Abstract:
An object of the present invention is to provide an ultimate analyzer which can display an element distribution image of an object to be analyzed with high contrast to determine the positions of the element distribution with high accuracy, and a scanning transmission electron microscope and a method of analyzing elements using the ultimate analyzer. The present invention exists in an ultimate analyzer comprising a scattered electron beam detector for detecting an electron beam scattered by an object to be analyzed; an electron spectrometer for energy dispersing an electron beam transmitted through the object to be analyzed; an electron beam detector for detecting said dispersed electron beam; and a control unit for analyzing elements of the object to be analyzed based on an output signal of the electron beam detected by the electron beam detector and an output signal of the electron beam detected by the scattered electron beam detector. Further, the present invention exists in a scanning transmission electron microscope comprising the above ultimate analyzer; an electron beam source; an electron beam scanning coil; a scattered electron beam detector; objective lenses; a focusing lens; a magnifying magnetic field lens; and a focus adjusting electromagnetic lens. Furthermore, the ultimate analyzer or the scanning transmission electron microscope may comprises a control unit which makes it possible that both of an image of element distribution and an STEM image detected and formed by the scatted electron beam detector are observed at a time in real time, and the image of element distribution is corrected by the STEM image detected and formed by the scattered electron beam detector.
Abstract:
A high data-rate electron beam spot-grid array imaging system is provided that overcomes the low resolution and severe linearity requirements of prior art systems. Embodiments include an imaging system comprising an electron beam generator for simultaneously irradiating an array of spots spaced apart from each other on a surface of an object to be imaged, and a detector for collecting backscattered and/or secondary electrons emitted as a result of the interaction of the spots with the surface of the object to form an image of the irradiated portions of the object surface. A mechanical system moves the substrate in a direction which is nearly parallel to an axis of the array of spots such that as the substrate is moved across the spot array in the scan direction (the y-direction) the spots trace a path which leaves no gaps in the mechanical cross-scan direction (the x-direction). A compensator, such as a servo or a movable mirror, compensates for mechanical inaccuracies in the moving stage, thereby increasing imaging accuracy. In other embodiments, multiple detectors placed at different angles to the substrate collect electrons to provide multiple perspective imaging of the substrate surface.
Abstract:
A detector for scanning electron microscopes with high pressure in the sample chamber has a first electrode for accelerating electrons emergent from a sample received on the sample holder, and at least one second electrode, the end of which directed toward the sample holder is at a smaller distance from the sample holder than the first electrode, and is at a potential between the potential of the first electrode and the potential of the beam guiding tube. The volume of the secondary electron cascade is increased by the second electrode. In an alternative embodiment for a gas scintillation detector, there is adjoined to a region of high secondary electron amplification, an elongate region in which the amplification factor for secondary electrons is approximately 1. The first region serves for the production of a relatively large electron current and the second, elongate, region for the production of a strong photon signal while maintaining the photon current.
Abstract:
A method and system for measuring lithographic image foreshortening. The method comprises the steps of providing a critical dimension scanning electron microscope, and using that critical dimension scanning electron microscope to measure lithographic image foreshortening. Preferably, a defined feature is formed using a lithographic process, and the critical dimension scanning electron microscope is used to measure foreshortening of that feature. For example, the feature may be a line, and the critical dimension scanning electron microscope may be used to measure foreshortening of the line. Also, the feature may be two arrays of lines, and the critical dimension scanning electron microscope may be used to measure the separation distance between the arrays. That separation distance may be used to determine a focus of the lithographic process.
Abstract:
Disclosed are methods and apparatus for simultaneously flooding a sample (e.g., a semiconductor wafer) to control charge and inspecting the sample. The apparatus includes a charged particle beam generator arranged to generate a charged particle beam substantially towards a first portion of the sample and a flood gun for generating a second beam towards a second portion of the sample. The second beam is generated substantially simultaneously with the inspection beam. The apparatus further includes a detector arranged to detect charged particles originating from the sample portion. In a further implementation, the apparatus further includes an image generator for generating an image of the first portion of the sample from the detected particles. In one embodiment, the sample is a semiconductor wafer. In a method aspect, a first area of a sample is flooded with a flood beam to control charge on a surface of the sample. A second area of the sample is inspected with an inspection beam. The second area comprises at least a portion of the first area flooded by the flood beam. The inspection beam moves in tandem with the flood beam. In another aspect of the present invention, methods and apparatus are provided for controlling the charge buildup of an area of the sample by an electrode having a voltage applied to it and through which the flood beam and charged particles emitted from the area of the sample can pass.
Abstract:
The present invention aims to prevent degradation in performance due to a change in image quality and deflection distortions or the like in the vicinity of both ends of a scan area and detect a defect in a sample such as a semiconductor wafer or the like with high accuracy when the defect is inspected by use of an electron beam image, and allow a monitor to confirm an image area to be checked. The present invention is provided with means for comparing and checking defects in the sample, based on an image signal in which the neighborhoods of both ends of horizontal and vertical scan areas are respectively deleted under control of a blanking signal and a vertical synchronizing signal.
Abstract:
Problems encountered in the conventional inspection method and the conventional apparatus adopting the method are solved by the present invention using an electron beam by providing a novel inspection method and an inspection apparatus adopting the novel method which are capable of increasing the speed to scan a specimen such as a semiconductor wafer. The inspection novel method provided by the present invention comprises the steps of: generating an electron beam; converging the generated electron beam on a specimen by using an objective lens; scanning the specimen by using the converged electron beam; continuously moving the specimen during scanning; detecting charged particles emanating from the specimen at a location between the specimen and the objective lens and converting the detected charged particles into an electrical signal; storing picture information conveyed by the electrical signal; comparing a picture with another by using the stored picture information; and detecting a defect of the specimen.
Abstract:
An electron beam inspection system of the image projection type includes a primary electron optical system for shaping an electron beam emitted from an electron gun into a rectangular configuration and applying the shaped electron beam to a sample surface to be inspected. A secondary electron optical system converges secondary electrons emitted from the sample. A detector converts the converged secondary electrons into an optical image through a fluorescent screen and focuses the image to a line sensor. A controller controls the charge transfer time of the line sensor at which the picked-up line image is transferred between each pair of adjacent pixel rows provided in the line sensor in association with the moving speed of a stage for moving the sample.
Abstract:
A main control system 34 prepares, in advance, a voltage map showing the amount of focus deviation of a secondary electron beam B2 at a detection surface of an electron beam detector 30 corresponding with the amount of charge-up generated on a sample 4 upon irradiation with a primary electron beam B1, and stores this voltage map in a storage device 43. During an observation, the main control system 34 reads the voltage map stored in the storage device 43 and corrects the focal position of the secondary electron beam B2 by controlling either the voltage applied to the secondary optical system 20 or the voltage applied to the sample 4. As a result, focal position deviations resulting from charge-up generated on the sample being observed can be corrected without causing inconvenience to an operator.
Abstract:
The present invention is intended to prevent the deterioration of resolution due to increase in off-axis aberration resulting from the deviation of a primary electron bean from the optical axis of a scanning electron microscope. A scanning electron microscope is provided with an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector disposed at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed and dimensions can be measured in a high accuracy. The SEM is able to achieving precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.