The present invention relates to a charged particle beam system comprising a deflection subsystem configured to deflect a charged particle beam in a deflection direction based on a sum of analog signals generated by separate digital to analog conversion of a first digital signal and a second digital signal. The present invention further relates to a method of configuring the charged particle beam system so that each of a plurality of regions of interest can be scanned by varying only the first digital signal while the second digital signal is held constant at a value associated with the respective region of interest. The present invention further relates to a method of recording a plurality of images of the regions of interest at the premise of reduced interference due to charge accumulation.

Apparatus and methods for adjusting beam condition of charged particles are disclosed. According to certain embodiments, the apparatus includes one or more first multipole lenses displaced above an aperture, the one or more first multipole lenses being configured to adjust a beam current of a charged-particle beam passing through the aperture. The apparatus also includes one or more second multipole lenses displaced below the aperture, the one or more second multipole lenses being configured to adjust at least one of a spot size and a spot shape of the beam.

A process control method is provided for ion implantation methods and apparatuses, to produce a high dosage area on a substrate such as may compensate for noted non-uniformities. In an ion implantation tool, separately controllable electrodes are provided as multiple sets of opposed electrodes disposed outside an ion beam. Beam blockers are positionable into the ion beam. Both the electrodes and beam blockers are controllable to reduce the area of the ion beam that is incident upon a substrate. The electrodes and beam blockers also change the position of the reduced-area ion beam incident upon the surface. The speed at which the substrate scans past the ion beam may be dynamically changed during the implantation process to produce various dosage concentrations in the substrate.

Methods for drift corrected, fast, low dose, adaptive sample imaging with a charged particle microscopy system include scanning a surface region of a sample with a charged particle beam to obtain a first image of the surface region with a first detector modality, and then determining a scan strategy for the surface region. The scan strategy comprises a charged particle beam path, a first beam dwell time associated with at least one region of interest in the first image, the first beam dwell time being sufficient to obtain statistically significant data from a second detector modality, and at least a second beam dwell time associated with other regions of the first image, wherein the first beam dwell time is different than the second beam dwell time. The surface region of the sample is then scanned with the determined scan strategy to obtain data from the first and second detector.

A method for scanning an object with a charged particle beam, the method may include repeating, for each pair of scan lines out of multiple pairs of scan lines, the stages of: (i) deflecting the charged particle beam along a first direction, thereby scanning the object along a first scan line of the pair of scan lines; (ii) collecting electrons emitted from the object during the scanning of the object along a majority of the first scan line; (iii) deflecting the charged particle beam along a second direction that is normal to the first direction; (iv) deflecting the charged particle beam along a third direction that is opposite to the first direction, thereby scanning the object along a second scan line of the pair of scan lines; (v) collecting electrons emitted from the object during the scanning of the object along a majority of the second scan line; and (vi) deflecting the charged particle beam along the second direction that is normal to the third direction.

The present invention provides an electrode assembly comprising two or more electrodes arranged around a primary axis forming a non-cylindrical channel space. General electronic apparatus/device, particularly apparatus of charged-particle beam such as electron microscope, may use the electrode assembly to create an optimized pattern of electrical field within non-cylindrical channel space. When the electrode assembly is used as a beam deflector in a magnetic objective lens, the electrical field within the central channel space can be co-optimized with the magnetic field for reducing aberration(s) such as distortion, field curvature, astigmatism, and chromatic aberration, after the beam passes through the central channel space.

An object of the invention is to provide a charged particle beam apparatus capable of performing high-precision measurement even on a pattern in which a width of edges is narrow and inherent peaks of the edges cannot be easily detected. In order to achieve the above object, there is proposed a charged particle beam apparatus including an opening portion forming member having a passage opening of a charged particle beam and a detector for detecting charged particles emitted from a sample or charged particles generated by causing the charged particles to collide with the opening portion forming member, the charged particle beam apparatus including: a deflector for deflecting the charged particles emitted from the sample; and a control device for controlling the deflector, the control device performing pattern measurement with the use of a first detected signal in which a signal of one edge is emphasized relatively more than a signal of another edge among a plurality of edges on the sample and a second detected signal in which the signal of the another edge is emphasized relatively more than the signal of the one edge among the plurality of edges.

A method of using a Charged Particle Microscope, comprising: A specimen holder, for holding a specimen; A source, for producing an irradiating beam of charged particles; An illuminator, for directing said beam so as to irradiate the specimen; A detector, for detecting a flux of emergent radiation emanating from the specimen in response to said irradiation,
additionally comprising the following steps: In said illuminator, providing an aperture plate comprising an array of apertures; Using a deflecting device to scan said beam across said array, thereby alternatingly interrupting and transmitting the beam so as to produce a train of beam pulses; Irradiating said specimen with said train of pulses, and using said detector to perform positionally resolved (temporally discriminated) detection of the attendant emergent radiation.

Provided are a multistage-connected multipole and a charged particle beam device that can be produced with precision in machining without requiring precision in brazing between a pole and an insulation material. This multi-stage connected multipole 100 comprises: a plurality of poles Q1-Q4 that are arranged along the optical-axis direction of a charged particle beam, and that have cutouts Non surfaces facing each other; and braces P1-P3 that are arranged between the plurality of poles Q1-Q4 and are made of an insulator. The poles Q1-Q4 and the braces P1-P3 are joined by fitting the braces P1-P3 into the cutouts N and applying brazing so as to be interposed by a bonding material.

Methods for drift corrected, fast, low dose, adaptive sample imaging with a charged particle microscopy system include scanning a surface region of a sample with a charged particle beam to obtain a first image of the surface region with a first detector modality, and then determining a scan strategy for the surface region. The scan strategy comprises a charged particle beam path, a first beam dwell time associated with at least one region of interest in the first image, the first beam dwell time being sufficient to obtain statistically significant data from a second detector modality, and at least a second beam dwell time associated with other regions of the first image, wherein the first beam dwell time is different than the second beam dwell time. The surface region of the sample is then scanned with the determined scan strategy to obtain data from the first and second detector.