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:
Aug. 18, 2020

Filed:

Jan. 03, 2019
Applicant:

Tokyo Electron Limited, Tokyo, JP;

Inventor:

Tatsuo Matsudo, Yamanashi, JP;

Assignee:
Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01B 11/06 (2006.01); H01J 37/32 (2006.01); G01K 5/48 (2006.01); G01B 9/02 (2006.01);
U.S. Cl.
CPC ...
G01B 11/0675 (2013.01); G01B 9/0209 (2013.01); G01B 9/02019 (2013.01); G01B 9/02021 (2013.01); G01B 9/02025 (2013.01); G01B 9/02044 (2013.01); G01K 5/48 (2013.01); H01J 37/3288 (2013.01); H01J 37/32449 (2013.01); H01J 37/32522 (2013.01); H01J 37/32642 (2013.01); H01J 37/32724 (2013.01);
Abstract

A wear amount measuring apparatus includes a light source, a light transmission unit, a first and a second irradiation unit, a spectroscope and an analysis unit. The light transmission unit splits a low-coherence light from the light source into a first and a second low-coherence light. The first and the second irradiation units irradiate the first and the second low-coherence light to the component to receive reflected lights from the component. The light transmission unit transmits the reflected lights received by the first irradiation unit and the second irradiation unit to the spectroscope. The spectroscope configured to detect intensity distribution of the reflected lights from the first and the second irradiation unit. The analysis unit calculates a thickness difference between a thickness of the component at the first measuring point and that at the second measuring point by performing Fourier transform on the intensity distribution.


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