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:
May. 03, 2022

Filed:

Mar. 01, 2019
Applicant:

Tasmit, Inc., Yokohama, JP;

Inventors:

Makoto Kato, Yokohama, JP;

Sumio Sasaki, Yokohama, JP;

Yukihiro Tanaka, Yokohama, JP;

Yuichiro Yamazaki, Yokohama, JP;

Assignee:

Tasmit, Inc., Yokohama, JP;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01J 37/244 (2006.01); H01J 37/28 (2006.01);
U.S. Cl.
CPC ...
H01J 37/244 (2013.01); H01J 37/28 (2013.01); H01J 2237/049 (2013.01); H01J 2237/15 (2013.01); H01J 2237/1532 (2013.01); H01J 2237/2446 (2013.01); H01J 2237/24475 (2013.01); H01J 2237/24485 (2013.01);
Abstract

The present invention relates to an apparatus and method for analyzing the energy of backscattered electrons generated from a specimen. The apparatus includes: an electron beam source () for generating a primary electron beam; an electron optical system () configured to direct the primary electron beam to a specimen while focusing and deflecting the primary electron beam; and an energy analyzing system configured to detect an energy spectrum of backscattered electrons emitted from the specimen. The energy analyzing system includes: a Wien filter () configured to disperse the backscattered electrons; a detector () configured to measure the energy spectrum of the backscattered electrons dispersed by the Wien filter (); and an operation controller () configured to change an intensity of a quadrupole field of the Wien filter (), while moving a detecting position of the detector () for the backscattered electrons in synchronization with the change in the intensity of the quadrupole field.


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