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. 09, 2017

Filed:

Jan. 14, 2014
Applicant:

Samsung Electronics Co., Ltd., Suwon-si, Gyeonggi-do, KR;

Inventors:

Hyung Jun Kim, Suwon-si, KR;

Ji-Hoon Lee, Suwon-si, KR;

Myung Sup Jung, Seongnam-si, KR;

Won-Cheol Jung, Seoul, KR;

Assignee:
Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G02F 1/13363 (2006.01); F21V 9/14 (2006.01); G02B 5/30 (2006.01); H01L 51/52 (2006.01);
U.S. Cl.
CPC ...
G02F 1/13363 (2013.01); F21V 9/14 (2013.01); G02B 5/3016 (2013.01); G02B 5/3083 (2013.01); G02F 1/133634 (2013.01); H01L 51/5275 (2013.01); B32B 2457/202 (2013.01); G02F 2001/133633 (2013.01); G02F 2001/133637 (2013.01); G02F 2001/133638 (2013.01); G02F 2413/02 (2013.01); G02F 2413/05 (2013.01); G02F 2413/12 (2013.01);
Abstract

A retardation film including: a first optical anisotropic layer including a polymer material; and a second optical anisotropic layer including a liquid crystal material, in which the first optical anisotropic layer has refractive indices which satisfy the following inequation: nz1≧nx1>ny1, the second optical anisotropic layer has refractive indices which satisfy the following inequation: nx2>ny2≧nz2, a fast axis of the first optical anisotropic layer and a slow axis of the second optical anisotropic layer form a predetermined angle such that refractive indices of the retardation film satisfy the following inequation: 0<(nx0−nz0)/(nx0−ny0)<1, and in-plane retardation values (Re0) of the retardation film respectively at a wavelength of about 450 nanometers, 550 nanometers and 650 nanometers satisfy the following inequation: Re0 (450 nm)<Re0 (550 nm)<Re0 (650 nm).


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