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.

Patent No.:

US 9128246 B1

PDF
Full Text
Expired
Date of Patent:
Sep. 08, 2015

Filed:

Oct. 17, 2012
Applicants:

Mohammad Hafezi, Washington, DC (US);

Peter Rabl, Innsbruck, AT;

Inventors:

Mohammad Hafezi, Washington, DC (US);

Peter Rabl, Innsbruck, AT;

Assignee:

University of Maryland, College Park, College Park, MD (US);

Attorneys:
Primary Examiner:
Int. Cl.
CPC ...
G02F 1/025 (2006.01); G02B 6/26 (2006.01); G02F 1/01 (2006.01); G02B 6/35 (2006.01);
U.S. Cl.
CPC ...
G02B 6/26 (2013.01); G02F 1/0126 (2013.01); G02F 1/0134 (2013.01); G02B 6/3546 (2013.01); G02F 2203/15 (2013.01);
Abstract

On-chip non-reciprocity can be achieved by employing micron-sized optomechanical (OM) devices that are fabricated on-chip and which can be integrated with other optical elements. Non-linear coupling between light and a mechanical mode inside a resonator can provide a non-reciprocal response of the OM system, which can be induced and fully controlled by an external driving electromagnetic field. By choosing different resonator and/or waveguide configurations and by tuning different system parameters, the same OM coupling mechanism can be used to provide isolation (e.g., as an optical diode), non-reciprocal phase shifting, and/or routing applications. Even in the presence of a finite intrinsic mode coupling inside the resonator, non-reciprocal effects remain large for a sufficiently strong OM coupling. The disclosed systems, methods, and devices can be applied on a single photon level, which may find use for various non-reciprocal applications in the classical optical as well as the quantum regime.


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