Method and system for the generation of optical multipartite quantum states

US10175556B2 · US · B2

Patent metadata
FieldValue
Publication numberUS-10175556-B2
Application numberUS-201615560614-A
CountryUS
Kind codeB2
Filing dateApr 12, 2016
Priority dateApr 20, 2015
Publication dateJan 8, 2019
Grant dateJan 8, 2019

How to read this patent

A practical reading order for non-experts. Skip the full description unless you need deep technical detail.

  1. Title

    What the patent document calls the invention.

  2. Abstract

    A short plain-language summary of the technical disclosure.

  3. Assignees and inventors

    Who owns or filed the patent and who is credited as inventor.

  4. Key dates

    Filing, priority, publication, and grant dates set the timeline.

  5. First independent claim

    The legal scope of protection — read this for what is actually claimed.

  6. CPC / IPC classifications

    Technology tags used to group this patent with similar filings.

  7. Citations and related patents

    Prior art links and similar publications in this corpus.

Abstract

Official abstract text for this publication.

A method and a system method for generating optical multipartite quantum states, comprising generating optical fields by at least two different spontaneous four-wave mixing processes and overlapping the optical fields spontaneously generated from the different spontaneous four-wave mixing processes into a same resonator mode of a third-order nonlinear resonator. The system comprises a multi-colored laser source exiting a nonlinear third-order resonator at different resonance frequencies belonging to different mode families of the resonator.

First claim

Opening claim text (preview).

The invention claimed is: 1. A method for generating optical multipartite quantum states, comprising generating optical fields by at least two different spontaneous four-wave mixing processes and overlapping the optical fields spontaneously generated from the different spontaneous four-wave mixing processes into a same resonator mode of a third-order nonlinear resonator. 2. The method of claim 1 , comprising suppressing undesired stimulated processes using at least one of: i) spatial-mode dispersion and ii) polarization dispersion. 3. The method of claim 1 , comprising controlling at least one of: i) spatial-mode dispersion and ii) polarization dispersion so that each resonator mode family exhibits different resonant frequencies and a similar free-spectral range. 4. The method of claim 1 , comprising controlling at least one of: i) spatial-mode dispersion and ii) polarization dispersion so that each resonator mode family exhibits different resonant frequencies and a similar free-spectral range, and adjusting an offset between resonances of each mode family to prevent overlap between stimulated four-wave mixing emission and modes of the resonator. 5. The method of claim 1 , comprising controlling at least one of: i) spatial-mode dispersion and ii) polarization dispersion so that each resonator mode family exhibits different resonant frequencies and a similar free-spectral range, and adjusting an offset between resonances of each mode family to prevent overlap between stimulated four-wave mixing emission and modes of the resonator so that the offset is different from half the average free-spectral range of any possible couple of resonator modes families. 6. The method of claim 1 , comprising using one of: traveling-wave two-port ring resonators, traveling-wave multi-port ring resonators, traveling-wave two-port racetrack resonators, traveling-wave multi-port racetrack resonators, and standing wave Fabry-Perot cavities. 7. The method of claim 1 , comprising using a spontaneous four-wave mixing process and a non-degenerate spontaneous four-wave mixing process. 8. The method of claim 1 , comprising using two non-degenerate spontaneous four-wave mixing processes and three different mode families. 9. The method of claim 1 , wherein the generated optical fields are ones of: continuous-variable states and discrete-variable states. 10. The method of claim 1 , wherein the generated optical fields are ones of: squeezed vacuum, squeezed coherent state, squeezed amplitude-phase and energy-time correlations. 11. The method of claim 1 , wherein the generated optical fields are ones of: time-bin states generated from single-photon states and photon number states. 12. The method of claim 1 , comprising selecting a birefringent and/or a mode-dispersive resonator. 13. The method of claim 1 , comprising selecting a multi-colored laser source. 14. A system for generating optical multipartite quantum states, comprising: a multi-colored laser source; and a nonlinear third-order resonator; wherein said multi-colored laser source excites said resonator at different resonance frequencies belonging to different mode families of said resonator, optical states generated in one resonator mode being correlated with optical states generated in at least two other resonator modes. 15. The system of claim 14 , wherein said multi-colored laser source comprises one of: i) a mode-locked laser and ii) at least two phase-locked laser sources. 16. The system of claim 14 , wherein said nonlinear third-order resonator is a birefringent and/or a mode-dispersive resonator.

Assignees

Inventors

Classifications

  • spatial light modulator · CPC title

  • in an optical waveguide structure (G02F1/377, {G02F1/395} take precedence) · CPC title

  • Nanooptics, e.g. quantum optics or photonic crystals · CPC title

  • Subject matter not provided for in other groups of this subclass · CPC title

  • Non-linear optics · CPC title

Patent family

Related publications grouped by family.

External sources

Frequently asked questions

Answers are generated from the same data shown on this page.

What does patent US10175556B2 cover?
A method and a system method for generating optical multipartite quantum states, comprising generating optical fields by at least two different spontaneous four-wave mixing processes and overlapping the optical fields spontaneously generated from the different spontaneous four-wave mixing processes into a same resonator mode of a third-order nonlinear resonator. The system comprises a multi-col…
Who is the assignee on this patent?
Inst Nat Rech Scient, Institute National De La Recherche Scient
What technology area does this patent fall under?
Primary CPC classification G02F1/3536. Mapped technology areas include Physics.
When was this patent published?
Publication date Tue Jan 08 2019 00:00:00 GMT+0000 (Coordinated Universal Time) (B2). Legal status and post-grant events are not shown on this page.
What related patents are in patentsdb?
We list 1 related publication on this page (citations in our corpus or others sharing the same primary CPC).