There is provided a gas analyzer apparatus including: a sample chamber which is equipped with a dielectric wall structure and into which only sample gas to be measured is introduced; a plasma generation mechanism that generates plasma inside the sample chamber, which has been depressurized, using an electric field and/or a magnetic field applied through the dielectric wall structure; and an analyzer unit that analyzes the sample gas via the generated plasma. By doing so, it is possible to provide a gas analyzer apparatus capable of accurately analyzing sample gases, even those including corrosive gas, over a long period of time.

A method comprising the irradiation of a wafer by an ion beam that passes through an implantation filter. The wafer is heated to a temperature of more than 200° C. The wafer is a semiconductor wafer including SiC, and the ion beam includes aluminum ions.

An energy spectrometer with dynamic focus for a transmission electron microscope (TEM) is disclosed herein. An example energy spectrometer and TEM at least includes a charged particle column including a projection system arranged after a sample plane, the projection system is operated in a first configuration; an energy spectrometer coupled to the charged particle column to acquire one or more energy loss spectra. The energy spectrometer including a dispersive element, a bias tube, optics for magnifying the energy loss spectrum and for correcting aberrations, and a detector arranged conjugate to a spectrum plane of the energy spectrometer, wherein the energy spectrometer further includes an optical element electrically biased to refocus at least a portion of a spectrum onto the detector, and wherein the value of the electrical bias is at least partially based on the first configuration of the charged particle column.

Semiconductor devices and methods of manufacturing semiconductor devices are described herein. A method includes implanting neutral elements into a dielectric layer, an etch stop layer, and a metal feature, the dielectric layer being disposed over the etch stop layer and the metal feature being disposed through the dielectric layer and the etch stop layer. The method further includes using a germanium gas as a source for the neutral elements and using a beam current above 6.75 mA to implant the neutral elements.

Provided herein are approaches for performing electrodynamic mass analysis with a radio frequency (RF) biased ion source to reduce ion beam energy spread. In some embodiments, a system may include an ion source including a power supply, the ion source operable to generate a plasma within a chamber housing, and an extraction power assembly including a first power supply and a second power supply electrically coupled with the chamber housing of the ion source, wherein the first power supply and the second power supply are operable to bias the chamber housing of the ion source with a time modulated voltage to extract an ion beam from the ion source. The system may further include an electrodynamic mass analysis (EDMA) assembly operable to receive the ion beam and perform mass analysis on the ion beam.

Provided herein are approaches for in-situ plasma cleaning of ion beam optics. In one approach, a system includes a component (e.g., a beam-line component) of an ion implanter processing chamber. The system further includes a power supply for supplying a first voltage and first current to the component during a processing mode and a second voltage and second current to the component during a cleaning mode. The second voltage and current are applied to one or more conductive beam optics of the component, individually, to selectively generate plasma around one or more of the one or more conductive beam optics. The system may further include a flow controller for adjusting an injection rate of an etchant gas supplied to the beam-line component, and a vacuum pump for adjusting pressure of an environment of the beam-line component.

An electron optical module for providing an off-axial electron beam with a tunable coma, according to the present disclosure includes a structure positioned downstream of an electron source and an electron lens assembly positioned between the structure and the electron source. The structure generates a decelerating electric field, and is positioned to prevent the passage of electrons along the optical axis of the electron lens assembly. The electron optical module further includes a micro-lens that is not positioned on the optical axis of the electron lens assembly and is configured to apply a lensing effect to an off-axial election beam. Aberrations applied to the off-axial electron beam by the micro-lens and the electron lens assembly combine so that a coma of the off-axial beam has a desired value in a downstream plane.

Some embodiments are related to a method of or apparatus for forming an image of a buried structure that includes: emitting primary charged particles from a source; receiving a plurality of secondary charged particles from a sample; and forming an image based on received secondary charged particles that have an energy within a first range.

A scanning electron microscope (SEM) includes an electron gun, a deflector, an objective lens, first and second detectors each configured to detect emission electrons emitted from the wafer based on the input electron beam being irradiated on the wafer, a first energy filter configured to block electrons having energy less than a first energy among emission electrons emitted from a wafer based on an input electron beam from being detected by the first detector, and a second energy filter configured to block electrons having energy less than second energy among the emission electrons from being detected by the second detector.

Some disclosed embodiments include an electron detector comprising: a first semiconductor layer having a first portion and a second portion; a second semiconductor layer; a third semiconductor layer; a PIN region formed by the first, second, and third semiconductor layers; a power supply configured to apply a reverse bias between the first and the third semiconductor layers; and a depletion region formed within the PIN region by the reverse bias and configured to generate a detector signal based on a first subset of the plurality of signal electrons captured within the depletion region, wherein the second portion of the first semiconductor layer is not depleted and is configured to provide an energy barrier to block a second subset of the plurality of signal electrons and to allow the first subset of the plurality of signal electrons to pass through to reach the depletion region.