IP Library › Granted Patent US 12,283,998
Granted Patent B2
US 12,283,998 · App. 18/100,857 · Granted Apr 22, 2025

Method and apparatus for mapping out sources of decoherence in quantum channels

Inventors: Michael Brodsky (Millburn, NJ); Cristian Antonelli (Sulmona, IT); Daniel E. Jones (Nottingham, MD); Gabriele Riccardi (Rome, IT)
Assignee: The United States America as represented by the Secretary of the Army
H04B10/70H04B10/079
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Quick Facts
Patent No.
US 12,283,998
App. No.
18/100,857
Granted
Apr 22, 2025
Kind
B2
Abstract

Systems, apparatus and methods for defining an impairment profile along a polarization quantum channel such as in terms of modal loss and decoherence. The disclosed impairment profile or characterization methods may be used as part of a tool such as to inform a network operator of a weakest span of the communication channel, thus facilitating optimal signal routing decisions.

Claims (29)

1. A method of characterizing an optical channel, comprising:

generating, using an entangled photon source (EPS), pairs of entangled photons, wherein first entangled photons A of the generated pairs of entangled photons are coupled to a first optical channel and second entangled photons B of the generated pairs of entangled photons are coupled to a second optical channel, wherein the first channel comprises an optical channel to be characterized and the second channel comprises a local storage optical channel;

detecting, at each of the first and second channels, respective entangled photons, wherein each entangled photon A is expressed in the basis (h A , h A′ ) and each corresponding entangled photon B is expressed in the basis (h B , h B′ );

determining quantum coincidence data (QCD) of detected entangled photons A and B;

measuring quantum-correlation along (h A , h B′ ) and (h A′ , h B ) of the detected entangled photons using the determined QCD; and

responsive to (h A , h B′ ) being greater than (h A′ , h B ), characterizing the first channel as a modal loss first channel;

responsive to (h A , h B′ ) being less than (h A′ , h B ), characterizing the first channel as a decoherence first channel.

2. The method of claim 1 , further comprising:

responsive to the first channel comprising a modal loss first channel, configuring the second channel to include a filtering element configured to compensate for modal loss.

3. The method of claim 1 , wherein the method is performed at an optical node N within an optical network comprising a plurality of optical nodes, each optical node N transmitting optical information to at least one adjacent optical node N+1 using a respective N first channel.

4. The method of claim 1 , wherein the pairs of entangled photons represent photon polarization qubits.

5. The method of claim 1 , wherein the pairs of entangled photons represent orbital angular momentum qubits.

6. The method of claim 1 , wherein the method is performed at each of a plurality of nodes in an optical network to identify preferred transmission channels thereat.

7. The method of claim 6 , wherein a preferred channel at a node comprises modal loss first channel.

8. The method of claim 7 , wherein in the absence of a node having associated with it a modal loss first channel, a preferred channel comprises a decoherence first channel having associated with it a lowest amount of decoherence.

9. The method of claim 6 , further comprising establishing a connection between a source node SN and a destination node ND within the optical network by entangling photons from the source node, the destination node ND, and any nodes N between the source node SN and destination node ND.

10. The method of claim 9 , wherein each node N is configured for receiving an entangled photon A N−1 from a preceding node N−1, performing a Bell State measurement on a locally stored intermediate node photon B N and the received photon A N−1 to entangle thereby a transmitted intermediate node N photon A N and preceding node (N−1) photon B N−1 .

11. A method of characterizing an optical channel at an optical node N configured for use within a network comprising a plurality of optical nodes wherein each optical node is coupled to at least one other optical node via respective optical channels, the method comprising:

generating, using an entangled photon source (EPS), pairs of entangled photons, wherein first ones A of the generated pairs of entangled photons are coupled to a first optical channel and second ones B of the generated pairs of entangled photons are coupled to a second optical channel, wherein the first channel comprises an optical channel to be characterized;

detecting, at each of the first and second channels, respective entangled photons, wherein each photon A is expressed in the basis (h A , h A′ ) and each corresponding entangled photon B is expressed in the basis (h B , h B′ );

determining quantum coincidence data (QCD) of detected entangled photons A and B;

measuring quantum-correlation along (h A , h B′ ) and (h A′ , h B ) of the detected entangled photons using the determined QCD; and

responsive to (h A , h B′ ) being greater than (h A′ , h B ), characterizing the first channel as a modal loss first channel;

responsive to (h A , h B′ ) being less than (h A′ , h B ), characterizing the first channel as a decoherence first channel; and

selecting a modal loss first optical channel as a transmission channel.

12. The method of an optical node of claim 11 , further comprising configuring the second channel to include a filtering element configured to compensate for modal loss.

13. The method of an optical node of claim 11 , wherein in the absence of the node having associated with it a modal loss first channel, selecting as a transmission channel a decoherence first channel having associated with it a lowest amount of decoherence.

14. The method of an optical node of claim 11 , wherein the optical node is configured to receive an optical communication from an input optical channel and transmit the received optical communication to the selected one of a plurality of output optical channels.

15. The method of an optical node of claim 11 , wherein the optical node is configured for receiving an entangled photon A N−1 from a preceding node N−1, performing a Bell State measurement on a locally stored intermediate node photon B N and the received photon A N−1 to entangle thereby a transmitted intermediate node N photon A N and preceding node (N−1) photon B N−1 .

Assignments (4)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 2, 2023
From: UNIVERSITY L'AQUILLA
To: THE UNITED STATES OF AMERICA AS REPRESENTED BY THE SECRETARY OF THE ARMY
Reel/Frame 062575/0968 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 2, 2023
From: ANTONELLI, CRISTIAN
To: UNIVERSITY L'AQUILLA
Reel/Frame 062576/0175 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 2, 2023
From: RICCARDI, GABRIELE
To: UNIVERSITY L'AQUILLA
Reel/Frame 062576/0295 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Feb 1, 2023
From: BRODSKY, MICHAEL; JONES, DANIEL E.
To: THE UNITED STATES OF AMERICA AS REPRESENTED BY THE SECRETARY OF THE ARMY
Reel/Frame 062560/0625 →
Continuity (2)
Provisional Application 63302373 · Jan 24, 2022
Related Publication 20230261762A1 · Aug 17, 2023
References Cited (13)
US 10693565B2 · Kirby et al. · 2020 [cited by applicant]
US 11193750B1 · Fertig · 2021 [cited by examiner]
US 20160164615A1 · Dailey · 2016 [cited by examiner]
US 20190349094A1 · Santra · 2019 [cited by examiner]
US 20200274703A1 · Lukens · 2020 [cited by examiner]
CN 215575770U · 2022 [cited by examiner]
EP 3917074A1 · 2021 [cited by examiner]
JP 2020028076A · 2020 [cited by examiner]
WO WO2021067631A1 · 2021 [cited by examiner]
WO WO2024173939A1 · 2024 [cited by examiner]
Jones et al; Exploring classical correlations in noise to recover quantum information using local filtering; Jul. 2020; pp. 1-14. (Year: 2020). [cited by examiner]
D. E. Jones, B. T. Kirby, G. Riccardi, C. Antonelli, M. Brodsky, “Exploring classical correlation in noise to recover quantum information using local filtering,” New Journal of Physics, 22, 073037, Jul. 2020. [cited by applicant]
Gabriele Riccardi, Cristian Antonelli, Daniel E. Jones, and Michael Brodsky, “Simultaneous Decoherence and Mode Filtering in Quantum Channels: Theory and Experiment,” Physical Review Applied, 15, 014060 (2021). [cited by applicant]