Abstract:
A spectrometer having an electron beam generator for generating an electron beam that is directed at a sample. An electron beam positioner directs the electron beam onto a position of the sample, and thereby produces a secondary emitted stream from the sample, where the secondary emitted stream includes at least one of electrons and x-rays. An secondary emitted stream positioner positions the secondary emitted stream onto a detector array, which receives the secondary emitted stream and detects both the amounts and the received positions of the secondary emitted stream. A modulator modulates the electron beam that is directed onto the sample, and thereby sweeps the electron beam between a first position and a second position on the sample. An extractor is in signal communication with both the modulator and the detector array, and extracts a differential signal that represents a difference between the signals that are received from the first position and the signals that are received from the second position.
Abstract:
A spherical aberration correction decelerating lens corrects a spherical aberration occurring in an electron beam or an ion beam (hereinafter, referred to as “beam”) emitted from a predetermined object plane position with a certain divergence angle, and said spherical aberration correction decelerating lens comprises at least two electrodes, each of which is constituted of a surface of a solid of revolution whose central axis coincides with an optical axis and each of which receives an intentionally set voltage applied by an external power supply, wherein at least one of the electrodes includes one or more meshes (M) which has a concaved shape opposite to an object plane (P0) and which is constituted of a surface of a solid of revolution so that a central axis of the concaved shape coincides with the optical axis, and a voltage applied to each of the electrodes causes the beam to be decelerated and causes formation of a decelerating convergence field for correcting the spherical aberration occurring in the beam. This makes it possible to provide a spherical aberration correction decelerating lens which converges a beam, emitted from the sample and having high energy and a large divergence angle, onto an image plane.
Abstract:
One embodiment relates to a scanning electron beam apparatus having curved electron-optical axes. An electron gun and illumination electron optics are configured to generate a primary electron beam along a first axis. Objective electron optics is configured about a second axis to receive the primary electron beam, to focus the incident electron beam onto the substrate, and to retrieve an emitted beam of scattered electrons from the substrate. Detection electron optics is configured about a third axis to receive the emitted beam and to focus the emitted beam onto a detector. A beam separator is coupled to and interconnecting the illumination electron optics, the objective electron optics, and the detection electron optics in such a way that there is a same angle between the first and second axes as between the second and third axes. A beam deflector is configured to controllably scan the primary electron beam across the substrate and to de-scan the emitted electron beam. Other embodiments are also disclosed.
Abstract:
There is disclosed a TEM (transmission electron microscope)/SEM (scanning electron microscope) instrument capable of x-ray mapping with automated correction of specimen drift. In x-ray mapping, an SE (secondary electron) image of a scanned region on a specimen is stored as a reference image in memory in the first scan. After a given number of scans are made, an SE image is derived and subject to comparison. The cross-correlation function between each image to be compared and the reference image is calculated to find the direction and amount of the deviation of each image from the reference image. The electron beam deflection system is so controlled as to cancel the deviation, thus correcting the specimen drift. Whenever a given number of scans are made, the correction of the specimen drift is performed.