IP Library › Granted Patent US 12,225,116
Granted Patent B1
US 12,225,116 · App. 18/073,240 · Granted Feb 11, 2025

Quantum key distribution network with centralized optical pulse generation

Inventors: Jing Wang (Broomfield, CO); Bernardo Huberman (Palo Alto, CA)
Assignee: Cable Television Laboratories, Inc.
H04L9/0852H04B10/70
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Quick Facts
Patent No.
US 12,225,116
App. No.
18/073,240
Granted
Feb 11, 2025
Kind
B1
Abstract

A method performed by a node of a quantum key distribution (QKD) network includes receiving, from a hub of the QKD network, a user-node pulse train of optical-pulse pairs, each of the optical-pulse pairs comprising a first pulse and a second pulse having an optical phase shift relative to the first pulse. The method further includes splitting the user-node pulse train into first and second pulse trains, calibrating an asymmetric Mach-Zehnder interferometer with the first pulse train, blocking the second pulse of each of the optical-pulse pairs of the second pulse train to generate a filtered pulse train, splitting the filtered pulse train into a timing pulse train and a pre-qubit pulse train, delaying the pre-qubit pulse train into a delayed pulse train, and encoding the delayed pulse train into a photonic-qubit pulse train and transmitting the photonic-qubit pulse train to the hub.

Claims (58)

1. A method performed by a node of a quantum key distribution network, comprising:

receiving, from a hub of the quantum key distribution network, a user-node pulse train of optical-pulse pairs, each of the optical-pulse pairs comprising a first pulse and second pulse that is temporally delayed relative to the first pulse, the second pulse having an optical phase shift relative to the first pulse;

splitting the user-node pulse train into first and second pulse trains;

calibrating an asymmetric Mach-Zehnder interferometer with the first pulse train such that an interferometer phase shift between first and second arms of the asymmetric Mach-Zehnder interferometer matches the optical phase shift;

blocking the second pulse of each of the optical-pulse pairs of the second pulse train to generate a filtered pulse train;

splitting the filtered pulse train into a timing pulse train and a pre-qubit pulse train;

detecting the timing pulse train to generate an electronic timing signal;

delaying the pre-qubit pulse train into a delayed pulse train;

encoding, based on the electronic timing signal and using the asymmetric Mach-Zehnder interferometer, the delayed pulse train into a photonic-qubit pulse train; and

transmitting the photonic-qubit pulse train to the hub.

2. The method of claim 1 , wherein said encoding includes one or both of time-bin encoding and phase encoding.

3. The method of claim 1 , wherein said blocking occurs synchronously with the electronic timing signal.

4. The method of claim 1 , wherein said delaying is based on a temporal delay transmitted to the node by the hub via a classical communication channel.

5. The method of claim 4 , wherein the temporal delay is no greater than one-half of a repetition period of the user-node pulse train.

6. The method of claim 1 , wherein said receiving includes receiving the user-node pulse train via a fiber optic channel.

7. A node for a quantum key distribution network, comprising:

an optical input operable to receive, from a hub of the quantum key distribution network, a user-node pulse train of optical-pulse pairs, each of the optical-pulse pairs comprising a first pulse and a second pulse that is temporally delayed relative to the first pulse, the second pulse having an optical phase shift relative to the first pulse;

a first beamsplitter configured to split the user-node pulse train into first and second pulse trains;

a modulator operable to block the second pulse of each of the optical-pulse pairs of the second pulse train to generate a filtered pulse train;

a second beamsplitter configured to split the filtered pulse train into an timing pulse train and a pre-qubit pulse train;

a photodetector operable to detect the timing pulse train to generate an electronic timing signal;

an optical delay operable to delay the pre-qubit pulse train into a delayed pulse train;

a qubit encoder including an asymmetric Mach-Zehnder interferometer, the qubit encoder being operable to encode, based on the electronic timing signal, the delayed pulse train into a photonic-qubit pulse train;

a phase calibrator operable to calibrate the asymmetric Mach-Zehnder interferometer with the first pulse train such that an interferometer phase shift between first and second arms of the asymmetric Mach-Zehnder interferometer matches the optical phase shift; and

an optical output operable to transmit the photonic-qubit pulse train to the hub.

8. The node of claim 7 , the qubit encoder being operable to perform one or both of time-bin and phase encoding.

9. The node of claim 7 , the modulator being operable to synchronously block the second pulse based on the electronic timing signal.

10. The node of claim 7 , the optical delay being an electronically tunable optical delay line.

11. The node of claim 10 , further comprising an electronic delay generator operable to control the electronically tunable optical delay line.

12. The node of claim 7 , each of the optical input and the optical output comprising a fiber-optic port.

13. A method performed by a hub of a quantum key distribution network, comprising:

transforming, with an asymmetric Mach-Zehnder interferometer, an optical pulse train into a double pulse train of optical-pulse pairs, each of the optical-pulse pairs comprising a first pulse and a second pulse that is temporally delayed relative to the first pulse, the second pulse having an optical phase shift relative to the first pulse;

splitting the double pulse train into a first-node pulse train and a second-node pulse train;

transmitting the first-node pulse train to a first node of the quantum key distribution network, the first node transforming the first-node pulse train into a first photonic-qubit pulse train;

transmitting the second-node pulse train to a second node of the quantum key distribution network, the second node transforming the second-node pulse train into a second photonic-qubit pulse train;

receiving the first photonic-qubit pulse train from the first node;

receiving the second photonic-qubit pulse train from the second node; and

performing a partial Bell-state measurement with a first photonic qubit of the first photonic-qubit pulse train and a second photonic qubit of the second photonic-qubit pulse train, the first and second photonic qubits being at least partially indistinguishable.

14. The method of claim 13 , further comprising publicly announcing a result of the partial Bell-state measurement.

15. The method of claim 13 , further comprising generating the optical pulse train.

16. The method of claim 15 , wherein said generating comprises modulating a laser.

17. The method of claim 13 , further comprising optically switching the first-node pulse train to a third node of the quantum key distribution network.

18. The method of claim 13 , wherein said transmitting the first-node pulse train includes transmitting the first-node pulse train to the first node via a fiber-optic channel.

19. The method of claim 13 , wherein said receiving the first photonic-qubit pulse train includes receiving the first photonic-qubit pulse train via a fiber-optic channel.

20. A hub for a quantum key distribution network, comprising:

an asymmetric Mach-Zehnder interferometer operable to transform an optical pulse train into a double pulse train of optical-pulse pairs, each of the optical-pulse pairs comprising a first pulse and a second pulse that is temporally delayed relative to the first pulse, the second pulse having an optical phase shift relative to the first pulse;

a beamsplitter configured to split the double pulse train into a first-node pulse train and a second-node pulse train;

a first optical output operable to transmit the first-node pulse train to a first node of the quantum key distribution network such that the first node transforms the first-node pulse train into a first photonic-qubit pulse train;

a second optical output operable to transmit the second-node pulse train to a second node of the quantum key distribution network such that the second node transforms the second-node pulse train into a second photonic-qubit pulse train;

a first optical input operable to receive the first photonic-qubit pulse train;

a second optical input operable to receive the second photonic-qubit pulse train; and

a Bell-state measurement module operable to perform a partial Bell-state measurement with a first photonic qubit of the first photonic-qubit pulse train and a second photonic qubit of the second photonic-qubit pulse train, the first and second photonic qubits being at least partially indistinguishable.

21. The hub of claim 20 , further comprising a laser system operable to generate the optical pulse train.

22. The hub of claim 21 , the laser system comprising a laser and a modulator operable to modulate an intensity of a continuous-wave laser beam outputted by the laser.

23. The hub of claim 21 , the laser system comprising a laser diode and a modulator circuit operable to modulate an electrical current that drives the laser diode.

24. The hub of claim 20 , further comprising a third optical output and an optical switch, the first-node pulse train being transmitted from the first optical output when the optical switch is in a first position, the first-node pulse train being transmitted from the third optical output when the optical switch is in a second position.

25. The hub of claim 20 , further comprising a signal-processing circuit operable to transmit a result of the partial Bell-state measurement via a classical communication channel.

26. The hub of claim 20 , each of the first and second optical inputs and the first and second optical outputs comprising a fiber-optic port.

Assignments (1)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded Dec 1, 2022
From: WANG, JING; HUBERMAN, BERNARDO
To: CABLE TELEVISION LABORATORIES, INC.
Reel/Frame 061945/0706 →
Continuity (3)
Continuation In Part 17951968 · Sep 23, 2022
Provisional Application 63284732 · Dec 1, 2021
Provisional Application 63247612 · Sep 23, 2021
References Cited (13)
US 7781754B2 · Loss · 2010 [cited by examiner]
US 9374376B2 · Hunt et al. · 2016 [cited by applicant]
US 10171238B2 · Howe · 2019 [cited by examiner]
US 11271661B2 · Yoshino · 2022 [cited by examiner]
US 11309970B2 · Woodward · 2022 [cited by examiner]
US 11496225B2 · Rahman · 2022 [cited by examiner]
US 11888978B1 · Wang · 2024 [cited by examiner]
US 20230393335A1 · Challener et al. · 2023 [cited by applicant]
Liu, Yang, et al., Experimental Measurement-Device-Independent Quantum Key Distribution, Physical Review Letters, PRL 111, 130502 (2013), Sep. 27, 2013. [cited by applicant]
Lo, Hoi-Kwong, et al., Measurement device independent quantum key distribution, May 28, 2012. [cited by applicant]
Tang, Yan-Lin, et al., Measurement-Device-Independent Quantum Key Distribution over 200 km, Physical Review Letters, PRL 113, 190501, Nov. 7, 2014. [cited by applicant]
Tang, Yan-Ling, et al., Measurement-Device-Independent Quantum Key Distribution over Untrustful Metropolitan Network, Physical Review X 6, 011024, Mar. 4, 2016. [cited by applicant]
Xu, Feihu, et al., Measurement-device-independent quantum cryptography, IEEE Jornal of Selected Topics in Quantum Electronics, Aug. 2014. [cited by applicant]