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:
Jun. 11, 2019

Filed:

Feb. 02, 2017
Applicant:

Jasco Corporation, Tokyo, JP;

Inventors:

Tetsuji Sunami, Tokyo, JP;

Takashi Shimamura, Tokyo, JP;

Norio Wakimoto, Tokyo, JP;

Jun Koshobu, Tokyo, JP;

Assignee:

JASCO CORPORATION, Tokyo, JP;

Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01J 5/02 (2006.01); G01J 3/45 (2006.01); G01N 21/35 (2014.01); G01J 3/28 (2006.01); G01J 3/453 (2006.01); G01N 21/31 (2006.01); G01N 21/25 (2006.01); G01N 21/00 (2006.01); G01J 3/02 (2006.01);
U.S. Cl.
CPC ...
G01J 3/45 (2013.01); G01J 3/28 (2013.01); G01J 3/453 (2013.01); G01N 21/00 (2013.01); G01N 21/25 (2013.01); G01N 21/31 (2013.01); G01N 21/35 (2013.01); G01J 3/0297 (2013.01); G01N 2021/3595 (2013.01);
Abstract

A method for measuring spectrum by Fourier-transforming an interferogram of an infrared interference wave acquired with an interferometer, including a step of over-sampling intensity signals of the interference wave at positions (D1, D2, . . . ) of a movable mirror set on the basis of a wavelength λ1 of a semi-conductor laser, and a step of interpolating intensity signals (I1', I2′, . . . ) that would be obtained when the interference wave is sampled at positions (D1′, D2′, . . . ) of the movable mirror set on the basis of a wavelength λ0 of a He—Ne laser, by using the over-sampled intensity signals (I1, I2, . . . ), for calculating the spectrum with the interferogram based on the interpolated intensity signals (I1′, I2′, . . . ) and for an efficient use of conventional stored spectrum data which are measured based on the wavelength λ0.


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