This invention provides a wafer processing method comprising a process of irradiating a wafer to be processed placed on the upper surface of a sample table arranged in a processing chamber with light or electromagnetic waves to heat and remove a compound layer of a film layer that is preliminarily formed on the upper surface of the film layer of the upper surface of the wafer, wherein in the process, by receiving the light or electromagnetic waves reflected by the upper surface of the wafer, a signal indicating a temporal change in intensity using the wavelength of the light or electromagnetic waves as a parameter is corrected using information of the intensity of the light or electromagnetic waves detected by receiving the light or electromagnetic waves at a position on the circumferential side of the upper surface of the sample table.

A Fast Faraday Cup includes a group of electrodes including a grounded electrode having a through hole and a collector electrode configured with a blind hole that functions a collector hole. The electrodes are configured to allow a beam (e.g., a non-relativistic beam) to fall onto the grounded electrode so that the through hole cuts a beamlet that flies into the collector hole and facilitates measurement of the longitudinal distribution of particle charge density in the beam. The diameters, depths, spacing and alignment of the collector hole and the through hole are controllable to enable the Fast Faraday day cup to operate with a fast response time (e.g., fine time resolution) and capture secondary particles.

A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.

An apparatus includes first and second VI sensors, an optical sensor, and an arcing detector. The first VI sensor is disposed in a power filter or on a power supply line connected to a heater disposed in a lower electrode of a process chamber in which a plasma process is performed. The first VI sensor senses a harmonic generated from a first power supply supplying power to the lower electrode and outputs a first signal. The optical sensor senses an intensity of light generated from the process chamber and outputs a second signal. The second VI sensor is disposed on a power supply line connected to an upper electrode and senses a harmonic generated from a second power supply supplying power to the upper electrode and outputs a third signal. The arcing detector determines whether arcing occurs based on one or more of the first, second, and third signals.

An ion collector includes a plurality of segments and a plurality of integrators. The plurality of segments are physically separated from one another and spaced around a substrate support. Each of the segments includes a conductive element that is designed to conduct a current based on ions received from a plasma. Each of the plurality of integrators is coupled to a corresponding conductive element. Each of the plurality of integrators is designed to determine an ion distribution for a corresponding conductive element based, at least in part, on the current conducted at the corresponding conductive element. An example benefit of this embodiment includes the ability to determine how uniform the ion distribution is across a wafer being processed by the plasma.

Systems and methods are provided for charged particle detection. The detection system can comprise a signal processing circuit configured to generate a set of intensity gradients based on electron intensity data received from a plurality of electron sensing elements. The detection system can further comprise a beam spot processing module configured to determine, based on the set of intensity gradients, at least one boundary of a beam spot; and determine, based on the at least one boundary, that a first set of electron sensing elements of the plurality of electron sensing elements is within the beam spot. The beam spot processing module can further be configured to determine an intensity value of the beam spot based on the electron intensity data received from the first set of electron sensing elements and also generate an image of a wafer based on the intensity value.

A radiographic image capturing device includes: plural radiation dose detection pixels that respectively output signal values according to a dose of irradiated radiation; a determination unit that determines a presence or absence of defects, block-by-block, based on signal values of radiation dose detection pixels included in each of plural blocks, which are arranged such that the respective blocks include at least a portion of the plural radiation dose detection pixels; a block rearrangement unit that performs block rearrangement to change the arrangement of the plural blocks according to a determination result of the determination unit; and a detection unit that detects a dose of irradiated radiation based on signal values of each arranged block or of each rearranged block.

There is provided a charged particle beam apparatus capable of obtaining a high SN ratio with a small electron irradiation amount. The charged particle beam apparatus includes a charged particle detection device. The charged particle detection device detects an analog pulse waveform signal (110) in a detection of emitted electrons (1 event) when one primary electron enters a sample, converts the analog pulse waveform signal (110) into a digital signal (111), perform a wave height discrimination (112) with the use of a unit peak corresponding electron, and outputs the digital signal (111) as a multilevel count value.

A particle beam system includes a particle source to produce a first beam of charged particles. The particle beam system also includes a multiple beam producer to produce a plurality of partial beams from a first incident beam of charged particles. The partial beams are spaced apart spatially in a direction perpendicular to a propagation direction of the partial beams. The plurality of partial beams includes at least a first partial beam and a second partial beam. The particle beam system further includes an objective to focus incident partial beams in a first plane so that a first region, on which the first partial beam is incident in the first plane, is separated from a second region, on which a second partial beam is incident. The particle beam system also a detector system including a plurality of detection regions and a projective system.

Provided is a plasma processing method for selectively removing, after plasma etching using a mask having an amorphous carbon film containing boron, the amorphous carbon film using plasma from a silicon nitride film, a silicon oxide film or a tungsten film. The plasma processing method includes a removing step of removing the amorphous carbon film using plasma generated by mixed gas of O.sub.2 gas and CH.sub.3F gas, or CH.sub.2F.sub.2 gas.