IP Library › Granted Patent US 11,556,831
Granted Patent B2
US 11,556,831 · App. 16/768,667 · Granted Jan 17, 2023

Method and system for generation and control of high-dimensional multi-partite quantum states

Inventors: Michael Kues (Hannover, DE); Christian Reimer (Lübeck, DE); Stefania Sciara (Montreal, CA); Piotr Roztocki (Longueuil, CA); Luis Romero Cortes (Bellavista, ES); José Azaña (Montreal, CA); Yoann Jestin (Montreal, CA); Roberto Morandotti (Montreal, KY)
G06N10/00G02F1/365
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Quick Facts
Patent No.
US 11,556,831
App. No.
16/768,667
Granted
Jan 17, 2023
Kind
B2
Abstract

A method and a system for generating a hyper-entangled high-dimensional time-bin frequency-bin state, the method comprising generating a hyper-entangled state composed of a time-bin and frequency-bin encoded state, and individually modifying at least one of: i) the amplitude and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state. The system comprises a non-linear medium exited with multiple pulses in broad phase-matching conditions, a frequency mode separator and an amplitude/phase modulator, the frequency mode separator temporally and spatially separating frequency modes of the hyper-entangled state, the amplitude/phase modulator individually modifying at least one of: i) the amplitude (and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state.

Claims (20)

1. A method for generating a hyper-entangled high-dimensional time-bin frequency-bin state from a hyper-entangled state composed of a time-bin and frequency-bin encoded state, comprising generating a hyper-entangled state composed of a time-bin and frequency-bin encoded state using a non-linear medium exited with multiple pulses in broad phase-matching conditions, and individually modifying at least one of: i) the amplitude and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state, by temporally and spatially separating frequency modes of the hyper-entangled state and modifying the at least one of: i) the amplitude and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state.

2. The method of claim 1 , wherein said modifying at least one of: i) the amplitude and ii) the phase of different state components at frequency-bins and time-bins of the hyper-entangled state comprises frequency-to-time-to-frequency mapping; and at least one of: i) phase modulating and ii) amplitude modulating.

3. The method of claim 1 , wherein said modifying at least one of: i) the amplitude and ii) the phase of different state components at frequency-bins and time-bins of the hyper-entangled state comprises frequency-to-time-to-frequency mapping using one of: dispersive fibers, fiber-Bragg gratings and fiber-Bragg waveguides, and at least one of: i) phase modulating and ii) amplitude modulating.

4. The method of claim 1 , wherein said modifying at least one of: i) the amplitude and ii) the phase of different state components at frequency-bins and time-bins of the hyper-entangled state comprises temporally and spatially separating frequency modes of the hyper-entangled state, and at least one of individually i) phase modulating and ii) amplitude modulating the frequency modes.

5. The method of claim 1 , comprising exciting the non-linear medium with multiple laser pulses depending on a target time-bin dimensionality in broad phase-matching conditions.

6. The method of claim 1 , wherein the non-linear medium is a non-resonant non-linear medium, the method comprising exciting the non-resonant non-linear medium with multiple pulses in broad phase-matching conditions and segmenting output spectra into different frequency bins.

7. The method of claim 1 , wherein the non-linear medium is a -resonant non-linear medium, the method comprising exciting the resonant non-linear medium with multiple pulses in broad phase-matching conditions.

8. The method of claim 1 , comprising exciting a nonlinear microring resonator with multiple pulses in broad phase-matching conditions.

9. The method of claim 1 , wherein said modifying at least one of: i) the amplitude and ii) the phase comprises using a controlled quantum gate.

10. The method of claim 1 , comprising modifying the amplitude, thereby turning the hyper-entangled state into a Greenberger-Horne-Zeilinger state.

11. The method of claim 1 , comprising modifying the phase, thereby turning the hyper-entangled state into a cluster state.

12. A system for generating a hyper-entangled high-dimensional time-bin frequency-bin state from a hyper-entangled state composed of a time-bin and frequency-bin encoded state, comprising a non-linear medium exited with multiple pulses in broad phase-matching conditions, a frequency mode separator and an amplitude/phase modulator, said frequency mode separator temporally and spatially separating frequency modes of the hyper-entangled state, said amplitude/phase modulator individually modifying at least one of: i) the amplitude and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state.

13. The system of claim 12 , wherein said non-linear medium is one of: a resonant and a non-resonant medium.

14. The system of claim 12 , wherein said non-linear medium is a non-resonant medium, the system comprising filters for segmenting output spectra into different frequency bins.

15. The system of claim 12 , wherein said non-linear medium is a nonlinear microring resonator, the system comprising filters for segmenting output spectra into different frequency bins.

16. The system of claim 12 , wherein said non-linear medium is one of: fibers and waveguides.

17. The system of claim 12 , wherein said non-linear medium is a nonlinear microring resonator.

18. The system of claim 12 , wherein said frequency mode separator comprises one of: dispersive fibers, fiber-Bragg gratings and fiber-Bragg waveguides.

19. An amplitude and phase quantum gate, comprising a frequency mode separator and an amplitude/phase modulator, said frequency mode separator temporally and spatially separating frequency modes of an hyper-entangled state composed of a time-bin and frequency-bin encoded state, said amplitude/phase modulator individually modifying at least one of: i) the amplitude and ii) the phase of the state components at different frequency-bins and different time-bins of the hyper-entangled state.

20. The amplitude and phase quantum gate of claim 19 , wherein said frequency mode separator comprises one of: dispersive fibers, fiber-Bragg gratings and fiber-Bragg waveguides.

Assignments (8)
NUNC PRO TUNC ASSIGNMENT Recorded May 30, 2020
From: KUES, MICHAEL
To: THE UNIVERSITY COURT OF THE UNIVERSITY OF GLASGOW
Reel/Frame 052795/0034 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: AZAÑA, JOSÉ
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0122 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: ROMERO CORTÉS, LUIS
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0130 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: JESTIN, YOANN
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0137 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: REIMER, CHRISTIAN
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0143 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: ROZTOCKI, PIOTR
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0146 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: MORANDOTTI, ROBERTO
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0149 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 30, 2020
From: SCIARA, STEFANIA
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 052795/0152 →
Continuity (2)
Provisional Application 62591825 · Nov 29, 2017
Related Publication 20210174235A1 · Jun 10, 2021