The patent badge is an abbreviated version of the USPTO patent document. The patent badge does contain a link to the full patent document.

The patent badge is an abbreviated version of the USPTO patent document. The patent badge covers the following: Patent number, Date patent was issued, Date patent was filed, Title of the patent, Applicant, Inventor, Assignee, Attorney firm, Primary examiner, Assistant examiner, CPCs, and Abstract. The patent badge does contain a link to the full patent document (in Adobe Acrobat format, aka pdf). To download or print any patent click here.

Date of Patent:
Jan. 22, 2013

Filed:

Jan. 26, 2010
Applicants:

Chie Shishido, Kawasaki, JP;

Atsushi Miyamoto, Yokohama, JP;

Mayuka Iwasaki, Yokohama, JP;

Tomofumi Nishiura, Kawasaki, JP;

Go Kotaki, Kumamoto, JP;

Inventors:

Chie Shishido, Kawasaki, JP;

Atsushi Miyamoto, Yokohama, JP;

Mayuka Iwasaki, Yokohama, JP;

Tomofumi Nishiura, Kawasaki, JP;

Go Kotaki, Kumamoto, JP;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01J 37/26 (2006.01); G01N 23/00 (2006.01); G06K 9/00 (2006.01);
U.S. Cl.
CPC ...
Abstract

A charged particle beam device enabling prevention of degradation of reproducibility of measurement caused by an increase of the beam diameter attributed to an image shift and having a function of dealing with device-to-device variation. The charged particle beam device is used for measuring the dimensions of a pattern on a specimen using a line profile obtained by detecting secondary charged particles emitted from the specimen when the specimen is scanned with a primary charged particle beam converged on the specimen. A lookup table in which the position of image shift and the variation of the beam diameter are associated is prepared in advance by actual measurement or calculation and registered. When the dimensions are measured, image processing is carried out so as to correct the line profile for the variation of the beam diameter while the lookup table is referenced, and thereby the situation where the beam diameter is effectively equal is produced irrespective of the position of the image shift. Whit this, measurement by the charged particle beam excellent reproducibility can be carried out.


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