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. 15, 2018

Filed:

Aug. 05, 2014
Applicants:

Fuji Kagaku Corporation, Osaka, JP;

National Institute for Materials Science, Ibarki, JP;

Inventors:

Satoshi Kawanaka, Osaka, JP;

Fumio Uchida, Osaka, JP;

Tsutomu Sawada, Ibaraki, JP;

Seiichi Furumi, Ibaraki, JP;

Hiroshi Fudoji, Ibaraki, JP;

Assignees:
Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01B 11/24 (2006.01); G02B 5/18 (2006.01); G02B 5/28 (2006.01); G02B 1/04 (2006.01); G02B 1/00 (2006.01); G02B 5/20 (2006.01); G02B 5/26 (2006.01);
U.S. Cl.
CPC ...
G01B 11/24 (2013.01); G02B 1/005 (2013.01); G02B 1/04 (2013.01); G02B 5/1861 (2013.01); G02B 5/207 (2013.01); G02B 5/28 (2013.01); G02B 5/26 (2013.01);
Abstract

Provided are: a sheet of colloidal crystals immobilized in resin exhibiting intense structural color, enabled to be observed easily from a squarely facing direction against a surface; and use thereof. The sheet of the present invention, assuming a direction perpendicular to part of a surface of a target area including partially the sheet surface is set as a specified axis, satisfies: (1) The target area includes plural inclined back-reflecting crystal-domains crystal domains having colloid particles immobilized in resin and including crystal lattice planes capable of Bragg-back reflecting at least some of components in a visible wavelength range of incident light having greater than 0 incident angle with the specified axis; and (2) By defining an azimuth angle around the specified axis, the inclined back-reflecting crystal-domains are so oriented that intensity of reflected light caused by Bragg back reflection varies depending on the azimuth angle of the incident light.


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