one or more emitter elements, each having a high aspect ratio structure with a nanometer scaled cross section; and one or more segmented electrodes, each surrounding one of the one or more emitters. Each of the one or more segmented electrodes has multiple electrode plates. This abstract is provided to comply with rules requiring an abstract that will allow a searcher or other reader to quickly ascertain the subject matter of the technical disclosure. It is submitted with the understanding that it will not be used to interpret or limit the scope or meaning of the claims.

There are disclosed an aberration correction method and a charged particle beam system capable of correcting off-axis first order aberrations. The aberration correction method is for use in the charged particle beam system (100) equipped with an aberration corrector (30) which has plural stages of multipole elements (32a, 32b) and a transfer lens system (34) disposed between the multipole elements (32a, 32b). The method includes varying the excitation of the transfer lens system (34) and correcting off-axis first order aberrations.

A system for melting, sintering, or heat treating a material is provided. The system includes a cathode, an anode, and a focus coil assembly having a quadrupole magnet. The quadrupole magnet includes four poles and a yoke. The four poles are spaced apart and surround a beam cavity. Each of the four poles includes a pole face proximate the beam cavity and an end opposite the pole face. The first and third poles are aligned along an x-axis and configured to have a first magnetic polarity at their respective pole faces and a second magnetic polarity opposite the first magnetic polarity at their respective ends. The second and fourth poles are aligned along a y-axis and configured to have the second magnetic polarity at their respective pole faces and the first magnetic polarity at their respective ends. The yoke surrounds the poles and is coupled to the poles.

Charged particle beam systems and methods, such as a multi beam charged particle beam system and related methods, can compensate sample charging.

It is provided a charged particle beam manipulation device for a plurality of charged particle beamlets, the charged particle beam manipulation device including a lens having a main optical axis, the lens including at least a first array of multipoles, each multipole of the first array of multipoles configured to compensate for a lens deflection force on a respective charged particle beamlet of the plurality of charged particle beamlets, the lens deflection force being a deflection force produced by the lens on the respective charged particle beamlet towards the main optical axis of the lens.

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.