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:
Feb. 09, 2016

Filed:

Sep. 20, 2011
Applicants:

Mikko Möttönen, Helsinki, FI;

Jukka Pekola, Helsinki, FI;

Inventors:

Mikko Möttönen, Helsinki, FI;

Jukka Pekola, Helsinki, FI;

Assignee:
Attorney:
Primary Examiner:
Int. Cl.
CPC ...
G01J 1/44 (2006.01); B82Y 10/00 (2011.01); G01J 1/42 (2006.01); G06N 99/00 (2010.01); H01L 39/22 (2006.01); G01J 5/20 (2006.01); B82Y 15/00 (2011.01);
U.S. Cl.
CPC ...
G01J 1/44 (2013.01); B82Y 10/00 (2013.01); G01J 1/42 (2013.01); G06N 99/002 (2013.01); H01L 39/22 (2013.01); B82Y 15/00 (2013.01); G01J 5/20 (2013.01);
Abstract

The present invention introduces a detector that is able to detect single microwave photons propagating in a waveguide. The waveguide of the invention is lowered to a temperature where it becomes superconductive. Disposed between a middle wire and a ground plane of the waveguide is a very small piece of a desired normal metal, whereby so-called SN contacts are formed between these materials. A separate reflection measurement circuit is coupled to the normal metal piece. When the impedance of the waveguide is matched to the impedance of the normal metal piece as well as possible, a photon propagating in the waveguide is most likely absorbed in the normal metal. The absorption slightly raises the temperature of the piece, which further changes the impedance observed in a so-called SIN junction between the reflection measurement circuit and the piece. The changed amplitude and phase are detectable at the outlet obtained from a mixer of the reflection measurement circuit, whereby a single absorbed photon can be detected. In principle, the present method and device enable quantum calculation in view of future applications.


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