An ion implantation system has an ion source configured to form an ion beam. A mass analyzer mass analyzes the ion beam, a scanning element scans the ion beam in a horizontal direction and a parallelizing lens translates the fanned-out scanned beam into parallel shifting scanning ion beam. For applications needing not only a mean incident angle, but highly-aligned ion incident angles and a tight angular distribution, a slit apparatus is positioned at horizontal and/or vertical front focal points of the parallelizing lens. Minimum horizontal and/or vertical angular distributions of the ion beam on the workpiece are attained by controlling a beam focusing lens upstream of the scanning element for the best beam transmission through the slit system.

The present invention addresses the problem of providing a method for automatically adjusting an electron beam emitted from an electron gun equipped with a photocathode to the incident axis of an electron optical system.

[Solution] An incident axis alignment method for an electron gun equipped with a photocathode, the electron gun being capable of emitting an electron beam in a first state due to the photocathode being irradiated with excitation light, and the method including at least an excitation light radiation step, a first excitation light irradiation position adjustment step for changing the irradiation position of the excitation light on the photocathode and adjusting the irradiation position of the excitation light, and an electron beam center detection step for detecting whether a center line of the electron beam in the first state coincides with an incident axis of an electron optical system.

A multi-beam inspection apparatus including an adjustable beam separator is disclosed. The adjustable beam separator is configured to change a path of a secondary particle beam. The adjustable beam separator comprises a first Wien filter and a second Wien filter. Both Wien filters are aligned with a primary optical axis. The first Wien filter and the second Wien filter are independently controllable via a first excitation input and a second excitation input, respectively. The adjustable beam separator is configured move the effective bending point of the adjustable beam separator along the primary optical axis based on the first excitation input and the second excitation input.

The present disclosure pertains to a beam deflection device capable of properly deflecting a beam. The present disclosure provides a beam deflection device for deflecting a beam inside a charged particle beam device, said beam deflection device being provided with: one or more electrostatic deflectors (207, 208) each having a pair of electrodes disposed so as to face each other across a beam path in a first direction orthogonal to the beam path; and one or more magnetic deflectors (209) each having a pair of magnetic poles disposed so as to face each other across the beam path in a second direction orthogonal to the beam path and to the first direction. When viewed from an incident direction of the beam, the one or more electrostatic deflectors and the one or more magnetic deflectors are stacked along the beam path such that the pair of electrodes at least partially overlap with the pair of magnetic poles and with a gap between the pair of magnetic poles.

A Wien filter and a charged particle beam imaging apparatus are provided. The Wien filter Wien filter, including a Wien filter body which includes: an electrostatic deflector, including at least one pair of electrodes, respective two electrodes in each pair of which are opposite to each other, each electrode including an electrode body constructed in an arc-shaped form, and respective electrode bodies of respective two electrodes in each pair of the at least one pair of electrodes being arranged concentrically with and opposite to each other in a diameter direction, and the at least one pair of electrodes being configured to generate respective electric fields by cooperation of the respective two electrodes in each pair of the at least one pair of electrodes, in the condition of respective bias voltages applied individually thereon; and a magnetic deflector, including at least one pair of magnetic poles, respective two magnetic poles in each pair of which are opposite to each other, each magnetic pole including a magnetic pole body constructed in an arc-shaped form, and respective magnetic pole bodies of respective two magnetic poles in each pair of the at least one pair of magnetic poles being arranged concentrically with and opposite to each other in the diameter direction, and the magnetic pole bodies of the at least one pair of magnetic poles in the magnetic deflector and the electrode bodies of the at least one pair of electrodes in the electrostatic deflector being arranged concentrically and spaced apart from each other in a circumferential direction, and the at least one pair of magnetic poles being configured to generate respective magnetic fields by cooperation of respective two magnetic poles in each pair of the at least one pair of magnetic poles; a resultant electric field formed collectively by all of the respective electric fields is perpendicular to a resultant magnetic field formed collectively by all of the respective magnetic fields; and each electrode is also provided with a respective first protrusion extending radially inwards from a radial inner side of the respective electrode body thereof, and each magnetic pole is also provided with a second protrusion extending radially inwards from a radial inner side of the respective magnetic pole body thereof.

A charged-particle source for generating a charged-particle comprises a sequence of electrodes, including an emitter electrode with an emitter surface, a counter electrode held at an electrostatic voltage with respect to the emitter electrode at a sign opposite to that of the electrically charged particles, and one or more adjustment electrodes surrounding the source space between the emitter electrode and the counter electrode. These electrodes have a basic overall rotational symmetry along a central axis, with the exception of one or more steering electrodes which is an electrode which interrupts the radial axial-symmetry of the electric potential of the source, for instance tilted or shifted to an eccentric position or orientation, configured to force unintended, secondary charged particles away from the emission surface.

In order to improve the accuracy of stage movement in a charged particle beam apparatus, this stage movement control apparatus is characterized by comprising: a storage device in which overshoot amount data in which the movement distance of a stage and the overshoot amount of the stage are associated is stored; a movement target position setting unit which sets the movement target position of the stage; a stage movement amount calculation unit which calculates a stage movement amount that is an amount by which the stage moves to the movement target position in future; an overshoot estimation unit which, on the basis of the calculated stage movement amount and the overshoot amount data, estimates an overshoot amount corresponding to the stage movement amount; a movement target position correction unit which sets a corrected movement target position obtained by correcting the movement target position closer than the movement target position by the calculated overshoot amount; and a stage movement control unit which moves the stage to the corrected movement target position.

A multi charged particle beam apparatus irradiates a substrate placed on a stage with a multi charged particle beam through an illumination optical system including a plurality of components, and an objective lens successively. In one embodiment, an optical system adjustment method for the multi charged particle beam apparatus includes measuring positional deviation amounts of a plurality of individual beams included in the multi charged particle beam at two or more different heights in an optical axis direction of a measurement surface or an imaging position of the multi charged particle beam, calculating a normalized position difference based on the two or more heights and the positional deviation amounts, the normalized position difference being an illumination system aberration equivalent amount of the illumination optical system, and adjusting a set value for at least one of the plurality of components using a value of the normalized position difference.

The present disclosure proposes a crossover-forming deflector array of an electro-optical system for directing a plurality of electron beams onto an electron detection device. The crossover-forming deflector array includes a plurality of crossover-forming deflectors positioned at or at least near an image plane of a set of one or more electro-optical lenses of the electro-optical system, wherein each crossover-forming deflector is aligned with a corresponding electron beam of the plurality of electron beams.

Provided is a scanning electron microscope provided with an energy selection and detection function for a SE.sub.1 generated on a sample while suppressing the detection amount of a SE.sub.3 excited due to a BSE in the scanning electron microscope that does not apply a deceleration method. Provided are: an electron optical system that includes an electron source 21 generating an irradiation electron beam and an objective lens 12 focusing the irradiation electron beam on a sample; a detector 13 that is arranged outside an optical axis of the electron optical system and detects a signal electron generated when the sample is irradiated with the irradiation electron beam; a deflection electrode that forms a deflection field 26 to guide the signal electron to the detector; a disk-shaped electrode 23 that is arranged to be closer to the electron source than the deflection field and has an opening through which the irradiation electron beam passes; and a control electrode arranged along the optical axis to be closer to the sample than the deflection field. The sample and the objective lens are set to a reference potential. A potential lower than the reference potential is applied to the disk-shaped electrode, and a potential higher than the reference potential is applied to the control electrode.