Patent classifications
H01J2237/063
Method and Apparatus for Plasma Processing
A method of processing includes directing an electron beam comprising ballistic electrons from an electron source towards a peripheral region of a substrate to be processed. The peripheral region surrounds a central region of the substrate. The electron beam may be directed such that the ballistic electrons impinge on the peripheral region and not on the central region of the substrate. The ballistic electrons may stimulate chemical reactions on the substrate. The method may include placing the substrate on a substrate holder disposed within a vacuum chamber. The method may also include generating the electron beam from a plasma in the vacuum chamber. The method may further include processing the substrate with ions from the plasma.
APPARATUS AND METHOD FOR DEPOSITING HARD CARBON LAYERS
An apparatus and method for depositing a carbon layer includes an arc discharge is formed between an electron source and an evaporation material by means of a first power supply device. The negative terminal of the first power supply device is connected in an electrically conducting manner to the electron source and the positive terminal of the first power supply device is connected in an electrically conducting manner to the evaporation material. A permanent magnet system and a solenoid coil are arranged in a rotationally symmetrical manner around the evaporation material. The evaporation material is formed as a graphite rod which is surrounded by at least one heat-insulating element at least on the rod end to be evaporated of the graphite rod.
Method and apparatus for plasma processing
In an embodiment, a plasma processing system includes a vacuum chamber, a substrate holder configured to hold a substrate to be processed where the substrate holder is disposed in the vacuum chamber. The system further includes an electron source disposed above a peripheral region of the substrate holder, the electron source being configured to generate an electron beam towards the peripheral region of the substrate holder.
LOW ENERGY ELECTRON MICROSCOPY
The disclosure relates to a low energy electron microscopy. The electron microscopy includes a vacuum chamber; an electron gun used to emit electron beam; a diffraction chamber; an imaging device; a sample holder used to fix two-dimensional nanomaterial sample; a vacuum pumping device; and a control computer. The electron beam transmits the sample to form a transmission electron beam and diffraction electron beam. The control computer includes a switching module to switch the work mode between a large beam spot diffraction imaging mode and small beam spot diffraction imaging mode.
Multi-Stage/Multi-Chamber Electron-Beam Inspection System
Techniques for yield management in semiconductor inspection systems are described. According to one aspect of the present invention, columns of sensing mechanism are configured with different functions, weights and performances to inspect a sample to significantly reduce the time that would be otherwise needed when all the columns were equally applied.
Individually switched field emission arrays
An electron beam apparatus is disclosed that includes a plurality of current source elements disposed in at least one field emitter array. Each current source element can be a gated vertical transistor, an ungated vertical transistor, or a current controlled channel that is proximate to an optically-modulated current source. The electron beam apparatus includes a plurality of field emitter tips, each field emitter tip of the plurality of field emitter tips being coupled to a current source element of the plurality of current source elements. The electron beam apparatus is configured to allow selective activation of one or more of the current source elements.
Method of recording an image using a particle microscope
A method, including: recording plural images of an object by scanning plural particle beams across the object and detecting signals generated by the particle beams, wherein the plural particle beams are generated by a multi-beam particle microscope; determining plural regions of interest; determining plural image regions in each of the recorded images; determining plural displacement vectors; and determining image distortions based on image data of the recorded images and the determined displacement vectors.
Height measuring device, charged particle beam apparatus, and height measuring method
A height measuring device includes a light source that emits light in a direction oblique to a top surface of a specimen, a slit that shapes the light from the light source to form a slit image on the specimen, an imaging element that detects reflected light reflected by the specimen, and an arithmetic unit. The arithmetic unit: identifies a slit image of the reflected light reflected by the top surface of the specimen from among a plurality of slit images based on respective positions of the plurality of slit images on a detection surface of the imaging element; and determines the height of the top surface of the specimen based on the position of the slit image of the reflected light reflected by the top surface of the specimen on the detection surface.
HYBRID ION SOURCE FOR ALUMINUM ION GENERATION USING ORGANOALUMINIUM COMPOUNDS AND A SOLID TARGET
An ion source that is capable of different modes of operation is disclosed. A solid target may be disposed in the arc chamber. The ion source may have several gas inlets, in communication with different gasses. When operating in a first mode, the ion source may supply a first gas, such as a halogen containing gas. When operating in a second mode, the ion source may supply an organoaluminium gas. Ions having single charges may be created in the first mode, while ions having multiple charges may be created in the second mode. In some embodiments, the solid target may be retractable.
CHARGED PARTICLE SOURCE
This invention provides a charged particle source, which comprises an emitter and means fo generating a magnetic field distribution. The magnetic field distribution is minimum, about zero, or preferred zero at the tip of the emitter, and along the optical axis is maximum away from the tip immediately. In a preferred embodiment, the magnetic field distribution is provided by dual magnetic lens which provides an anti-symmetric magnetic field at the tip, such that magnetic field at the tip is zero.