An anomaly determination method of the present embodiment includes: measuring a first resistance value of a processing target via a first grounding member when the first grounding member is attached to the processing target in a first chamber; bringing the first grounding member into contact with a grounded second grounding member to measure a second resistance value of the processing target via the first and second grounding members in a second chamber; and determining an anomaly of the second grounding member with an arithmetic processing unit based on a trend of a resistance difference between the first resistance value and the second resistance value for a plurality of processing targets.

A method of extracting and accelerating ions is provided. The method includes providing a ion source. The ion source includes a chamber. The ion source further includes a first hollow cathode having a first hollow cathode cavity and a first plasma exit orifice and a second hollow cathode having a second hollow cathode cavity and a second plasma exit orifice, the first and second hollow cathodes being disposed adjacently in the chamber. The ion source further includes a first ion accelerator between and in communication with the first plasma exit orifice and the chamber. The first ion accelerator forms a first ion acceleration cavity. The ion source further includes a second ion accelerator between and in communication with the second plasma orifice and the chamber. The second ion accelerator forms a second ion acceleration cavity. The method further includes generating a plasma using the first hollow cathode and the second hollow cathode. The first hollow cathode and the second hollow cathode are configured to alternatively function as electrode and counter-electrode. The method further includes extracting and accelerating ions. Each of the first ion acceleration cavity and the second ion acceleration cavity are sufficient to enable the extraction and acceleration of ions.

To provide a functional membrane for ion beam transmission capable of enhancing ion beam transmittance and improving beam emittance. A functional membrane for ion beam transmission according to the present invention is used in a beam line device through which an ion beam traveling in one direction passes and has a channel. The axis of the channel is substantially parallel to the travel direction of the ion beam.

A method and a charged particle beam system that includes charged particle beam optics and a movable stage; wherein the movable stage is configured to introduce a movement between the object and charged particle beam optics; wherein the movement is of a constant velocity and along a first direction; wherein the charged particle beam optics is configured to scan, by the charged particle beam, multiple areas of the object so that each point of the multiple areas is scanned multiple times; wherein the multiple areas partially overlap; wherein the scanning is executed by the charged particle beam optics; wherein the scanning comprises performing counter-movement deflections of the charged particle beam for at least partially compensating for the movement; and wherein each area of the multiple areas is scanned by following an area scan scheme that defines multiple scan lines that differ from each other.

A frame member for an electron beam lithography device of the present disclosure includes a frame body comprising sapphire or aluminum oxide-based ceramics having an open porosity of 0.2% or less and a conductive film disposed at least on a main surface of an electron gun side of the frame body.

Described is a method comprising directing an ultra-low voltage electron beam to a surface of a first insulating layer. The first insulating layer is disposed on a second insulating layer. The method includes modifying, by the application of the ultra-low voltage electron beam, the surface of the first insulating layer to selectively switch an interface between a first state having a first electronic property and a second state having a second electronic property.

An apparatus is provided. The apparatus includes a beam current measuring device and a first electrode. The beam current measuring device is retractably movable into an ion beam trajectory so as to measure an ion beam current. The first electrode is disposed immediately upstream of the beam current measuring device in an ion beam transport channel. The first electrode serves both as a suppressor electrode for repelling secondary electrons released from the beam current measuring device, back toward the beam current measuring device, and as a beam optical element other than the suppressor electrode.

Disclosed are apparatus and methods for performing overlay metrology upon a target having at least two layers formed thereon. A target having a plurality of periodic structures for measuring overlay in at least two overlay directions is provided. A charged particle beam is scanned in a first direction across a plurality of scan swaths of the target and at a first tilt with respect to the target so that each edge of the periodic structures is scanned at an angle. The charged particle beam is scanned in a second direction, which is opposite the first direction, across the plurality of scan swaths and at a second tilt that is 180 from the first tilt. The first and second direction scanning operations are then repeated for different first and second tilts and a different plurality of scan swaths of the target so that the target is scanned symmetrically. Images that are generated by the first and second direction scanning operations are combined to form a combined image, and an overlay error of the target is determined and reported based on analyzing the combined image.

Disclosed are apparatus and methods for performing overlay metrology upon a target having at least two layers formed thereon. A target having a plurality of periodic structures for measuring overlay in at least two overlay directions is provided. A charged particle beam is scanned in a first direction across a plurality of scan swaths of the target and at a first tilt with respect to the target so that each edge of the periodic structures is scanned at an angle. The charged particle beam is scanned in a second direction, which is opposite the first direction, across the plurality of scan swaths and at a second tilt that is 180 from the first tilt. The first and second direction scanning operations are then repeated for different first and second tilts and a different plurality of scan swaths of the target so that the target is scanned symmetrically. Images that are generated by the first and second direction scanning operations are combined to form a combined image, and an overlay error of the target is determined and reported based on analyzing the combined image.

An electron beam inspection apparatus includes an acquisition processing circuitry to acquire surface material information presenting a surface material of the substrate and a value of an acceleration voltage of an electron beam; a sequence determination processing circuitry to determine a scan sequence of a plurality of stripe regions on the basis of the surface material of the substrate and the value of the acceleration voltage, the plurality of stripe regions obtained by virtually dividing an inspection region of the substrate in a stripe shape; a secondary electron image acquisition mechanism including a detector for detecting a secondary electron and configured to scan the plurality of stripe regions of the substrate according to a determined scan sequence and to acquire a secondary electron image of the substrate; and a comparison processing circuitry to compare the secondary electron image with a corresponding reference image.