Abstract: Signal electrons with high energy that pass near an optical axis, for example, backscattered electrons or secondary electrons in a booster optical system, can be detected. Therefore, there is provided a charged particle beam device including: a charged particle beam source configured to generate a charged particle beam; an objective lens configured to focus the charged particle beam to a sample; and a first charged particle detecting element disposed between the charged particle beam source and the objective lens and configured to detect charged particles generated by an interaction between the charged particle beam and the sample, in which a detection surface of the first charged particle detecting element is disposed on a center axis of the objective lens.

Abstract: Provided is a charged particle beam device which includes a storage unit that stores relationship information indicating a relationship between intensity or an intensity ratio of a charged particle signal obtained when a layer disposed on the sample is irradiated with the charged particle beam and a thickness of the layer; and a calculation unit that calculates the thickness of the layer as a thickness of the sample by using the relationship information and the intensity or the intensity ratio of the charged particle signal.

Abstract: A charged particle beam device includes: a charged particle beam source configured to generate a charged particle beam with which a sample is irradiated; a charged particle detection unit configured to detect a charged particle generated when the sample is irradiated with the charged particle beam; an intensity data generation unit configured to generate intensity data of the charged particle detected by the charged particle detection unit; a pulse-height value data generation unit configured to generate pulse-height value data of the charged particle detected by the charged particle detection unit; and an output unit configured to output a first image of the sample based on the intensity data and a second image of the sample based on the pulse-height value data.

Abstract: To provide, in observation of a sample that requires a movement between various devices, a charged particle beam device, a method for processing the sample, and an observation method which facilitate the movement between the devices. The charged particle beam device that processes an observation target on the sample using a charged particle beam includes: a sample stage on which the sample is placed; an observation unit configured to observe the observation target; and a writing unit configured to write information of the observation target in a writing position of the sample.

Abstract: As a device for correcting positive spherical aberration of an electromagnetic lens for a charged particle beam, a spherical aberration correction device combining a hole electrode and a ring electrode is known. In this spherical aberration correction device, when a voltage is applied between the hole electrode and the ring electrode, the focus of the charged particle beam device changes due to the convex lens effect generated in the hole electrode. Therefore, in a charged particle beam device including a charged particle beam source which generates a charged particle beam, a charged particle beam aperture having a ring shape, and a charged particle beam aperture power supply which applies a voltage to the charged particle beam aperture, the charged particle beam aperture power supply is configured to apply, to the charged particle beam aperture, a voltage having a polarity opposite to a polarity of charges of the charged particle beam.

Abstract: When a charged particle beam aperture having an annular shape is used, since a charged particle beam directly above the optical axis having the highest current density in the charged particle beam is blocked, it is difficult to dispose the charged particle beam aperture at an optimal mounting position.

Abstract: When using a charged particle beam aperture having a ring shape in a charged particle beam device, the charged particle beam with the highest current density immediately above the optical axis, among the charged particle beams is blocked, so that it is difficult to dispose the charged particle beam aperture at the optimal mounting position. Therefore, in addition to the ring-shaped charged particle beam aperture, a hole-shaped charged particle beam aperture is provided, and it is possible to switch between the case where the ring-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam and the case where the hole-shaped charged particle beam aperture is disposed on the optical axis of the charged particle beam.

Abstract: A charged particle beam device includes: a charged particle source that emits a charged particle beam; a boosting electrode disposed between the charged particle source and a sample to form a path of the charged particle beam and to accelerate and decelerate the charged particle beam; a first pole piece that covers the boosting electrode; a second pole piece that covers the first pole piece; a first lens coil disposed outside the first pole piece and inside the second pole piece to form a first lens; a second lens coil disposed outside the second pole piece to form a second lens; and a control electrode formed between a distal end portion of the first pole piece and a distal end portion of the second pole piece to control an electric field formed between the sample and the distal end portion of the second pole piece.

Abstract: To enable evaluation of a shape of a fine particle and a fine particle type, a substrate is set as a substrate on which an isolated fine particle to be measured and an isolated standard fine particle in the vicinity of the isolated fine particle to be measured are disposed, and a scanning electron microscope body including a detector configured to detect secondary charged particles obtained by scanning a surface of the substrate with an electron beam probe, and a computer that processes a detection signal and generates an image of the isolated fine particle to be measured and the isolated standard fine particle are provided. The computer corrects a shape of the isolated fine particle to be measured by using a measurement result of the isolated standard fine particle disposed in the vicinity of the isolated fine particle to be measured.

Abstract: The present invention provides a charged particle beam apparatus capable of efficiently reducing the effect of a residual magnetic field when SEM observation is performed. The charged particle beam apparatus according to the present invention includes a first mode for passing a direct current to a second coil after turning off a first coil, and a second mode for passing an alternating current to the second coil after turning off the first coil.

Abstract: The present invention realizes a composite charged particle beam apparatus capable of suppressing a leakage magnetic field from a pole piece forming an objective lens of an SEM with a simple structure. The charged particle beam apparatus according to the present invention obtains an ion beam observation image while passing a current to a first coil constituting the objective lens, and performs an operation of reducing the image shift by passing a current to a second coil with a plurality of current values, and determines a current to be passed to the second coil based on a difference between the operations.

Abstract: Signal electrons with high energy that pass near an optical axis, for example, backscattered electrons or secondary electrons in a booster optical system, can be detected. Therefore, there is provided a charged particle beam device including: a charged particle beam source configured to generate a charged particle beam; an objective lens configured to focus the charged particle beam to a sample; and a first charged particle detecting element disposed between the charged particle beam source and the objective lens and configured to detect charged particles generated by an interaction between the charged particle beam and the sample, in which a detection surface of the first charged particle detecting element is disposed on a center axis of the objective lens.

Abstract: Provided is a charged particle beam device which includes a storage unit that stores relationship information indicating a relationship between intensity or an intensity ratio of a charged particle signal obtained when a layer disposed on the sample is irradiated with the charged particle beam and a thickness of the layer; and a calculation unit that calculates the thickness of the layer as a thickness of the sample by using the relationship information and the intensity or the intensity ratio of the charged particle signal.

Abstract: A charged particle beam device includes: a charged particle source that emits a charged particle beam; a boosting electrode disposed between the charged particle source and a sample to form a path of the charged particle beam and to accelerate and decelerate the charged particle beam; a first pole piece that covers the boosting electrode; a second pole piece that covers the first pole piece; a first lens coil disposed outside the first pole piece and inside the second pole piece to form a first lens; a second lens coil disposed outside the second pole piece to form a second lens; and a control electrode formed between a distal end portion of the first pole piece and a distal end portion of the second pole piece to control an electric field formed between the sample and the distal end portion of the second pole piece.

Abstract: The charged particle beam device includes a charged particle beam source which emits a primary charged particle beam, an objective lens which focuses the primary charged particle beam on a sample, a passage electrode which is formed of a metal material and is disposed between the charged particle beam source and a tip end of the objective lens, a detector which detects a secondary charged particle emitted from the sample, and an electrostatic field electrode which is electrically insulated from the passage electrode. The passage electrode is formed such that the primary charged particle beam passes through the inside of the passage electrode. The electrostatic field electrode is formed to cover an outer periphery of the passage electrode.

Abstract: A composite charged particle beam apparatus modulates an irradiation condition of a charged particle beam at high speed and detects a signal in synchronization with a modulation period to extract a signal arising from a particular charged particle beam when a sample is irradiated with a plurality of charged particle beams simultaneously. Light emitted from two or more kinds of scintillators having different light emitting properties is dispersed, signal strength is detected, and a signal is processed based on a ratio of first signal strength when the sample is irradiated with a first charged particle beam alone to second signal strength when the sample is irradiated with a second charged particle beam alone. The apparatus can extract only a signal arising from a desired charged particle beam even when the sample is irradiated with the plurality of charged particle beams simultaneously.

Abstract: The present invention provides an electron beam device that achieves high spatial resolution and high luminance, while remaining insusceptible to the effects of external disturbance. The present invention relates to an electron beam device, wherein, between, e.g., an electron source for generating an electron beam and an objective lens for focusing the electron beam onto a sample, a high voltage beam tube is disposed close to the electron source and a low voltage beam tube is disposed close to the objective lens. This makes it possible to achieve high luminance while maintaining spatial resolution, even with an SEM that is provided with a type of objective lens that actively leaks a magnetic field onto a sample.

Abstract: A composite charged particle beam apparatus modulates an irradiation condition of a charged particle beam at high speed and detects a signal in synchronization with a modulation period to extract a signal arising from a particular charged particle beam when a sample is irradiated with a plurality of charged particle beams simultaneously. Light emitted from two or more kinds of scintillators having different light emitting properties is dispersed, signal strength is detected, and a signal is processed based on a ratio of first signal strength when the sample is irradiated with a first charged particle beam alone to second signal strength when the sample is irradiated with a second charged particle beam alone. The apparatus can extract only a signal arising from a desired charged particle beam even when the sample is irradiated with the plurality of charged particle beams simultaneously.

Abstract: The present invention relates to modulating an irradiation condition of a charged particle beam at high speed and detecting a signal in synchronization with a modulation period for the purpose of extracting a signal arising from a certain charged particle beam when a sample is irradiated with a plurality of charged particle beams simultaneously or, for example, for the purpose of separating a secondary electron signal arising from ion beam irradiation and a secondary electron signal arising from electron beam irradiation in an FIB-SEM system. The present invention further relates to dispersing light emitted from two or more kinds of scintillators having different light emitting properties, detecting each signal strength, and processing a signal on the basis of a ratio of first signal strength when the sample is irradiated with a first charged particle beam alone to second signal strength when the sample is irradiated with a second charged particle beam alone, the ratio being set by a mechanism.

Abstract: The present invention provides an electron beam device that achieves high spatial resolution and high luminance, while remaining insusceptible to the effects of external disturbance. The present invention relates to an electron beam device, wherein, between, e.g., an electron source for generating an electron beam and an objective lens for focusing the electron beam onto a sample, a high voltage beam tube is disposed close to the electron source and a low voltage beam tube is disposed close to the objective lens. This makes it possible to achieve high luminance while maintaining spatial resolution, even with an SEM that is provided with a type of objective lens that actively leaks a magnetic field onto a sample.