Systems and methods for conducting charged particle beam modulation are disclosed. According to certain embodiments, a charged particle beam apparatus generates a plurality of charged particle beams. A modulator may be configured to receive the plurality of charged particle beams and generate a plurality of modulated charged particle beams. A detector may be configured to receive the plurality of modulated charged particle beams.

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.

An ElectroMagnetic-Mechanical Pulser (EMMP) generates electron pulses at a continuously tunable rate between 100 MHz and 20-50 GHz, with energies up to 0.5 MeV, duty cycles up to 20%, and pulse widths between 100 fs and 10 ps. A dielectric-filled Traveling Wave Transmission Stripline (TWTS) that is terminated by an impedance-matching load such as a 50 ohm load imposes a transverse modulation on a continuous electron beam. The dielectric is configured such that the phase velocity of RF propagated through the TWTS matches a desired electron energy, which can be between 100 and 500 keV, thereby transferring electromagnetic energy to the electrons. The beam is then chopped into pulses by an adjustable aperture. Pulse dispersion arising from the modulation is minimized by a suppressing section that includes a mirror demodulating TWTS, so that the spatial and temporal coherence of the pulses is substantially identical to the input beam.

Systems and methods for conducting charged particle beam modulation are disclosed. According to certain embodiments, a charged particle beam apparatus generates a plurality of charged particle beams. A modulator may be configured to receive the plurality of charged particle beams and generate a plurality of modulated charged particle beams. A detector may be configured to receive the plurality of modulated charged particle beams.

Disclosed is a device for, in combination with a stop having an aperture, generating charged particle beam pulses, an apparatus for inspecting a surface of a sample, and a method for inspecting a surface of a sample. The device includes a deflection unit which is arranged for positioning in or along a trajectory of a charged particle beam. The deflection unit is arranged for generating an electric field for deflecting said charged particle beam over the stop and across the aperture. The device also includes an electrical driving circuit for providing a periodic signal. The electrical driving circuit is connected to the manipulation unit via a photoconductive switch, wherein the photoconductive switch is arranged for: substantially insulating the deflection unit from the electrical driving circuit, and for conductively connecting the deflection unit to the electrical driving circuit only when said photoconductive switch is illuminated by a light beam.

In one embodiment, a charged particle beam writing apparatus includes a blanking circuit applying a blanking voltage to a blanking deflector, a stage on which a substrate is placed, a mark on the stage, a detector detecting an irradiation position of the charged particle beam based on irradiation of the mark with the charged particle beam, and a diagnostic electric circuitry that causes the charged particle beam to enter a predetermined defocused state relative to the mark, obtains a difference between a first irradiation position when the mark is scanned under first irradiation conditions and a second irradiation position when the mark is scanned under second irradiation conditions in which at least either of irradiation time and settling time in the first irradiation conditions is varied, and determines occurrence of a failure of the blanking circuit when the difference is a predetermined value or more.

In one embodiment, a multi charged particle beam writing apparatus includes a shaping aperture array forming multiple beams by allowing part of a charged particle beam to pass through a plurality of first openings, a blanking aperture array having a plurality of second openings having respective blankers each configured to deflect and blank the beam passing therethrough, a stopping aperture member having a third opening and configured to block deflected beams of the multiple beams at a position off the third opening, a first alignment coil disposed between the blanking aperture array and the stopping aperture member and adjusting a beam path, an objective lens disposed between the stopping aperture member and a stage, and a movement controller controlling a movement of a position of the third opening in an in-plane direction of the stopping aperture member.

A system includes an aperture array comprising a plurality of active apertures, respective ones of the active apertures configured to selectively deflect beams passing therethrough. The system also includes a limiting aperture configured to pass beams not deflected by the active apertures to a target object. The system further includes a control circuit configured to control the active apertures to provide first and second different exposure duration resolutions.

A multi charged particle beam writing method includes performing ON/OFF switching of a beam by an individual blanking system for the beam concerned, for each beam in multi-beams of charged particle beam, with respect to each time irradiation of irradiation of a plurality of times, by using a plurality of individual blanking systems that respectively perform beam ON/OFF control of a corresponding beam in the multi-beams, and performing blanking control, in addition to the performing ON/OFF switching of the beam for the each beam by the individual blanking system, with respect to the each time irradiation of the irradiation of the plurality of times, so that the beam is in an ON state during an irradiation time corresponding to irradiation concerned, by using a common blanking system that collectively performs beam ON/OFF control for a whole of the multi-beams.

An electron energy loss spectrometer is described having a direct detection sensor, a high speed shutter and a sensor processor wherein the sensor processor combines images from individual sensor read-outs and converts a two dimensional image from said sensor into a one dimensional spectrum and wherein the one dimensional spectrum is output to a computer and operation of the high speed shutter is integrated with timing of imaging the sensor. The shutter is controlled to allow reduction in exposure of images corresponding to the individual sensor readouts. A plurality of images are exposed by imaging less than the full possible exposure and wherein the plurality of images are combined to form a composite image. The plurality of images can be comprised of images created by exposing the sensor for different exposure times.