Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Quantum correlations in three-beam symmetric Gaussian states accessed via photon-number-resolving detection and quantum universal invariants

Jan Peřina, Jr.1,*, Nazarii Sudak2, Artur Barasiński2,†, and Antonín Černoch3

  • 1Joint Laboratory of Optics of Palacký University and Institute of Physics of CAS, Faculty of Science, Palacký University, 17. listopadu 12, 771 46 Olomouc, Czech Republic
  • 2Institute of Theoretical Physics, University of Wroclaw, Plac Maxa Borna 9, 50-204 Wrocław, Poland
  • 3Joint Laboratory of Optics, Institute of Physics of CAS, 17. listopadu 50a, 779 00 Olomouc, Czech Republic

  • *Contact author: jan.perina.jr@upol.cz
  • †Contact author: artur.barasinski@uwr.edu.pl

Phys. Rev. Research 7, 043292 – Published 15 December, 2025

DOI: https://doi.org/10.1103/vd3h-4pts

Abstract

Quantum correlations of symmetric three-beam Gaussian states are analyzed using their quantum universal invariants. These invariants, one-, two-, and three-beam purities, are expressed in terms of the beams’ intensity moments up to sixth order. The three-beam symmetric Gaussian states with varying amounts of the noise are experimentally generated using entangled photon pairs from down-conversion, their invariants are determined, and their quantum correlations are quantified. The coexistence of bipartite and tripartite entanglement and genuine tripartite entanglement is observed in these states that resemble the noisy GHZ/W states.

View figure in article

Physics Subject Headings (PhySH)

Article Text

Supplemental Material

References (43)

  1. D. Stoler, Equivalence classes of minimum uncertainty packets, Phys. Rev. D 1, 3217 (1970).
  2. R. E. Slusher, L. W. Hollberg, B. Yurke, J. C. Mertz, and J. F. Valleys, Observation of squeezed states generated by four-wave mixing in an optical cavity, Phys. Rev. Lett. 55, 2409 (1985).
  3. V. V. Dodonov, Nonclassical states in quantum optics: A squeezed review of the first 75 years, J. Opt. B: Quantum Semiclass. Opt. 4, R1 (2002).
  4. F. Laudenbach, C. Pacher, C.-H. F. Fung, A. Poppe, M. Peev, B. Schrenk, M. Hentschel, and P. W. H. Hübel, Continuous-variable quantum key distribution with Gaussian modulation—The theory of practical implementations, Adv. Quantum Technol. 1, 1800011 (2018).
  5. A. Franzen, B. Hage, J. DiGuglielmo, J. Fiurášek, and R. Schnabel, Experimental demonstration of continuous variable purification of squeezed states, Phys. Rev. Lett. 97, 150505 (2006).
  6. S. Grebien, J. Göttsch, B. Hage, J. Fiurášek, and R. Schnabel, Multistep two-copy distillation of squeezed states via two-photon subtraction, Phys. Rev. Lett. 129, 273604 (2022).
  7. K. Fukui, A. Tomita, A. Okamoto, and K. Fujii, High-threshold fault-tolerant quantum computation with analog quantum error correction, Phys. Rev. X 8, 021054 (2018).
  8. N. C. Menicucci, Fault-tolerant measurement-based quantum computing with continuous-variable cluster states, Phys. Rev. Lett. 112, 120504 (2014).
  9. R. Schnabel, Squeezed states of light and their applications in laser interferometers, Phys. Rep. 684, 1 (2017).
  10. A. I. Lvovsky and M. G. Raymer, Continuous-variable optical quantum-state tomography, Rev. Mod. Phys. 81, 299 (2009).
  11. L. Mandel and E. Wolf, Optical Coherence and Quantum Optics (Cambridge University Press, Cambridge, 1995).
  12. N. Sudak, J. Peřina Jr., A. Barasiński, and A. Černoch, Efficient characterization of N-beam Gaussian fields through photon-number measurements: Quantum universal invariants, Phys. Rev. Res. 7, 023278 (2025).
  13. G. Adesso, A. Serafini, and F. Illuminati, Quantification and scaling of multipartite entanglement in continuous variable systems, Phys. Rev. Lett. 93, 220504 (2004).
  14. G. Adesso, A. Serafini, and F. Illuminati, Multipartite entanglement in three-mode Gaussian states of continuous-variable systems: Quantification, sharing structure, and decoherence, Phys. Rev. A 73, 032345 (2006).
  15. S. Pirandola, S. Mancini, D. Vitali, and P. Tombesi, Continuous-variable entanglement and quantum-state teleportation between optical and macroscopic vibrational modes through radiation pressure, Phys. Rev. A 68, 062317 (2003).
  16. H. Yonezawa, T. Aoki, and A. Furusawa, Demonstration of a quantum teleportation network for continuous variables, Nature (London) 431, 430 (2004).
  17. A. Ferraro and M. G. A. Paris, Multimode entanglement and telecloning in a noisy environment, Phys. Rev. A 72, 032312 (2005).
  18. A. Barasiński, J. Peřina, and A. Černoch, Quantification of quantum correlations in two-beam Gaussian states using photon-number measurements, Phys. Rev. Lett. 130, 043603 (2023).
  19. G. Adesso and F. Illuminati, Continuous variable tangle, monogamy inequality, and entanglement sharing in Gaussian states of continuous variable systems, New J. Phys. 8, 15 (2006).
  20. J. Peřina, Jr., A. Černoch, and J. Soubusta, Compound twin beams without the need of genuine photon-number-resolving detection, Phys. Rev. Appl. 16, 024061 (2021).
  21. G. Giedke, B. Kraus, M. Lewenstein, and J. I. Cirac, Separability properties of three-mode Gaussian states, Phys. Rev. A 64, 052303 (2001).
  22. In the literature, such tripartite CV Gaussian states are commonly referred to as three-mode Gaussian states. However, to account for the multimode structure of the experimental fields, we adopt the term three-beam symmetric Gaussian states to prevent any potential misunderstanding.
  23. H. P. Robertson, The uncertainty principle, Phys. Rev. 34, 163 (1929).
  24. E. Schrödinger, Zum Heisenbergschen Unschärfeprinzip, Ber. Kgl. Akad. Wiss. Berlin 24, 296 (1930).
  25. A. Serafini, Multimode uncertainty relations and separability of continuous variable states, Phys. Rev. Lett. 96, 110402 (2006).
  26. R. Simon, Peres-Horodecki separability criterion for continuous variable systems, Phys. Rev. Lett. 84, 2726 (2000).
  27. L.-M. Duan, G. Giedke, J. I. Cirac, and P. Zoller, Inseparability criterion for continuous variable systems, Phys. Rev. Lett. 84, 2722 (2000).
  28. A. Serafini, G. Adesso, and F. Illuminati, Unitarily localizable entanglement of Gaussian states, Phys. Rev. A 71, 032349 (2005).
  29. J. Peřina, Quantum Statistics of Lnear and Nonlinear Optical Phenomena (Kluwer, Dordrecht, 1991).
  30. G. Adesso, A. Serafini, and F. Illuminati, Determination of continuous variable entanglement by purity measurements, Phys. Rev. Lett. 92, 087901 (2004).
  31. G. Adesso, A. Serafini, and F. Illuminati, Optical state engineering, quantum communication, and robustness of entanglement promiscuity in three-mode Gaussian states, New J. Phys. 9, 60 (2007).
  32. X.-Y. Chen, Entanglement bounds of tripartite squeezed thermal states, Phys. Lett. A 335, 121 (2005).
  33. S. A. Hill and W. K. Wootters, Computable entanglement, Phys. Rev. Lett. 78, 5022 (1997).
  34. R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, Quantum entanglement, Rev. Mod. Phys. 81, 865 (2009).
  35. G. Adesso and F. Illuminati, Entanglement in continuous-variable systems: Recent advances and current perspectives, J. Phys. A 40, 7821 (2007).
  36. I. Kogias, A. R. Lee, S. Ragy, and G. Adesso, Quantification of Gaussian quantum steering, Phys. Rev. Lett. 114, 060403 (2015).
  37. For STBGSs, the Schur complement is given by Mσ=αγγα−γγα−1γγ .
  38. See Supplemental Material at http://link.aps.org/supplemental/10.1103/vd3h-4pts for the structure of the analyzed experimental multimode fields, experimental setup, reconstruction of experimental photocount histograms, multimode Gaussian model, and relation between multimode and single-mode intensity moments of three-beam Gaussian fields.
  39. A. P. Dempster, N. M. Laird, and D. B. Rubin, Maximum likelihood from incomplete data via the EM algorithm, J. R. Stat. Soc. B 39, 1 (1977).
  40. Y. Vardi and D. Lee, From image deblurring to optimal investments: Maximum likelihood solutions for positive linear inverse problems, J. R. Stat. Soc. B 55, 569 (1993).
  41. I. I. Arkhipov, J. Peřina, Jr., J. Peřina, and A. Miranowicz, Comparative study of nonclassicality, entanglement, and dimensionality of multimode noisy twin beams, Phys. Rev. A 91, 033837 (2015).
  42. V. Michálek, J. Peřina Jr., and O. Haderka, Experimental quantification of the entanglement of noisy twin beams, Phys. Rev. Appl. 14, 024003 (2020).
  43. J. Perina, Jr., N. Sudak, A. Barasinski, and A. Cernoch, Quantum correlations in three-beam symmetric Gaussian states accessed via photon-number-resolving detection and quantum universal invariants [Data set], ASEP repository (2025), https://doi.org/10.57680/asep.0619579.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation