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.

Abstract: A charged particle beam apparatus that can achieve both high defect-detection sensitivity and high inspection speed for a sample with various properties in a multi-beam type semiconductor inspection apparatus. The allocation of the primary beam on the sample is made changeable, and furthermore, the beam allocation for performing the inspection at the optimum inspection specifications and at high speed is selected based on the property of the sample. In addition, many optical parameters and apparatus parameters are optimized. Furthermore, the properties of the selected primary beam are measured and adjusted.

Abstract: A charged particle beam microscope device of the present invention is configured such that in a diffraction pattern obtained by radiating a parallel charged particle beam onto a sample (22) having a known structure, a distance (r) between spots of a diffraction pattern, which reflects the structure of the sample, is measured, and the variation of a distance (L) between the sample and a detector, which depends on a diffraction angle (?), is corrected. This enables the correction of distortion that varies with an off-axis distance from the optical axis in a diffraction pattern, and a high precision structural analysis by performing accurately analyzing the spot positions of the diffraction pattern.

Abstract: A plurality of primary beams are formed from a single electron source, the surface charge of a sample is controlled by at least one primary beam, and at the same time, the inspection of the sample is conducted using a primary beam other than this. Also, for an exposure area of the primary beam for surface charge control and an exposure area of the primary beam for the inspection, the surface electric field strength is set individually. Also, the current of the primary beam for surface charge control and the interval between the primary beam for surface charge control and the primary beam for inspection are controlled.

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.

Abstract: A plurality of primary beams are formed from a single electron source, the surface charge of a sample is controlled by at least one primary beam, and at the same time, the inspection of the sample is conducted using a primary beam other than this. Also, for an exposure area of the primary beam for surface charge control and an exposure area of the primary beam for the inspection, the surface electric field strength is set individually. Also, the current of the primary beam for surface charge control and the interval between the primary beam for surface charge control and the primary beam for inspection are controlled.

Abstract: With a multi-beam type charged particle beam apparatus, and a projection charged particle beam apparatus, in the case of off-axial aberration corrector, there is the need for preparing a multitude of multipoles, and power supply sources in numbers corresponding to the number of the multipoles need be prepared. In order to solve this problem as described, a charged particle beam apparatus is provided with at least one aberration corrector wherein the number of the multipoles required in the past is decreased by about a half by disposing an electrostatic mirror in an electron optical system.

Abstract: In an electron microscope to which a phase retrieval method is applied, an image size determined by a pixel size p of a diffraction pattern, a camera length L, and a wavelength ? of an illumination beam is allowed to have a certain relation with an illumination area on a specimen. Further, a beam illumination area or a scanning area of a deflector when a magnified image is observed is set by an illumination adjustment system, so that an image size when the magnified image is used for the phase retrieval method is allowed to have a certain relation with the image size determined by the pixel size of the diffraction pattern, the camera length, and the wavelength of the illumination beam. Accordingly, the information of the diffraction pattern is substantially equal to an object image to be reconstructed.

Abstract: In a multi-charged-particle-beam apparatus, when an electric field and voltage on a surface of a specimen are varied according to characteristics of the specimen, a layout of plural primary beams on the surface of the specimen and a layout of plural secondary beams on each detector vary. Then, calibration is executed to adjust the primary beams on the surface of the specimen to an ideal layout corresponding to the variation of operating conditions including inspecting conditions such as an electric field on the surface and voltage applied to the specimen. The layout of the primary beams on the surface of the specimen is acquired as images displayed on a display of reference marks on the stage. Variance with an ideal state of the reference marks is measured based upon these images and is corrected by the adjustment of a primary electron optics system and others.

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.

Abstract: A charged particle beam apparatus that can achieve both high defect-detection sensitivity and high inspection speed for a sample with various properties in a multi-beam type semiconductor inspection apparatus. The allocation of the primary beam on the sample is made changeable, and furthermore, the beam allocation for performing the inspection at the optimum inspection specifications and at high speed is selected based on the property of the sample. In addition, many optical parameters and apparatus parameters are optimized. Furthermore, the properties of the selected primary beam are measured and adjusted.

Abstract: A technology capable of reducing the influence of the noise overlapped in a long transmission line when accurately measuring weak beam current in an electron beam writing system and capable of accurately and efficiently measuring weak beam current in a beam writing system using multiple beams is provided. With using a switch for connecting and disconnecting an electron beam detecting device and a detected signal line, the electron beam detecting device is disconnected from the detected signal line to accumulate the detected signals in the electron beam detecting device during the beam current measurement. Simultaneously with the finish of the measurement, the electron beam detecting device and the detected signal line are connected to measure the accumulated signals. Also, in order to simultaneously perform the measurement method, a plurality of electron beam detecting devices and switches are used to simultaneously measure a plurality of electron beams with high accuracy.

Abstract: An electron beam writing technology which enables highly accurate deflection correction of a minute field used in an electron beam writing system is provided. In this system, a function to move an electron beam by a deflection means through high-speed deflection scanning so as to repeat formation of a cyclic patterned electron beam and a function to move the patterned electron beam on cyclic correction marks by the deflection means through low-speed deflection scanning in synchronization with one cycle of the repetition are provided, and reflected electrons or secondary electrons emitted from the correction marks and the vicinity thereof or transmitted electrons transmitted through the correction marks in the low-speed deflection scanning are detected so as to correct the position or deflection amount of the electron beam based on the detection result.

Abstract: A charged particle beam lithography machine for exposing a target exposure surface by using a plurality of charged particle beams.

Abstract: This invention provides a charged particle beam apparatus that can makes reduction in off axis aberration and separate detection of secondary beams to be compatible. The charged particle beam apparatus has: an electron optics that forms a plurality of primary charged particle beams, projects them on a specimen, and makes them scan the specimen with a first deflector; a plurality of detectors that individually detect a plurality of secondary charged particle beams produced from the plurality of locations of the specimen by irradiation of the plurality of primary charged particle beams; and a voltage source for applying a voltage to the specimen.

Abstract: In a mold in which a pattern is formed of a fine concavo-convex shape, two or more of alignment marks for determining a relative positional relation between a substrate and a mold are formed concentrically. Moreover, a damaged mark is identified from the positional information and shape of the respective marks, and an alignment between the mold and the substrate to which a resin film is applied is carried out excluding the damaged mark.

Abstract: An aberration adjusting method of a charged particle beam optical system. The method includes an aberration measuring step of measuring N aberrations of the charged particle beam optical system, an aberration sensitivity acquiring step of changing M control amounts to control optical elements included in the charged particle beam optical system, obtaining variations of the N aberrations by executing the aberration measuring step, and obtaining aberration sensitivities of the M control amounts. The method further includes a control amount deciding step of deciding the M control amounts on the basis of the N aberrations and the aberration sensitivities of the M control amounts to set the N aberrations to target aberrations. The aberration is a displacement of each image height of charged particles beams. The control amount is an amount for controlling a position of the charged particle beams, and M<N, in which M and N are positive integers.

Abstract: An electron gun includes a cathode portion which emits electrons, an anode portion which accelerates the emission electrons, a bias portion which is arranged between the cathode portion and the anode portion and controls trajectories of the emission electrons, a shielding portion which is arranged below the anode portion and shields some of the emission electrons, and a cooling portion which cools the shielding portion. The bias portion controls the trajectories of the electrons so as to form a crossover between the bias portion and the anode portion, and prevents the electrons from emitting on the anode portion.

Abstract: A multi-electron beam exposure method and apparatus, wherein electron beams are applied to a sample surface mounted on a traveling sample stage to perform repeated exposure of chip patterns. An exposure region of the sample surface is partitioned into multiple stripe regions having a width in an x-axis direction, and each of the multiple stripe regions is further partitioned into multiple main fields having a width in a y-axis direction. At least one of the widths of the main fields in the x- and y-axis directions is set to a value, and exposure pattern data for one chip based on the partitioned main fields is stored as a unit. The stored exposure pattern data is readout a number of times corresponding to the number of chips repeatedly, and each electron beam provides repeated exposure of same regions of the chips.

Abstract: An electron beam writing technology which enables highly accurate deflection correction of a minute field used in an electron beam writing system is provided. In this system, a function to move an electron beam by a deflection means through high-speed deflection scanning so as to repeat formation of a cyclic patterned electron beam and a function to move the patterned electron beam on cyclic correction marks by the deflection means through low-speed deflection scanning in synchronization with one cycle of the repetition are provided, and reflected electrons or secondary electrons emitted from the correction marks and the vicinity thereof or transmitted electrons transmitted through the correction marks in the low-speed deflection scanning are detected so as to correct the position or deflection amount of the electron beam based on the detection result.