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:
Dec. 03, 2019

Filed:

Dec. 28, 2017
Applicant:

Sensor Electronic Technology, Inc., Columbia, SC (US);

Inventors:

Maxim S. Shatalov, Columbia, SC (US);

Remigijua Gaska, Columbia, SC (US);

Jinwei Yang, Columbia, SC (US);

Michael Shur, Vienna, VA (US);

Alexander Dobrinsky, Silver Spring, MD (US);

Assignee:
Attorney:
Primary Examiner:
Int. Cl.
CPC ...
H01L 33/06 (2010.01); H01L 33/04 (2010.01); H01L 29/15 (2006.01); H01L 29/20 (2006.01); H01L 33/32 (2010.01); H01L 33/00 (2010.01); B82Y 10/00 (2011.01); H01L 29/201 (2006.01); H01S 5/20 (2006.01); H01S 5/32 (2006.01); H01S 5/34 (2006.01); H01S 5/343 (2006.01); H01L 29/207 (2006.01); B82Y 20/00 (2011.01);
U.S. Cl.
CPC ...
H01L 33/06 (2013.01); B82Y 10/00 (2013.01); H01L 29/155 (2013.01); H01L 29/2003 (2013.01); H01L 33/0075 (2013.01); H01L 33/04 (2013.01); H01L 33/32 (2013.01); B82Y 20/00 (2013.01); H01L 29/15 (2013.01); H01L 29/201 (2013.01); H01L 29/207 (2013.01); H01S 5/2009 (2013.01); H01S 5/3211 (2013.01); H01S 5/3216 (2013.01); H01S 5/3407 (2013.01); H01S 5/34333 (2013.01);
Abstract

A solution for designing and/or fabricating a structure including a quantum well and an adjacent barrier is provided. A target band discontinuity between the quantum well and the adjacent barrier is selected to coincide with an activation energy of a dopant for the quantum well and/or barrier. For example, a target valence band discontinuity can be selected such that a dopant energy level of a dopant in the adjacent barrier coincides with a valence energy band edge for the quantum well and/or a ground state energy for free carriers in a valence energy band for the quantum well. Additionally, a target doping level for the quantum well and/or adjacent barrier can be selected to facilitate a real space transfer of holes across the barrier. The quantum well and the adjacent barrier can be formed such that the actual band discontinuity and/or actual doping level(s) correspond to the relevant target(s).


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