IP Library Granted Patent US 9,929,311
Granted Patent B2
US 9,929,311 · App. 14/777,176 · Granted Mar 27, 2018

Semiconductor light emitting element and method for producing the same

Inventors: Yukio Kashima (Tokyo, JP); Eriko Matsuura (Tokyo, JP); Mitsunori Kokubo (Shizuoka, JP); Takaharu Tashiro (Shizuoka, JP); Takafumi Ookawa (Shizuoka, JP); Hideki Hirayama (Saitama, JP); Sung Won Youn (Ibaraki, JP); Hideki Takagi (Ibaraki, JP); Ryuichiro Kamimura (Shizuoka, JP); Yamato Osada (Shizuoka, JP); Satoshi Shimatani (Kanagawa, JP)
Assignees: MARUBUN CORPORATION; TOSHIBA KIKAI KABUSHIKI KAISHA; RIKEN; NATIONAL INSTITUTE OF ADVANCED INDUSTRIAL SCIENCE & TECHNOLOGY; ULVAC, INC.; TOKYO OHKA KOGYO CO., LTD.
H01L33/22G06F17/10G06F17/5009H01L33/44H01L33/502H01L33/24H01L2933/0083
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Quick Facts
Patent No.
US 9,929,311
App. No.
14/777,176
Granted
Mar 27, 2018
Kind
B2
Abstract

A semiconductor light emitting element with a design wavelength of λ, comprising a photonic crystal periodic structure having two structures with different refractive indices at each of one or more interfaces between layers that form the light emitting element. The period a and the radius R that are parameters of each of the one or more periodic structures and the design wavelength λ satisfy Bragg conditions. The ratio (R/a) between the period a and the radius R is a value determined so that a predetermined photonic band gap (PBG) for TE light becomes maximum for each periodic structure. The parameters of each periodic structure are determined so that light extraction efficiency of the entire semiconductor light emitting element with respect to light with the wavelength λ becomes maximum as a result of conducting a simulation analysis with a FDTD method using as variables the depth h of the periodic structure that is of greater than or equal to 0.5a and the period a and the radius R that are determined for each order m of the Bragg conditions.

Claims (3)

1. A semiconductor light emitting element with a design wavelength of λ, comprising:

a transmitted-type photonic crystal periodic structure including a plurality of pillar structures, each having a radius of R at a backside of a substrate, wherein the photonic crystal periodic structure is formed by two-types of structures, air having a refractive index n 2 , and the substrate having refractive index n 1 ,

wherein the photonic crystal periodic structure has two photonic band gaps, wherein the photonic band gaps are open for TM polarization component, and have an average refractive index n av of the two-types of structures, the average refractive index n av satisfies Bragg conditions mλ/n av =2a, wherein n av is calculated by the equation of n av =(n 2 2 +(n 1 2 −n 2 2 )(2π/√3)(R/a) 2 ) 1/2 , a is a period of the pillar structures, an order m of the Bragg conditions is 4, 0.31≤R/a≤0.36, and a depth of each of the pillar structures h≥0.5a.

Assignments (3)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 21, 2020
From: NATIONAL INSTITUTE OF ADVANCED INDUSTRIAL SCIENCE AND TECHNOLOGY
To: MARUBUN CORPORATION
Reel/Frame 054711/0356 →
CHANGE OF NAME Recorded Dec 21, 2020
From: TOSHIBA KIKAI KABUSHIKI KAISHA
To: SHIBAURA MACHINE CO., LTD.
Reel/Frame 054821/0344 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Sep 15, 2015
From: KASHIMA, YUKIO; MATSUURA, ERIKO; KOKUBO, MITSUNORI; TASHIRO, TAKAHARU; OOKAWA, TAKAFUMI; HIRAYAMA, HIDEKI; YOUN, SUNG WON; TAGAKI, HIDEKI; KAMIMURA, RYUICHIRO; OSADA, YAMATO; SHIMATANI, SATOSHI
To: MARUBUN CORPORATION; TOSHIBA KIKAI KABUSHIKI KAISHA; RIKEN; NATIONAL INSTITUTE OF ADVANCED INDUSTRIAL SCIENCE & TECHNOLOGY; ULVAC, INC.; TOKYO OHKA KOGYO CO., LTD.
Reel/Frame 036569/0921 →
Priority Claims (1)
JP 2013-148234 · Jul 17, 2013 · national
Continuity (1)
Related Publication 20160042102A1 · Feb 11, 2016