A monitoring circuit that includes a pickup loop to monitor a voltage applied to a cavity of a linear accelerator is disclosed. The monitoring circuit is electrically isolated from the linear accelerator and is also electrically isolated from the controller that receives input from the circuit and controls the linear accelerator. In certain embodiments, the monitoring circuit also includes an energy harvester so as to capture energy without any physical connection to the controller. This may be achieved using light energy or electromagnetic energy, for example. In certain embodiments, the monitoring circuit includes an analog-to-digital converter to convert the signals received from the pickup loop to digital values. In other embodiments, the monitoring circuit passes analog voltages to the controller. The outputs from the monitoring circuit may include the amplitude and phase of the voltage being applied to the respective cavity.

A charged particle beam device includes: a charged particle beam source; an analyzer that analyzes and detects particles including secondary electrons and backscattered charged particles that are emitted from a specimen by irradiating the specimen with a primary charged particle beam emitted from the charged particle beam source; a bias voltage applying unit that applies a bias voltage to the specimen; and an analysis unit that extracts a signal component of the secondary electrons based on a first spectrum obtained by detecting the particles with the analyzer in a state where a first bias voltage is applied to the specimen, and a second spectrum obtained by detecting the particles with the analyzer in a state where a second bias voltage different from the first bias voltage is applied to the specimen.

A system for measuring and controlling the phase of an incoming analog waveform is disclosed. The system comprises an analog to digital converter to convert the incoming analog waveform to a digital representation. The system also includes a clock delay generator, which allows a programmable amount of delay to be introduced into the sample clock for the ADC. The system further comprises a controller to manipulate the delay used by the clock delay generator and store the outputs from the ADC. The controller can then use the digitized representation to determine the frequency of the incoming analog waveform, its phase drift and its phase relative to a master clock. The controller can then modify the output of a RF generator in response to these determinations.

An apparatus may include a first beam sensor, disposed adjacent a first position along a beamline. The apparatus may further include a second beam sensor, disposed adjacent a second position along the beamline, at a predetermined distance, downstream of the first beam sensor. The apparatus may include a detection system, coupled to the first beam sensor and to the second beam sensor to receive from a pulsed ion beam a first electrical signal from the first beam sensor and a second electrical signal from the second beam sensor.

An ion implanter includes: a main body which includes a plurality of units which are disposed along a beamline along which an ion beam is transported, and a substrate transferring/processing unit which is disposed farthest downstream of the beamline, and has a neutron ray source in which a neutron ray is generated due to collision of a ultrahigh energy ion beam; an enclosure which at least partially encloses the main body; and a neutron ray scattering member which is disposed at a position where a neutron ray which is emitted from the neutron ray source is incident in a direction in which a distance from the neutron ray source to the enclosure is equal to or less than a predetermined value.

Embodiments herein are directed to a resonator for an ion implanter. In some embodiments, a resonator may include a housing, and a first coil and a second coil partially disposed within the housing. Each of the first and second coils may include a first end including an opening for receiving an ion beam, and a central section extending helically about a central axis, wherein the central axis is parallel to a beamline of the ion beam, and wherein an inner side of the central section has a flattened surface.

An object of the invention is to stably supply an electron beam from an electron gun, that is, to prevent variation in intensity of the electron beam. The invention provides a charged particle beam device that includes an electron gun having an electron source, an extraction electrode to which a voltage used for extracting electrons from the electron source is applied, and an acceleration electrode to which a voltage used for accelerating the electrons extracted from the electron source is applied, a first heating unit that heats the extraction electrode, and a second heating unit that heats the acceleration electrode.

An apparatus and method for processing a workpiece with a beam is described. The apparatus includes a vacuum chamber having a beam-line for forming a particle beam and treating a workpiece with the particle beam, and a scanner for translating the workpiece through the particle beam. The apparatus further includes a scanner control circuit coupled to the scanner, and configured to control a scan property of the scanner, and a beam control circuit coupled to at least one beam-line component, and configured to control the beam flux of the particle beam according to a duty cycle for switching between at least two different states during processing.

A mass analyzer includes a mass analyzing magnet that applies a magnetic field to ions extracted from an ion source to deflect the ions, a mass analyzing slit that is provided downstream of the mass analyzing magnet and allows an ion of a desired ion species among the deflected ions to selectively pass, and a lens device that is provided between the mass analyzing magnet and the mass analyzing slit and applies a magnetic field and/or an electric field to the ion beam to adjust the convergence or divergence of a ion beam. The mass analyzer changes a focal point of the ion beam in a predetermined adjustable range between an upstream side and a downstream side of the mass analyzing slit with the lens device to adjust mass resolution.

Multiple electron beamlets are split from a single electron beam. The electron beam passes through an acceleration tube, a beam-limiting aperture, an anode disposed between an electron beam source and the acceleration tube, a focusing lens downstream from the beam-limiting aperture, and a micro aperture array downstream from the acceleration tube. The micro aperture array generates beamlets from the electron beam. The electron beam can be focused from a divergent illumination beam into a telecentric illumination beam.