Abstract:
An electron beam inspection apparatus images reflected electrons and cancels negative charging derived from electron-beam irradiation. Ultraviolet rays are irradiated and an irradiated area of ultraviolet rays is displayed as a photoelectron image. The photoelectron image and a reflected-electron image are displayed on a monitor while being superposed on each other, to easily grasp the positional relationship between the images and the difference in size between them. Specifically, the shape of the irradiated area of an electron beam includes the shape of the irradiated area of ultraviolet rays on a display screen. The intensity of the ultraviolet rays in the irradiated area of the electron beam is adjusted while the reflected-electron imaging conditions for the reflected-electron image are sustained. Moreover, an amount-of-ultraviolet ray adjustment mechanism is controlled on the monitor so that an amount of the ultraviolet rays is adjusted while observing a reflected-electron image obtained during ultraviolet irradiation.
Abstract:
An electron beam inspection apparatus images reflected electrons and cancels negative charging derived from electron-beam irradiation. Ultraviolet rays are irradiated and an irradiated area of ultraviolet rays is displayed as a photoelectron image. The photoelectron image and a reflected-electron image are displayed on a monitor while being superposed on each other, to easily grasp the positional relationship between the images and the difference in size between them. Specifically, the shape of the irradiated area of an electron beam includes the shape of the irradiated area of ultraviolet rays on a display screen. The intensity of the ultraviolet rays in the irradiated area of the electron beam is adjusted while the reflected-electron imaging conditions for the reflected-electron image are sustained. Moreover, an amount-of-ultraviolet ray adjustment mechanism is controlled on the monitor so that an amount of the ultraviolet rays is adjusted while observing a reflected-electron image obtained during ultraviolet irradiation.
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:
In the present invention, the structure of an electrification control electrode is changed from a grid type to a slit type and thereby shadows are not formed when a wafer is irradiated with a beam. Further, a beam forming slit is disposed ahead of an electrification control slit, thus the electrification control slit is prevented from being irradiated with an electron beam for preliminary electrification, and thereby secondary electrons which disturb the control of the electrification are inhibited from being generated. The shape of the slit is designed so that the strength of an electron beam may gradually decrease toward both the ends of an electron beam irradiation region in the longitudinal direction thereof. Furthermore, a preliminary static eliminator to remove or reduce the unevenness in an electrification potential distribution which has undesirably been formed earlier is disposed.
Abstract:
In a method for inspecting positions and types of defects on wafers with circuit patterns in the semiconductor manufacturing process, a highly sensitive inspection is made regardless of the types and materials of junctions of circuit patterns of the semiconductor devices, different kinds of defects being distinguished from one another. Further, extraordinary electrification of the circuit pattern is prevented and an area to be exposed to an electron beam is controlled evenly and at a desired voltage. Thus, this method contributes to the early setup of manufacturing processes of integrated circuits and early measures against defects, increasing the reliability and productivity of the semiconductor devices. During an inspection of positions and types of defects on a wafer with a circuit pattern in the semiconductor manufacturing process, with the use of a charged-particle beam from a charged-particle source, an optical beam from an optical source as well as a charged-particle beam are applied to a junction of the circuit pattern of the wafer placed on a wafer holder. Thus, regardless of the types and materials of circuit patterns, a highly sensitive inspection is made according to contrasts of the defects in an image captured.
Abstract:
In a method for observing or processing and analyzing the surface of a sample by irradiating a charged beam on the sample covered at least partially by an insulator film, an ultraviolet light is irradiated possibly as pulse on the sample (substrate), thereby transforming the insulator into a conductive material due to the photoconductivity effect, thereby transforming the surface of the sample (substrate) into a conductive material, so that charged particles are grounded from a grounded portion in order to prevent the charged beam from being repulsed due to charged particles of the irradiated charged beam accumulated in the insulator formed on the surface of the sample (substrate).
Abstract:
Electron or ion spectroscopy methods are commonly used for the surface analysis of insulating materials. During the illumination of the surface, electrons are emitted leaving behind a positively charged surface. The positively charged surface causes the energy of the emitted electrons to change and interferes with the analysis of their energy spectra. Conventionally, a source of neutralizing low energy electrons is directed to the illuminated region of the surface to neutralize the positive surface charge. The addition, to the non-illuminated region of the material, of a flux of positive particles or a means of emitting negative particles causes a discharge of the positive charge from the illuminated area of the material and establishes a dynamic equilibrium over the surface of the entire specimen. This permits the surface to be maintained at an arbitrarily uniform level controlled by the relative fluxes of the emitted electrons, the neutralizing electron flux, and the discharging means.