Abstract:
Disclosed is a charged particle beam device, wherein multibeam secondary electron detectors (121a, 121b, 121c) and a single beam detector (140; 640) are provided, and under the control of a system control unit (135), an optical system control circuit (139) controls a lens and a beam selecting diaphragm (141) and switches the electrooptical conditions between those for multibeam mode and those for single beam mode, thereby one charged particle beam device can be operated as a multibeam charged particle device and a single beam charged particle device by switching. Thus, observation conditions are flexibly changed in accordance with an object to be observed, and a sample can be observed with a high accuracy and high efficiency.
Abstract:
Provided is a multi-beam type charged particle beam applied apparatus in an implementable configuration, capable of achieving both high detection accuracy of secondary charged particles and high speed of processing characteristically different specimens. An aperture array (111) includes plural aperture patterns. A deflector (109) for selecting an aperture pattern through which a primary beam passes is disposed at the position of a charged particle source image created between an electron gun (102), i.e., a charged particle source, and the aperture array (111). At the time of charge-control beam illumination and at the time of signal-detection beam illumination, an aperture pattern of the aperture array (111) is selected, and conditions of a lens array (112), surface electric-field control electrode (118) and the like are switched in synchronization with each beam scanning. Thus, the charges are controlled and the signals are detected at different timings under suitable conditions, respectively.
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 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. 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 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:
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
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:
In order to measure an aberration of a charged particle beam optical system, an aberration measuring machine includes a charged particle generating unit adapted to make a plurality of charged particle beams strike the object plane of the charged particle beam optical system at different incident angles, and a detecting unit adapted to detect a position where the plurality of charged particle beams form images on the image surface of the charged particle beam optical system. The charged particle generating unit includes electron optical systems corresponding to the charged particle beams and an aperture stop to make the charged particle beams corresponding to pupil positions of the electron optical systems incident on the object plane at different incident angles.
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.