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Continuous majorization in quantum phase space for Wigner-positive states and proposals for Wigner-negative states

Jan de Boer1, Giuseppe Di Giulio2, Esko Keski-Vakkuri3,4,5, and Erik Tonni6

Phys. Rev. A 112, 032405 – Published 2 September, 2025

DOI: https://doi.org/10.1103/w561-h3z5

Abstract

In quantum resource theory, one is often interested in identifying which states serve as the best resources for particular quantum tasks. If a relative comparison between quantum states can be made, this gives rise to a partial order, where states are ordered according to their suitability to act as a resource. In the literature, various different partial orders for a variety of quantum resources have been proposed. In discrete variable systems, vector majorization of Wigner functions in discrete phase space provides a natural partial order between quantum states. In the continuous variable case, a natural counterpart would be continuous majorization of Wigner functions in quantum phase space. Indeed, this concept was recently proposed and explored (mostly restricting to the single-mode case) by Van Herstraeten et al. [Quantum 7, 1021 (2023)]. In this work, we develop the theory of continuous majorization in the general N-mode case. In addition, we propose extensions to include states with finite Wigner negativity. For the special case of the convex hull of N-mode Gaussian states, we prove a conjecture made by Van Herstraeten, Jabbour, and Cerf. We also prove a phase space counterpart of Uhlmann's theorem of majorization.

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References (75)

  1. A. Serafini, Quantum Continuous Variables: A Primer of Theoretical Methods (CRC Press, Boca Raton, 2017).
  2. 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).
  3. G. Adesso, S. Ragy and A. R. Lee, Continuous variable quantum information: Gaussian states and beyond, Open Syst. Inf. Dyn. 21, 1440001 (2014).
  4. S. L. Braunstein and P. van Loock, Quantum information with continuous variables, Rev. Mod. Phys. 77, 513 (2005).
  5. S. Lloyd and S. L. Braunstein, Quantum computation over continuous variables, Phys. Rev. Lett. 82, 1784 (1999).
  6. N. C. Menicucci, P. van Loock, M. Gu, C. Weedbrook, T. C. Ralph and M. A. Nielsen, Universal quantum computation with continuous-variable cluster states, Phys. Rev. Lett. 97, 110501 (2006).
  7. E. Chitambar and G. Gour, Quantum resource theories, Rev. Mod. Phys. 91, 025001 (2019).
  8. M. B. Plenio and S. S. Virmani, An introduction to entanglement theory, Quant. Inf. Comput. 7, 001 (2007).
  9. M. A. Nielsen, Conditions for a class of entanglement transformations, Phys. Rev. Lett. 83, 436 (1999).
  10. V. Veitch, S. A. H. Mousavian, D. Gottesman and J. Emerson, The resource theory of stabilizer quantum computation, New J. Phys. 16, 013009 (2014).
  11. In quantum computing, an important resource is magic, aka nonstabilizerness, which is needed for an advantage over classical computing. For qubits, this result follows from the Gottesman-Knill theorem [72], which was later extended for qudits and continuous variable systems [40, 73, 74]. Both in the discrete variable (DV) case of qudits and in the CV case, quantum advantage requires computation involving states whose Wigner function takes negative values in some parts of the quantum phase space. Thus, the resource magic can also be called Wigner negativity, and indeed this is the convention for continuous variables.
  12. S. Bravyi, G. Smith and J. A. Smolin, Trading classical and quantum computational resources, Phys. Rev. X 6, 021043 (2016).
  13. M. Howard and E. Campbell, Application of a resource theory for magic states to fault-tolerant quantum computing, Phys. Rev. Lett. 118, 090501 (2017).
  14. X. Wang, M. M. Wilde and Y. Su, Quantifying the magic of quantum channels, New J. Phys. 21, 103002 (2019).
  15. J. R. Seddon and E. T. Campbell, Quantifying magic for multi-qubit operations, Proc. R. Soc. A 475, 20190251 (2019).
  16. L. Leone, S. F. Oliviero and A. Hamma, Stabilizer Rényi entropy, Phys. Rev. Lett. 128, 050402 (2022).
  17. R. J. Garcia, G. Bhole, K. Bu, L. Chen, H. Arthanari, and A. Jaffe, On the hardness of measuring magic, arXiv:2408.01663.
  18. N. Koukoulekidis and D. Jennings, Constraints on magic state protocols from the statistical mechanics of Wigner negativity, npj Quantum Inf. 8, 42 (2022).
  19. F. Albarelli, M. Genoni, M. Paris and A. Ferraro, Resource theory of quantum non-Gaussianity and Wigner negativity, Phys. Rev. A 98, 052350 (2018).
  20. R. Takagi and Q. Zhuang, Convex resource theory of non-Gaussianity, Phys. Rev. A 97, 062337 (2018).
  21. A. Kenfack and K. Życzkowski, Negativity of the Wigner function as an indicator of non-classicality, J. Opt. B 6, 396 (2004).
  22. G. H. Hardy, J. E. Littlewood and G. Pólya, Some simple inequalities satisfied by convex functions, Messenger Math. 58, 145 (1929).
  23. K.-M. Chong, Some extensions of a theorem of Hardy, Littlewood and Polya and their applications, Can. J. Math. 26, 1321 (1974).
  24. R. Hickey, Continuous majorisation and randomnes, J. Appl. Probab. 21, 924 (1984).
  25. H. Joe, Majorization, randomness and dependence for multivariate distributions, Ann. Probab. 26, 1217 (1987).
  26. Z. Van Herstraeten, M. G. Jabbour and N. J. Cerf, Continuous majorization in quantum phase space, Quantum 7, 1021 (2023).
  27. G. H. Hardy, J. E. Littlewood and G. Pólya, Inequalities (Cambridge University Press, Cambridge, 1988).
  28. A. W. Marshall, I. Olkin, and B. C. Arnold, Inequalities: Theory of Majorization and Its Applications, Springer Series in Statistics (Springer, New York, 2011).
  29. S. Manjegani and S. Moein, Majorization and semidoubly stochastic operators on L1(X), J. Inequal. Appl. 2023, 27 (2023).
  30. N. J. Cerf and T. Haas, Information and majorization theory for fermionic phase-space distributions, arXiv:2401.08523.
  31. Technical and conceptual difficulties will arise when we move to consider non-Wigner-positive states, with the Wigner function becoming negative in some domain. For that reason, Ref. [75] considered applying continuous majorization in quantum phase space through Husimi Q distributions, which are non-negative, and difficulties can be avoided. However, here we are motivated by the familiarity of Wigner functions, the connection between quantum advantage and Wigner negativity, and by the resource theories of non-Gaussianity and Wigner negativity. Hence, we focus on Wigner functions.
  32. Strictly speaking, even a non-negative Wigner function is not an ordinary probability distribution, since the random variables are eigenvalues of noncommuting operators [75] and therefore it could be more appropriately called a quasi-probability distribution. In this work to simplify the language, we use the word probability distribution for a non-negative Wigner function and quasi-probability distribution for nonpositive Wigner function.
  33. T. Bröcker and R. F. Werner, Mixed states with positive Wigner functions, J. Math. Phys. 36, 62 (1995).
  34. J. Williamson, On the algebraic problem concerning the normal forms of linear dynamical systems, Am. J. Math. 58, 141 (1936).
  35. Result 1 can be proven by plugging (25) into the left-hand side of (4) and performing the change of variables yj=rj/σj. We obtain. ∫e−12rtr(2π)N−tdetγ+dr≡I(tdetγ). (5.3) The fact that the function I(x) is monotonically decreasing in x and the condition (4) implies Result 1.
  36. J. E. Bourassa, N. Quesada, I. Tzitrin, A. Száva, T. Isacsson, J. Izaac, K. K. Sabapathy, G. Dauphinais and I. Dhand, Fast simulation of bosonic qubits via Gaussian functions in phase space, PRX Quantum 2, 040315 (2021).
  37. M. G. Jabbour, R. García-Patrón and N. J. Cerf, Interconversion of pure Gaussian states requiring non-Gaussian operations, Phys. Rev. A 91, 012316 (2015).
  38. G. Giedke and J. I. Cirac, Characterization of Gaussian operations and distillation of Gaussian states, Phys. Rev. A 66, 032316 (2002).
  39. M. Walschaers, Non-Gaussian quantum states and where to find them, PRX Quantum 2, 030204 (2021).
  40. A. Mari and J. Eisert, Positive Wigner functions render classical simulation of quantum computation efficient, Phys. Rev. Lett. 109, 230503 (2012).
  41. A. Arqand, L. Memarzadeh and S. Mancini, Quantum capacity of a bosonic dephasing channel, Phys. Rev. A 102, 042413 (2020).
  42. L. Lami and M. M. Wilde, Exact solution for the quantum and private capacities of bosonic dephasing channels, Nat. Photon. 17, 525 (2023).
  43. A. Uhlmann, Sätze über Dichtematrizen, Wiss. Z. Karl-Marx-Univ. Leipzig, Math.-Nat. R. 20, 633 (1971).
  44. A. Hertz, M. G. Jabbour and N. J. Cerf, Entropy-power uncertainty relations: Towards a tight inequality for all Gaussian pure states, J. Phys. A 50, 385301 (2017).
  45. G. Adesso, D. Girolami and A. Serafini, Measuring Gaussian quantum information and correlations using the Rényi entropy of order 2, Phys. Rev. Lett. 109, 190502 (2012).
  46. Z. Van Herstraeten and N. J. Cerf, Quantum Wigner entropy, Phys. Rev. A 104, 042211 (2021).
  47. L. Lami, C. Hirche, G. Adesso and A. Winter, From log-determinant inequalities to Gaussian entanglement via recoverability theory, IEEE Trans. Inf. Theory 63, 7553 (2017).
  48. L. Vanbever, In Wigner phase space, convolution explains why the vacuum majorizes mixtures of Fock states, arXiv:2104.14996.
  49. R. Arias, G. Di Giulio, E. Keski-Vakkuri and E. Tonni, Probing RG flows, symmetry resolution and quench dynamics through the capacity of entanglement, J. High Energy Phys. 03 (2023) 175.
  50. R. Orus, Entanglement and majorization in (1 + 1)-dimensional quantum systems [Phys. Rev. A 71, 052327 (2005)], Phys. Rev. A 73, 019904(E) (2006).
  51. A. S. Holevo and R. F. Werner, Evaluating capacities of bosonic Gaussian channels, Phys. Rev. A 63, 032312 (2001).
  52. V. Giovannetti, S. Lloyd, L. Maccone, J. H. Shapiro and B. J. Yen, Minimum Rényi and Wehrl entropies at the output of bosonic channels, Phys. Rev. A 70, 022328 (2004).
  53. A. Jamiołkowski, Linear transformations which preserve trace and positive semidefiniteness of operators, Rep. Math. Phys. 3, 275 (1972).
  54. M.-D. Choi, Completely positive linear maps on complex matrices, Linear Algebra Appl. 10, 285 (1975).
  55. J. Eisert and M. M. Wolf, Gaussian quantum channels, in Quantum Information with Continous Variables of Atoms and Light (Imperial College Press, London, 2007), pp. 23–42.
  56. R. Horn and C. Johnson, Matrix Analysis (Cambridge, 2013).
  57. We thank Ludovico Lami and an anonymous referee for pointing out this example.
  58. E. Lieb and Y. Ostrover, Localization of multidimensional Wigner distributions, J. Math. Phys. 51, 102101 (2010).
  59. W. P. Schleich, Quantum Optics in Phase Space (Wiley-VCH, Berlin, 2001).
  60. O. Fawzi, A. Oufkir, and R. Salzmann, Optimal fidelity estimation from binary measurements for discrete and continuous variable systems, arXiv:2409.04189.
  61. T. Heinosaari, A. S. Holevo and M. M. Wolf, The semigroup structure of Gaussian channels, Quantum Inf. Comput. 10, 0619 (2010).
  62. This channel is perfectly well-defined, as we can observe from the definition (31) of a Gaussian channel acting on a Gaussian state. We refer to it as degenerate given that detX=0. Consequently, the second integral in (34) is divergent. However, this does not affect the action of the channel on a generic input Wigner function. Indeed, as a consequence of X=0, the kernel (33) loses its dependence on z, and the second condition in (34) is not necessary.
  63. To avoid the choice of the branch, we could have defined the Wigner Rényi entropies (41) with an absolute value on the integrand. However, in this way, the Wigner function would have lost its normalization, and, therefore, the interpretation of the resulting quantity as a Rényi entropy would have been more difficult. We postpone the discussion of this potentially interesting new definition to future investigations.
  64. N. J. Cerf, A. Hertz and Z. Van Herstraeten, Complex-valued Wigner entropy of a quantum state, Quantum Stud.: Math. Found. 11, 331 (2024).
  65. To show this inequality, we first observe that [af(x)−t]+=a[f(x)−t/a]+. Given that the right-hand side is monotonically decreasing as a function of t/a, if a≥1, we have [af(x)−t]+≥a[f(x)−t]+, which is what we wanted to prove.
  66. L. van Luijk, A. Stottmeister, R. F. Werner, and H. Wilming, Pure state entanglement and von Neumann algebras, arXiv:2409.17739.
  67. R. Basu, A. Ganguly, S. Nath and O. Parrikar, Complexity growth and the Krylov-Wigner function, J. High Energy Phys. 05 (2024) 264.
  68. G. Di Giulio, Continuous majorization in quantum phase space for Wigner-positive states and proposals for Wigner-negative states [Data set], Zenodo (2025), https://doi.org/10.5281/zenodo.16877200.
  69. B. Demoen, P. Vanheuverzwijn, and A. Verbeure, Completely positive maps on the CCR-algebra, Lett. Math. Phys. 2, 161 (1977).
  70. B. Demoen, P. Vanheuverzwijn and A. Verbeure, Completely positive quasi-free maps of the CCR-algebra, Rep. Math. Phys. 15, 27 (1979).
  71. I. Bengtsson and K. Życzkowski, Geometry of Quantum States: An Introduction to Quantum Entanglement (Cambridge University Press, Cambridge, 2017).
  72. D. Gottesman, The Heisenberg representation of quantum computers, in Proceedings of the XXII International Colloquium on Group Theoretical Methods in Physics, edited by S. P. Corney, R. Delbourgo, and P. D. Jarvis (International Press, Cambridge, MA, 1999), pp. 32–43.
  73. V. Veitch, C. Ferrie, D. Gross and J. Emerson, Negative quasi-probability as a resource for quantum computation, New J. Phys. 14, 113011 (2012).
  74. V. Veitch, N. Wiebe, C. Ferrie and J. Emerson, Efficient simulation scheme for a class of quantum optics experiments with non-negative Wigner representation, New J. Phys. 15, 013037 (2013).
  75. M. Gärttner, T. Haas, and J. Noll, Detecting continuous-variable entanglement in phase space with the Q distribution, Phys. Rev. A 108, 042410 (2023).

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