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:
Jan. 25, 2011

Filed:

Aug. 18, 2005
Applicants:

Gregory Belenky, Port Jefferson, NY (US);

John D. Bruno, Bowie, MD (US);

Mikhail V. Kisin, Centereach, NY (US);

Serge Luryi, Setauket, NY (US);

Leon Shterengas, Centereach, NY (US);

Sergey Suchalkin, Centereach, NY (US);

Richard L. Tober, Elkridge, MD (US);

Inventors:

Gregory Belenky, Port Jefferson, NY (US);

John D. Bruno, Bowie, MD (US);

Mikhail V. Kisin, Centereach, NY (US);

Serge Luryi, Setauket, NY (US);

Leon Shterengas, Centereach, NY (US);

Sergey Suchalkin, Centereach, NY (US);

Richard L. Tober, Elkridge, MD (US);

Attorneys:
Primary Examiner:
Assistant Examiner:
Int. Cl.
CPC ...
H01S 3/10 (2006.01); H01S 5/00 (2006.01);
U.S. Cl.
CPC ...
Abstract

A semiconductor light source comprises a substrate, lower and upper claddings, a waveguide region with imbedded active area, and electrical contacts to provide voltage necessary for the wavelength tuning. The active region includes single or several heterojunction periods sandwiched between charge accumulation layers. Each of the active region periods comprises higher and lower affinity semiconductor layers with type-II band alignment. The charge carrier accumulation in the charge accumulation layers results in electric field build-up and leads to the formation of generally triangular electron and hole potential wells in the higher and lower affinity layers. Nonequillibrium carriers can be created in the active region by means of electrical injection or optical pumping. The ground state energy in the triangular wells and the radiation wavelength can be tuned by changing the voltage drop across the active region.


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