Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity

Research output: Chapter in book/report/conference proceedingConference contributionResearchpeer review

Authors

  • Alí M. Angulo M
  • Jan Heine
  • J. S.S.Duran Gomez
  • Hatam Mahmudlu
  • Raktim Haldar
  • Charalambos Klitis
  • Marc Sorel
  • Michael Kues

External Research Organisations

  • University of Glasgow
  • Scuola Superiore Sant'Anna di Studi Universitari e di Perfezionamento
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Details

Original languageEnglish
Title of host publication2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference
Subtitle of host publication CLEO/Europe-EQEC
PublisherInstitute of Electrical and Electronics Engineers Inc.
Number of pages1
ISBN (electronic)9798350345995
ISBN (print)979-8-3503-4600-8
Publication statusPublished - 2023
Event2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2023 - Munich, Germany
Duration: 26 Jun 202330 Jun 2023

Abstract

The photon pair generation (PPG) via spontaneous four-wave mixing (SFWM) in an optically excited third-order nonlinear cavity forms large-scale high-dimensional quantum states, called quantum frequency combs (QFC). The scalable practical generation and control of these photonic states via integrated devices enable quantum information processing for applications in secured communications and quantum computing [1]. Modifying the excitation field properties in different degrees of freedom, e.g., polarization [2], frequency or spatial modes [3], allows controlling the structure of the generated quantum state by favoring different types of SFWM processes. In this work, by using two excitation fields and varying their intensity, P1 and P2, respectively, we demonstrate the occurrence of two different SFWM processes (degenerately and non-degenerately excited SFWM) and a control of the pair generation rate: µ(r, P) = µ1(P1(r, P)) + µ2(P2(r, P)) + µND(r, P), where P is the total excitation power, r = P1/P is the power ratio, µ1, µ2 describe the degenerate process and µND the non-degenerate process.

ASJC Scopus subject areas

Cite this

Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity. / Angulo M, Alí M.; Heine, Jan; Gomez, J. S.S.Duran et al.
2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference: CLEO/Europe-EQEC . Institute of Electrical and Electronics Engineers Inc., 2023.

Research output: Chapter in book/report/conference proceedingConference contributionResearchpeer review

Angulo M, AM, Heine, J, Gomez, JSSD, Mahmudlu, H, Haldar, R, Klitis, C, Sorel, M & Kues, M 2023, Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity. in 2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference: CLEO/Europe-EQEC . Institute of Electrical and Electronics Engineers Inc., 2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference, CLEO/Europe-EQEC 2023, Munich, Germany, 26 Jun 2023. https://doi.org/10.1109/CLEO/EUROPE-EQEC57999.2023.10232334
Angulo M, A. M., Heine, J., Gomez, J. S. S. D., Mahmudlu, H., Haldar, R., Klitis, C., Sorel, M., & Kues, M. (2023). Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity. In 2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference: CLEO/Europe-EQEC Institute of Electrical and Electronics Engineers Inc.. https://doi.org/10.1109/CLEO/EUROPE-EQEC57999.2023.10232334
Angulo M AM, Heine J, Gomez JSSD, Mahmudlu H, Haldar R, Klitis C et al. Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity. In 2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference: CLEO/Europe-EQEC . Institute of Electrical and Electronics Engineers Inc. 2023 doi: 10.1109/CLEO/EUROPE-EQEC57999.2023.10232334
Angulo M, Alí M. ; Heine, Jan ; Gomez, J. S.S.Duran et al. / Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity. 2023 Conference on Lasers and Electro-Optics Europe and European Quantum Electronics Conference: CLEO/Europe-EQEC . Institute of Electrical and Electronics Engineers Inc., 2023.
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title = "Tailoring photon pair emission characteristics via bi-chromatic excitation of an integrated nonlinear cavity",
abstract = "The photon pair generation (PPG) via spontaneous four-wave mixing (SFWM) in an optically excited third-order nonlinear cavity forms large-scale high-dimensional quantum states, called quantum frequency combs (QFC). The scalable practical generation and control of these photonic states via integrated devices enable quantum information processing for applications in secured communications and quantum computing [1]. Modifying the excitation field properties in different degrees of freedom, e.g., polarization [2], frequency or spatial modes [3], allows controlling the structure of the generated quantum state by favoring different types of SFWM processes. In this work, by using two excitation fields and varying their intensity, P1 and P2, respectively, we demonstrate the occurrence of two different SFWM processes (degenerately and non-degenerately excited SFWM) and a control of the pair generation rate: µ(r, P) = µ1(P1(r, P)) + µ2(P2(r, P)) + µND(r, P), where P is the total excitation power, r = P1/P is the power ratio, µ1, µ2 describe the degenerate process and µND the non-degenerate process.",
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AU - Angulo M, Alí M.

AU - Heine, Jan

AU - Gomez, J. S.S.Duran

AU - Mahmudlu, Hatam

AU - Haldar, Raktim

AU - Klitis, Charalambos

AU - Sorel, Marc

AU - Kues, Michael

N1 - Funding Information: This work received funding from the European Research Council (ERC) under grant agreement No. 947603 (QFreC project) from the German Federal Ministry of Education and Research, Quantum Futur Program (PQuMAL) and from the German Research Foundation (DFG) under Germany's Excellence Strategy within the Cluster of Excellence PhoenixD (EXC 2122, Project ID 390833453).

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N2 - The photon pair generation (PPG) via spontaneous four-wave mixing (SFWM) in an optically excited third-order nonlinear cavity forms large-scale high-dimensional quantum states, called quantum frequency combs (QFC). The scalable practical generation and control of these photonic states via integrated devices enable quantum information processing for applications in secured communications and quantum computing [1]. Modifying the excitation field properties in different degrees of freedom, e.g., polarization [2], frequency or spatial modes [3], allows controlling the structure of the generated quantum state by favoring different types of SFWM processes. In this work, by using two excitation fields and varying their intensity, P1 and P2, respectively, we demonstrate the occurrence of two different SFWM processes (degenerately and non-degenerately excited SFWM) and a control of the pair generation rate: µ(r, P) = µ1(P1(r, P)) + µ2(P2(r, P)) + µND(r, P), where P is the total excitation power, r = P1/P is the power ratio, µ1, µ2 describe the degenerate process and µND the non-degenerate process.

AB - The photon pair generation (PPG) via spontaneous four-wave mixing (SFWM) in an optically excited third-order nonlinear cavity forms large-scale high-dimensional quantum states, called quantum frequency combs (QFC). The scalable practical generation and control of these photonic states via integrated devices enable quantum information processing for applications in secured communications and quantum computing [1]. Modifying the excitation field properties in different degrees of freedom, e.g., polarization [2], frequency or spatial modes [3], allows controlling the structure of the generated quantum state by favoring different types of SFWM processes. In this work, by using two excitation fields and varying their intensity, P1 and P2, respectively, we demonstrate the occurrence of two different SFWM processes (degenerately and non-degenerately excited SFWM) and a control of the pair generation rate: µ(r, P) = µ1(P1(r, P)) + µ2(P2(r, P)) + µND(r, P), where P is the total excitation power, r = P1/P is the power ratio, µ1, µ2 describe the degenerate process and µND the non-degenerate process.

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