The present invention provides a plasma generating system that includes: a waveguide for transmitting a microwave energy therethrough; an inner wall disposed within the waveguide to define a plasma cavity, wherein a plasma is generated within the plasma cavity using the microwave energy; a first gas inlet mounted on a first side of the waveguide and configured to introduce a first gas into the plasma cavity and generate a first vortex flow within the plasma cavity using the first gas, the first gas inlet having a through hole through which a gas processed by the plasma exits the plasma cavity; and a plasma stabilizer having a shape of a circular hollow cylinder and installed on a second side of the waveguide, an axial direction of the plasma stabilizer being in parallel to a rotational axis of the first vortex flow.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

Provided is a multi-charged-particle beam writing apparatus including: an emitter emitting a charged particle beam; a first shaping aperture array substrate having a plurality of first apertures and forming first multiple beams by passing a part of the charged particle beam through the first apertures, respectively; a second shaping aperture array substrate having second apertures formed at positions corresponding to the respective first apertures and forming second multiple beams by passing at least a part of each of the first multiple beams through corresponding the second apertures, respectively; a blanking aperture array having third apertures formed at positions corresponding to the respective second apertures and including blankers disposed in the respective third apertures to perform blanking deflection on the respective beams of the corresponding second multiple beams; a movable mechanism moving at least one of the first shaping aperture array substrate and the second shaping aperture array substrate; and a controller controlling the movable mechanism.

A mounting table has a first surface for mounting jigs one by one and a second surface for mounting a ring member. An acquisition unit acquires a gap dimension between the second surface and a facing portion of the mounted jig. A measurement unit measures a lifted distance of the ring member at each of circumferential multiple locations when an upper surface of the ring member is in contact with the facing portion. A thickness calculation unit calculates, for each of the multiple locations, thickness at each of different radial positions of the ring member based on the gap dimension and the lifted distance. A misalignment calculation unit specifies a characteristic position of the ring member for each of the multiple locations based on the calculated thickness and calculate a misalignment amount between a center of a circle passing through the characteristic positions and a center of the first surface.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

A method for adjusting a primary side of an X-ray diffractometer wherein the primary side comprises a collimator, X-ray optics, an X-ray source, in particular an X-ray tube, wherein the collimator, the X-ray optics and the X-ray source are mounted directly or indirectly on a base structure, and wherein the orientation and position of the X-ray optics and the position of the X-ray source are adjusted relative to the base structure, wherein the method is characterized in that the orientation and position of the X-ray optics and the position of the X-ray tube relative to the base structure are measured and set at predetermined target values, so that with these set target values, X-ray radiation emanating from the X-ray source and conditioned by the X-ray optics is detectable at the output end of the collimator.

A multi-beam apparatus for observing a sample with high resolution and high throughput and in flexibly varying observing conditions is proposed. The apparatus uses a movable collimating lens to flexibly vary the currents of the plural probe spots without influencing the intervals thereof, a new source-conversion unit to form the plural images of the single electron source and compensate off-axis aberrations of the plural probe spots with respect to observing conditions, and a pre-beamlet-forming means to reduce the strong Coulomb effect due to the primary-electron beam.

According to one aspect of the present invention, a charged particle beam image acquisition apparatus includes a rectangular parallelepiped chamber where a target object is disposed; a primary electron optical column placed on an upper surface of the chamber so that a point of intersection between two diagonal lines on the upper surface of the chamber is located at a center of a horizontal section of the primary electron optical column, a primary charged particle beam optics irradiating the target object with a primary charged particle beam being disposed in the primary electron optical column; and a secondary electron optical column connected to a lower portion of the primary electron optical column, a secondary charged particle beam optics being disposed in the secondary electron optical column and a secondary charged particle beam passing through the secondary charged particle beam optics.

An ion milling device capable of high-speed milling is realized even for a specimen containing a material having an imide bond. Therefore, the ion milling device includes: a vacuum chamber 6 configured to hold a specimen 3 in a vacuum atmosphere; an ion gun 1 configured to irradiate the specimen with a non-focused ion beam 2; a vaporization container 17 configured to store a mixed solution 13 of a water-soluble ionic liquid and water; and nozzles 11, 12 configured to supply water vapor obtained by vaporizing the mixed solution to a vicinity of a surface of the specimen processed by the ion beam.

An apparatus may include an electrode assembly, the electrode assembly comprising a plurality of electrodes, arranged in a plurality of electrode pairs arranged to conduct an ion beam therethrough. A given electrode pair lies along a radius of an arc describing a nominal central ray trajectory, wherein a radius of a first electrode pair and an adjacent electrode pair define an angular spacing. The plurality of electrode pairs may define a plurality of angular spacings, wherein, in a first configuration, the plurality of angular spacings are not all equal. The apparatus may also include a power supply in communication with the EM, the power supply configured to independently supply voltage to the plurality of electrodes.