Abstract:
Provided is a pattern inspection apparatus including: a charge formation means which forms charge on a surface of a substrate (7) by generating an electron beam from a second electron source (20) which is different from an electron source (I) which generates an electron beam before irradiating an electron beam (3), a current measuring means (34) which measures a value of current flowing in the substrate while the charge is formed on the surface of the substrate by the charge formation means; and an adjustment means (37) which adjusts the charge formed by the charge formation means so that the value of the current measured by the current measuring means is a predetermined target value. Provided is also a pattern inspection method which uses the pattern inspection apparatus. Thus, it is possible to easily set an optimal condition of precharge executed before inspection of a pattern formed by a semiconductor apparatus manufacturing process and automatically inspection whether the precharge is good. Then, the inspection result is fed back to the operation afterward. This prevents lowering of the reliability of the inspection result and always enables a stable inspection.
Abstract:
To make it possible to observe the bottom of a contact hole and internal wires, in observation of the contact hole 102, by scanning it at a predetermined acceleration voltage, the positive charge 106 is formed on the surface of the insulator 101, and the secondary electrons 104 are attracted in the hole by this electric field, and the hole is continuously scanned at an acceleration voltage different from the acceleration voltage, and the sample is observed. When the wires embedded in the insulator are to be observed, by observing the insulator at a predetermined acceleration voltage, an electron beam is allowed to enter the sample, and the sample is continuously scanned at an acceleration voltage different from the acceleration voltage, and hence the existence of wires is reflected as a change in the charge of the surface, and it is observed. In either case, the acceleration voltage before observation is different from the one during observation, and the sample surface is temporarily radiated at an acceleration voltage positively generating a positive or negative charge, and thereafter, the acceleration voltage is returned to a one suited to observation, and the sample is observed.
Abstract:
Methods and a system of an ion implantation system are disclosed that are capable of increasing beam current above a maximum kinetic energy of a first charge state from an ion source without changing the charge state at the ion source. Positive ions having a first positive charge state are selected into an accelerator. The positive ions of the first positive charge state are accelerated in acceleration stages and stripped to convert them to positive ions of a second charge state. A second kinetic energy level higher than the maximum kinetic energy level of the first charge state can be obtained.
Abstract:
A semiconductor device analyzer comprises a function of radiating a charged particle beam on a sample and displaying a detected secondary electron image according to detected secondary electron intensity. A charged particle beam is radiated according to a first radiation pattern onto a semiconductor device that is to be analyzed, and a charge is injected. Next, a charge accumulation state of the semiconductor device that is to be analyzed is observed. A location where the charge accumulation state is abnormal can be detected as a defect location in the semiconductor device. A defect location is identified easily.
Abstract:
A surface-potential distribution measuring apparatus includes an electron gun, an electron-beam optical system, an electron-emission panel, a detector, and a control system. The electron-beam optical system is located between the electron gun and a sample, and focuses a beam of electrons emitted from the electron gun to the surface of the sample. The electron-emission panel is located near the sample to be collided with at least part of the electrons via the sample, and emits secondary electrons corresponding to the number of collided electrons. The detector detects at least part of the secondary electrons. The control system obtains potential distribution on the surface of the sample based on a detection result obtained by the detector.
Abstract:
An ion implanter includes an electrostatic chuck. The electrostatic chuck is configured to repel charged particles from a surface of the electrostatic chuck to limit deposits of the charged particles on the surface when the electrostatic chuck is not supporting any workpiece. An electrostatic chuck including a dielectric layer and at least one electrode is also provided. The at least one electrode is configured to accept a DC voltage signal to produce a first charge to repel charged particles from the dielectric layer when the dielectric layer is not supporting any workpiece to thereby limit deposits of the charged particles on the dielectric layer.
Abstract:
The present invention provides a mirror electron projection (MPJ) type (SEPJ type included) scanning electron beam apparatus that is capable of performing condition setup, and a method and apparatus for inspecting pattern defects with the scanning electron beam apparatus. A mirror electron projection type defect inspection apparatus, which comprises a charging device for emitting a charging electron beam, electron beam irradiation means for shedding a mirror electron projection electron beam onto an inspection region near which an electrical potential distribution is formed, detection means for detecting secondary electrons or reflected electrons generated from a surface and proximity of the specimen, and defect detection means for detecting a defect by processing a mirror image signal that is detected by the detection means, includes irradiation condition optimization means for optimizing charging electron beam irradiation conditions.
Abstract:
A surface of an insulating substrate is charged to a target potential. In one embodiment, the surface is flooded with a higher-energy electron beam such that the electron yield is greater than one. Subsequently, the surface is flooded with a lower-energy electron beam such that the electron yield is less than one. In another embodiment, the substrate is provided with the surface in a state at an approximate initial potential above the target potential. The surface is then flooded with charged particle such that the charge yield of scattered particles is less than one, such that a steady state is reached at which the target potential is achieved. Another embodiment pertains to an apparatus for charging a surface of an insulating is substrate to a target potential.
Abstract:
One embodiment disclosed relates to a method of setting a surface charge of an area on a substrate to a desired level. The substrate is held on a stage, and a stage bias voltage applied to the stage is controlled. A flood of electrons is directed to the area. The stage bias voltage is controlled such that the surface charge of the area reaches an equilibrium at the desired level. Another embodiment disclosed relates to a method of auto-focusing a main electron beam incident upon an imaging area of a substrate. A monitor electron beam is generated and directed towards a monitoring area of the substrate at a non-perpendicular incidence angle. An in-focus band in data collected from the monitor beam is detected. The focal length of an objective lens focusing the main beam is adjusted based upon a position of the in-focus band.
Abstract:
Mapping electron microscopes are disclosed in which the amount of charging of the specimen is controlled to between a minimum amount needed to view an image and a maximum amount beyond which a viewable image cannot be obtained that has low distortion or that does not result in specimen damage. Multiple irradiation-electron beams, or multiple segments of a single irradiation-electron beam, are directed to a specimen surface. The irradiation beams (or segments) are decelerated by a retarding voltage applied by a cathode lens and are incident on the specimen surface. The respective current and incident energy of each irradiation beam (or segment thereof) are controlled independently to a predetermined relationship so as to impart predetermined amounts of charging to different insulator regions of the specimen.