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Characterization of spatial Schmidt modes in high-gain SU(1,1) interferometers

D. Scharwald1,2,3,4,* and P. R. Sharapova3

  • 1Heinz Nixdorf Institute, Paderborn University, Fürstenallee 11, 33102 Paderborn, Germany
  • 2Department of Electrical Engineering and Information Technology, Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany
  • 3Department of Physics, Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany
  • 4Institute for Photonic Quantum Systems (PhoQS), Paderborn University, Warburger Straße 100, 33098 Paderborn, Germany

  • *Contact author: dennis.scharwald@uni-paderborn.de

Phys. Rev. Research 8, 033139 – Published 4 August, 2026

DOI: https://doi.org/10.1103/ph64-ts39

Abstract

Multimode quantum light has promising applications in many areas of physics, such as quantum communications and quantum computing. However, its multimode nature also makes it challenging to measure its properties. Recently [I. Barakat et al., Optica Quantum 3, 36 (2025)], a technique for the simultaneous measurement of squeezing of multiple broadband modes based on a phase-sensitive amplification approach was experimentally implemented using a setup that effectively corresponds to an SU(1,1) interferometer. Here, we aim to provide a complete theoretical analysis of the modal structure of (generally unbalanced) SU(1,1) interferometers and a detailed theoretical formal derivation of the framework for this technique. Utilizing the joint Schmidt decomposition of the transfer functions, we investigate the shape and phase profiles of the modes of the SU(1,1) interferometer and its components [parametric down-conversion (PDC) sections] for different parametric gain regimes. We discover a complicated interplay between the PDC modes and the modes of the entire interferometer, and analyze it by using their overlap coefficients as a similarity measure. Finally, we develop a rigorous processing method for the aforementioned multimode squeezing measurement technique and discuss necessary approximations to make this method experimentally feasible.

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References (66)

  1. F. S. Roux, Nonlinear interferometry in all spatiotemporal degrees of freedom, Phys. Rev. A 105, 043701 (2022).
  2. A. M. Pérez, K. Y. Spasibko, P. R. Sharapova, O. V. Tikhonova, G. Leuchs, and M. V. Chekhova, Giant narrowband twin-beam generation along the pump-energy propagation direction, Nat. Commun. 6, 7707 (2015).
  3. N. Quesada, G. Triginer, M. D. Vidrighin, and J. E. Sipe, Theory of high-gain twin-beam generation in waveguides: From Maxwell's equations to efficient simulation, Phys. Rev. A 102, 033519 (2020).
  4. J. Fuenzalida, E. Giese, and M. Gräfe, Nonlinear interferometry: A new approach for imaging and sensing, Adv. Quantum Technol. 7, 2300353 (2024).
  5. I. Barakat, M. Kalash, D. Scharwald, P. Sharapova, N. Lindlein, and M. Chekhova, Simultaneous measurement of multimode squeezing through multimode phase-sensitive amplification, Optica Quantum 3, 36 (2025).
  6. N. Fabre and S. Felicetti, Parameter estimation of time and frequency shifts with generalized Hong-Ou-Mandel interferometry, Phys. Rev. A 104, 022208 (2021).
  7. D. Scharwald, T. Meier, and P. R. Sharapova, Phase sensitivity of spatially broadband high-gain SU(1,1) interferometers, Phys. Rev. Res. 5, 043158 (2023).
  8. P. R. Sharapova, G. Frascella, M. Riabinin, A. M. Pérez, O. V. Tikhonova, S. Lemieux, R. W. Boyd, G. Leuchs, and M. V. Chekhova, Properties of bright squeezed vacuum at increasing brightness, Phys. Rev. Res. 2, 013371 (2020).
  9. P. Sharapova, A. M. Pérez, O. V. Tikhonova, and M. V. Chekhova, Schmidt modes in the angular spectrum of bright squeezed vacuum, Phys. Rev. A 91, 043816 (2015).
  10. C. Weedbrook, S. Pirandola, R. García-Patrón, N. J. Cerf, T. C. Ralph, J. H. Shapiro, and S. Lloyd, Gaussian quantum information, Rev. Mod. Phys. 84, 621 (2012).
  11. M. V. Larsen, X. Guo, C. R. Breum, J. S. Neergaard-Nielsen, and U. L. Andersen, Deterministic multi-mode gates on a scalable photonic quantum computing platform, Nat. Phys. 17, 1018 (2021).
  12. L. S. Madsen et al., Quantum computational advantage with a programmable photonic processor, Nature (London) 606, 75 (2022).
  13. S. Schaffrath, D. Derr, M. Gräfe, and E. Giese, Quantum imaging beyond the standard-quantum limit and phase distillation, New J. Phys. 26, 023018 (2024).
  14. F. Meylahn, B. Willke, and H. Vahlbruch, Squeezed states of light for future gravitational wave detectors at a wavelength of 1550 nm, Phys. Rev. Lett. 129, 121103 (2022).
  15. G. S. Atkinson, E. J. Allen, G. Ferranti, A. R. McMillan, and J. C. F. Matthews, Quantum enhanced precision estimation of transmission with bright squeezed light, Phys. Rev. Appl. 16, 044031 (2021).
  16. M. Hillery, Quantum cryptography with squeezed states, Phys. Rev. A 61, 022309 (2000).
  17. W. Asavanant et al., Generation of time-domain-multiplexed two-dimensional cluster state, Science 366, 373 (2019).
  18. C. Roh, G. Gwak, Y.-D. Yoon, and Y.-S. Ra, Generation of three-dimensional cluster entangled state, Nat. Photon. 19, 526 (2025).
  19. H.-S. Zhong et al., Phase-programmable Gaussian Boson sampling using stimulated squeezed light, Phys. Rev. Lett. 127, 180502 (2021).
  20. Q. Kang, Z. Zhao, T. Zhao, C. Liu, and L. Hu, Phase estimation via a number-conserving operation inside a SU(1,1) interferometer, Phys. Rev. A 110, 022432 (2024).
  21. M. Manceau, F. Khalili, and M. Chekhova, Improving the phase super-sensitivity of squeezing-assisted interferometers by squeeze factor unbalancing, New J. Phys. 19, 013014 (2017).
  22. B. Yurke, S. L. McCall, and J. R. Klauder, SU(2) and SU(1,1) interferometers, Phys. Rev. A 33, 4033 (1986).
  23. D. A. Kopylov, T. Meier, and P. R. Sharapova, Theory of multimode squeezed light generation in lossy media, Quantum 9, 1621 (2025).
  24. R. S. Bennink and R. W. Boyd, Improved measurement of multimode squeezed light via an eigenmode approach, Phys. Rev. A 66, 053815 (2002).
  25. W. Wasilewski, A. I. Lvovsky, K. Banaszek, and C. Radzewicz, Pulsed squeezed light: Simultaneous squeezing of multiple modes, Phys. Rev. A 73, 063819 (2006).
  26. C. Cui, C. N. Gagatsos, S. Guha, and L. Fan, High-purity pulsed squeezing generation with integrated photonics, Phys. Rev. Res. 3, 013199 (2021).
  27. E. Gouzien, L. Labonté, J. Etesse, A. Zavatta, S. Tanzilli, V. D’Auria, and G. Patera, Hidden and detectable squeezing from microresonators, Phys. Rev. Res. 5, 023178 (2023).
  28. F. Arzani, C. Fabre, and N. Treps, Versatile engineering of multimode squeezed states by optimizing the pump spectral profile in spontaneous parametric down-conversion, Phys. Rev. A 97, 033808 (2018).
  29. M. Houde and N. Quesada, Waveguided sources of consistent, single-temporal-mode squeezed light: The good, the bad, and the ugly, AVS Quantum Sci. 5, 011404 (2023).
  30. A. Patra, R. Gupta, S. Roy, T. Das, and A. Sen(De), Quantum dense coding network using multimode squeezed states of light, Phys. Rev. A 106, 052607 (2022).
  31. V. Roman-Rodriguez, D. Fainsin, G. L. Zanin, N. Treps, E. Diamanti, and V. Parigi, Multimode squeezed state for reconfigurable quantum networks at telecommunication wavelengths, Phys. Rev. Res. 6, 043113 (2024).
  32. L. V. Amitonova, T. B. H. Tentrup, I. M. Vellekoop, and P. W. H. Pinkse, Quantum key establishment via a multimode fiber, Opt. Express 28, 5965 (2020).
  33. Y. Eto, T. Tajima, Y. Zhang, and T. Hirano, Observation of squeezed light at 1.535µm using a pulsed homodyne detector, Opt. Lett. 32, 1698 (2007).
  34. C. Gerry and P. Knight, Introductory Quantum Optics (Cambridge University Press, Cambridge, 2004).
  35. M. Kalash and M. V. Chekhova, Wigner function tomography via optical parametric amplification, Optica 10, 1142 (2023).
  36. D. Scharwald, Theoretical investigations of spatially multimode high-gain SU(1,1) interferometers, Ph.D. thesis, Universität Paderborn, 2025, https://doi.org/10.17619/UNIPB/1-2491.
  37. A. Christ, B. Brecht, W. Mauerer, and C. Silberhorn, Theory of quantum frequency conversion and type-II parametric down-conversion in the high-gain regime, New J. Phys. 15, 053038 (2013).
  38. D. Scharwald, L. Gehse, and P. R. Sharapova, Schmidt modes carrying orbital angular momentum generated by cascaded systems pumped with Laguerre–Gaussian beams, APL Photon. 10, 016112 (2025).
  39. Numerically, the decomposition of β as written in Eq.  (2.3) corresponds to the Takagi/Autonne decomposition [40].
  40. M. Houde, W. McCutcheon, and N. Quesada, Matrix decompositions in quantum optics: Takagi/Autonne, Bloch–Messiah/Euler, Iwasawa, and Williamson, Can. J. Phys. 102, 497 (2024).
  41. M. Houde and N. Quesada, Perfect pulsed inline twin-beam squeezers, AVS Quantum Sci. 6, 021402 (2024).
  42. In this work, we use Fraktur letters g and h (and c) to designate the overlap coefficients that were dubbed g and h in Ref.  [5] in order to avoid confusion with the phase-matching function h appearing in Eqs.  (1.2a) and (1.2b).
  43. Even if both crystals have the same parametric gain, the qs- and qi-dependent phase term eiΔkair(qs,qi)δz in Eq.  (3.7b) still prevents this.
  44. This follows, for example, similarly to Eq.  (1.5) from Eqs. (D2a) and (D2b) of Ref.  [7] and can be verified by combining Eqs.  (1.5) and (4.3) and using the connections between the eigenvalues as written in Eq.  (1.4).
  45. M. O. Scully and M. S. Zubairy, Quantum Optics (Cambridge University Press, Cambridge, 1997).
  46. In this work, we use the notation Δ2 for the variance of an operator: Δ2X̂=X̂2X̂2.
  47. These can be obtained as follows: An expression of the form x+1 can be factorized as x1+1/x. For large x, the second square root can be expanded into its Taylor series (binomial series) for x>1, since 1/x<1. Thus, 1+1/x=1+1/(2x)+O(1/x2). Truncating the series after the second term leads to the binomial approximation 1+1/x1+1/(2x). Plugging this back into the original expression directly leads to the approximations as written in Eqs.  (4.16a) and (4.16b).
  48. M. A. Finger, N. Y. Joly, P. S. J. Russell, and M. V. Chekhova, Characterization and shaping of the time-frequency Schmidt mode spectrum of bright twin beams generated in gas-filled hollow-core photonic crystal fibers, Phys. Rev. A 95, 053814 (2017).
  49. M. Chekhova, I. Barakat, M. Kalash, D. Scharwald, P. Sharapova, and N. Lindlein, Supplementary document for “Simultaneous measurement of multimode squeezing through multimode phase-sensitive amplification”, Figshare, 2025, https://doi.org/10.6084/m9.figshare.28007657.v3.
  50. D. Scharwald and P. R. Sharapova, Characterization of spatial Schmidt modes in high-gain SU(1,1) interferometers, dataset, Zenodo, 2025, https://doi.org/10.5281/zenodo.15794760.
  51. G. Cariolaro and G. Pierobon, Reexamination of Bloch-Messiah reduction, Phys. Rev. A 93, 062115 (2016).
  52. G. Cariolaro and G. Pierobon, Bloch-Messiah reduction of Gaussian unitaries by Takagi factorization, Phys. Rev. A 94, 062109 (2016).
  53. L. Trefethen and D. Bau, Numerical Linear Algebra (Society for Industrial and Applied Mathematics, Philadelphia, PA, 1997).
  54. This may not be necessarily true numerically due to floating-point errors. However, these usually only become relevant for extremely large eigenvalues Λn1. As such, this issue can, in principle, be mitigated by appropriately rescaling β and η̃.
  55. Note that the notation used here is slightly different than in Refs.  [23, 51, 52]. When comparing with these works, note that H̃E and BF.
  56. Note that numerical implementations of the SVD may return either V0H and ṼH or V0 and Ṽ as the right-hand side unitary.
  57. Generally, the Takagi factorization of a symmetric matrix G is defined as G=DSDT [40, 51, 59], where D is unitary and S is the diagonal matrix containing the singular values. However, for a unitary matrix, all singular values are equal to 1, meaning D=In, and therefore the Takagi factorization takes the form as in Eq.  (1.4).
  58. As an example for the abovementioned issues that may arise, consider the 2×2 identity matrix I2=1001, which is a unitary, symmetric, and block-diagonal matrix consisting of two blocks of size 1. The matrix S=1i01 is one of the matrix square roots of I2: S2=I2. However, S is clearly neither symmetric nor unitary; see, for example, SHS=1ii2I2. Furthermore, S consists of a single block of size 2. Generally, a numerical algorithm may therefore not necessarily preserve the symmetry, unitarity, and/or the block-diagonal structure of the input matrix.
  59. A. M. Chebotarev and A. E. Teretenkov, Singular value decomposition for the Takagi factorization of symmetric matrices, Appl. Math. Comput. 234, 380 (2014).
  60. P. Virtanen et al., SciPy 1.0: Fundamental algorithms for scientific computing in Python, Nat. Methods 17, 261 (2020).
  61. In numerical applications, depending on the implementation, J may be replaced by J/dq, where dq is the step size of the q lattices. This corresponds to the replacement of the identity matrix by the Dirac delta distribution in the continuous case.
  62. E. Celledoni, E. Çokaj, A. Leone, D. Murari, and B. Owren, Lie group integrators for mechanical systems, Int. J. Comput. Math. 99, 58 (2022).
  63. A. Iserles, H. Z. Munthe-Kaas, S. P. Nørsett, and A. Zanna, Lie-group methods, Acta Numer. 9, 215 (2000).
  64. R. Demkowicz-Dobrzański, J. Kołodyński, and M. Guţă, The elusive Heisenberg limit in quantum-enhanced metrology, Nat. Commun. 3, 1063 (2012).
  65. E. Giese, S. Lemieux, M. Manceau, R. Fickler, and R. W. Boyd, Phase sensitivity of gain-unbalanced nonlinear interferometers, Phys. Rev. A 96, 053863 (2017).
  66. A. Christ, C. Lupo, M. Reichelt, T. Meier, and C. Silberhorn, Theory of filtered type-II parametric down-conversion in the continuous-variable domain: Quantifying the impacts of filtering, Phys. Rev. A 90, 023823 (2014).

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