The present disclosure provides a method to adjust asymmetric velocity of a scan in a scanning ion beam deposition or etch process to correct asymmetry of depositing or etching between the inboard side and the outboard side of device structures on a wafer, while maintaining the overall uniformity of the respective deposition or etch across the full wafer.

An objective of the present invention is to provide a charged particle beam device capable of estimating a lifetime of a filament of a charged particle beam source with a cheap and simple circuit configuration. The charged particle beam device according to the present invention includes a boosting circuit that boosts a voltage to be supplied to a filament and estimates a remaining duration of the filament using a measured value of a current flowing on a low-voltage side of the boosting circuit (see FIG. 3).

A plasma processing apparatus includes an external circuit electrically connected through a line to an electrical component in a processing chamber and a filter provided on the line to attenuate or block noise introduced into the line from the electrical component toward the external circuit. The filter includes a coil having constant diameter and coil length; a tubular outer conductor accommodating the coil and forming a distributed constant line in which parallel resonance occurs at multiple frequencies in combination with the coil; and a movable member for changing each winding gap of the coil and provided in an effective section where a specific one or a plurality of parallel resonance frequencies is shifted to a higher frequency side or a lower frequency side in frequency-impedance characteristics of the filter by changing the winding gap of the coil in the effective section in a longitudinal direction of the coil.

A plasma processing apparatus includes an external circuit electrically connected through a line to an electrical component in a processing chamber and a filter provided on the line to attenuate or block noise introduced into the line from the electrical component toward the external circuit. The filter includes a coil having constant diameter and coil length; a tubular outer conductor accommodating the coil and forming a distributed constant line in which parallel resonance occurs at multiple frequencies in combination with the coil; and a movable member for changing each winding gap of the coil and provided in an effective section where a specific one or a plurality of parallel resonance frequencies is shifted to a higher frequency side or a lower frequency side in frequency-impedance characteristics of the filter by changing the winding gap of the coil in the effective section in a longitudinal direction of the coil.

To provide a technique capable of measuring high-frequency electrical noise in a charged particle beam device. A charged particle beam device 100 includes an electron source 2 for generating an electron beam EB1, a stage 4 for mounting a sample 10, a detector 5 for detecting secondary electrons EB2 emitted from the sample 10, and a control unit 7 electrically connected to the electron source 2, the stage 4, and the detector 5 and can control the electron source 2, the stage 4, and the detector 5. Here, when the sample 10 is mounted on the stage 4, and a specific portion 11 of the sample 10 is continuously irradiated with the electron beam EB1 from the electron source 2, the control unit 7 can calculate a time-series change in irradiation position of the electron beam EB1 based on an amount of the secondary electrons EB2 emitted from the specific portion 11, and can calculate a feature quantity for a shake of the electron beam EB1 based on the time-series change in irradiation position. Further, the feature quantity includes a frequency spectrum.

To provide a technique capable of measuring high-frequency electrical noise in a charged particle beam device. A charged particle beam device 100 includes an electron source 2 for generating an electron beam EB1, a stage 4 for mounting a sample 10, a detector 5 for detecting secondary electrons EB2 emitted from the sample 10, and a control unit 7 electrically connected to the electron source 2, the stage 4, and the detector 5 and can control the electron source 2, the stage 4, and the detector 5. Here, when the sample 10 is mounted on the stage 4, and a specific portion 11 of the sample 10 is continuously irradiated with the electron beam EB1 from the electron source 2, the control unit 7 can calculate a time-series change in irradiation position of the electron beam EB1 based on an amount of the secondary electrons EB2 emitted from the specific portion 11, and can calculate a feature quantity for a shake of the electron beam EB1 based on the time-series change in irradiation position. Further, the feature quantity includes a frequency spectrum.

A device may include an electron source, a detector, and a deflector. The electron source may be directed toward a sample area. The detector may receive an electron signal or an electron-induced signal. A deflector may be positioned between the electron source and the sample. The deflector may modulate an intensity of the electron source directed to the sample area according to an electron dose waveform having a continuously variable temporal profile.

A scintillator assembly including an entrance surface for receiving charged particles into the scintillator assembly, the charged particles including first charged particles at a first energy level and second charged particles at a second energy level. A first scintillator structure configured for receiving the first charged particles and generating a corresponding first signal formed of first photons with a first wavelength of λ1, a second scintillator structure configured for receiving the second charged particles and generating a corresponding second signal of second photons with a second wavelength of λ2, and an emitting surface for egress of a combined signal from the scintillator assembly, the combined signal including the first and second photons, and at least one beam splitter for receiving the combined signal and separating the combined signal to first and second photons.

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 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.