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Optimal Fidelity Estimation from Binary Measurements for Discrete and Continuous Variable Systems

Omar Fawzi1, Aadil Oufkir2, and Robert Salzmann1,*

  • *Contact author: robert.als.salzmann@gmail.com

PRX Quantum 7, 010309 – Published 15 January, 2026

DOI: https://doi.org/10.1103/qd1c-1fk9

Abstract

Estimating the fidelity between a desired target quantum state and an actual prepared state is essential for assessing the success of experiments. For pure target states, we use functional representations that can be measured directly and determine the number of copies of the prepared state needed for fidelity estimation. In continuous variable (CV) systems, we use the Wigner function, which can be measured via displaced parity measurements. We provide upper and lower bounds on the sample complexity required for fidelity estimation, considering the worst-case scenario across all possible prepared states. For target states of particular interest, such as Fock and Gaussian states, we find that this sample complexity is characterized by the L1-norm of the Wigner function, a measure of Wigner negativity widely studied in the literature, in particular in resource theories of quantum computation. For discrete variable systems consisting of n qubits, we explore fidelity estimation protocols using Pauli string measurements. Similarly as for the CV approach, the sample complexity is shown to be characterized by the L1-norm of the characteristic function of the target state for both Haar random states and stabilizer states. Furthermore, in a general black box model, we prove that, for any target state, the optimal sample complexity for fidelity estimation is characterized by the smoothed L1-norm of the target state. To the best of our knowledge, this is the first time the L1-norm of the Wigner function provides a lower bound on the cost of some information processing task.

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References (81)

  1. M. P. da Silva, O. Landon-Cardinal, and D. Poulin, Practical characterization of quantum devices without tomography, Phys. Rev. Lett. 107, 210404 (2011).
  2. S. T. Flammia and Y.-K. Liu, Direct fidelity estimation from few Pauli measurements, Phys. Rev. Lett. 106, 230501 (2011).
  3. Antoine Royer, Wigner function as the expectation value of a parity operator, Phys. Rev. A 15, 449 (1977).
  4. L. G. Lutterbach and L. Davidovich, Method for direct measurement of the Wigner function in cavity QED and ion traps, Phys. Rev. Lett. 78, 2547 (1997).
  5. G. Nogues, A. Rauschenbeutel, S. Osnaghi, P. Bertet, M. Brune, J. M. Raimond, S. Haroche, L. G. Lutterbach, and L. Davidovich, Measurement of a negative value for the Wigner function of radiation, Phys. Rev. A 62, 054101 (2000).
  6. P. Bertet, A. Auffeves, P. Maioli, S. Osnaghi, T. Meunier, M. Brune, J. M. Raimond, and S. Haroche, Direct measurement of the Wigner function of a one-photon Fock state in a cavity, Phys. Rev. Lett. 89, 200402 (2002).
  7. Brian Vlastakis, Gerhard Kirchmair, Zaki Leghtas, Simon E. Nigg, Luigi Frunzio, S. M. Girvin, Mazyar Mirrahimi, M. H. Devoret, and R. J. Schoelkopf, Deterministically encoding quantum information using 100-photon Schrödinger cat states, Science 342, 607 (2013).
  8. Antoine Marquet, Simon Dupouy, Ulysse Réglade, Antoine Essig, Joachim Cohen, Emanuele Abertinale, Audrey Bienfait, Théau Peronnin, Sébastien Jezouin, Raphaël Lescanne, and Benjamin Huard, Harnessing two-photon dissipation for enhanced quantum measurement and control, Phys. Rev. Applied 22, 034053 (2024).
  9. A. Marquet, A. Essig, J. Cohen, N. Cottet, A. Murani, E. Albertinale, S. Dupouy, A. Bienfait, T. Peronnin, S. Jezouin, R. Lescanne, and B. Huard, Autoparametric resonance extending the bit-flip time of a cat qubit up to 0.3 s, Phys. Rev. X 14, 021019 (2024).
  10. Harald Putterman, Kyungjoo Noh, Connor T. Hann, Gregory S. MacCabe, Shahriar Aghaeimeibodi, Rishi N. Patel, Menyoung Lee, William M. Jones, Hesam Moradinejad, Roberto Rodriguez, et al., Hardware-efficient quantum error correction using concatenated bosonic qubits, Nature 638, 927–934 (2025).
  11. U. Réglade, A. Bocquet, R. Gautier, J. Cohen, A. Marquet, E. Albertinale, N. Pankratova, M. Hallén, F. Rautschke, L.-A. Sellem, P. Rouchon, A. Sarlette, M. Mirrahimi, P. Campagne-Ibarcq, R. Lescanne, S. Jezouin, and Z. Leghtas, Quantum control of a cat qubit with bit-flip times exceeding ten seconds, Nature 629, 778 (2024).
  12. Chen Wang, Yvonne Y. Gao, Philip Reinhold, R. W. Heeres, Nissim Ofek, Kevin Chou, Christopher Axline, Matthew Reagor, Jacob Blumoff, K. M. Sliwa, L. Frunzio, S. M. Girvin, Liang Jiang, M. Mirrahimi, M. H. Devoret, and R. J. Schoelkopf, A Schrödinger cat living in two boxes, Science 352, 1087 (2016).
  13. More precisely, we choose in Sec. 5 the set ΩP=Pn∖{1} instead of Pn as on the identity string the characteristic function of any state σ trivially satisfies χσ(1)=1 and hence no information is gained when we measure the observable 1 in σ.
  14. Gregory Valiant and Paul Valiant, An automatic inequality prover and instance optimal identity testing, SIAM J. Comput. 46, 429 (2017).
  15. Sitan Chen, Jerry Li, and Ryan O’Donnell, Toward instance-optimal state certification with incoherent measurements, in Conference on Learning Theory (PMLR, London, 2022), p. 2541.
  16. Clemens Markett, Mean Cesàro summability of Laguerre expansions and norm estimates with shifted parameter, Anal. Math. 8, 19 (1982).
  17. Francesco Albarelli, Marco G. Genoni, Matteo G. A. Paris, and Alessandro Ferraro, Resource theory of quantum non-Gaussianity and Wigner negativity, Phys. Rev. A 98, 052350 (2018).
  18. Anatole Kenfack and Karol Życzkowski, Negativity of the Wigner function as an indicator of non-classicality, J. Opt. B: Quantum Semiclassical Opt. 6, 396 (2004).
  19. K. C. Tan, S. Choi, and H. Jeong, Negativity of quasiprobability distributions as a measure of nonclassicality, Phys. Rev. Lett. 124, 110404 (2020).
  20. R. I. Booth, U. Chabaud, and P.-E. Emeriau, Contextuality and Wigner negativity are equivalent for continuous-variable quantum measurements, Phys. Rev. Lett. 129, 230401 (2022).
  21. S. D. Bartlett, B. C. Sanders, S. L. Braunstein, and K. Nemoto, Efficient classical simulation of continuous variable quantum information processes, Phys. Rev. Lett. 88, 097904 (2002).
  22. A. Mari and J. Eisert, Positive Wigner functions render classical simulation of quantum computation efficient, Phys. Rev. Lett. 109, 230503 (2012).
  23. Victor Veitch, Nathan Wiebe, Christopher Ferrie, and Joseph Emerson, Efficient simulation scheme for a class of quantum optics experiments with non-negative Wigner representation, New J. Phys. 15, 013037 (2013).
  24. Oliver Hahn, Giulia Ferrini, and Ryuji Takagi, Bridging magic and non-Gaussian resources via Gottesman-Kitaev-Preskill encoding, PRX Quantum 6, 010330 (2025).
  25. H. Pashayan, J. J. Wallman, and S. D. Bartlett, Estimating outcome probabilities of quantum circuits using quasiprobabilities, Phys. Rev. Lett. 115, 070501 (2015).
  26. C. Calcluth, A. Ferraro, and G. Ferrini, Vacuum provides quantum advantage to otherwise simulatable architectures, Phys. Rev. A 107, 062414 (2023).
  27. L. García-Álvarez, C. Calcluth, A. Ferraro, and G. Ferrini, Efficient simulatability of continuous-variable circuits with large Wigner negativity, Phys. Rev. Res. 2, 043322 (2020).
  28. E. T. Campbell, Catalysis and activation of magic states in fault-tolerant architectures, Phys. Rev. A—At., Mol. Opt. Phys. 83, 032317 (2011).
  29. O. Hahn, A. Ferraro, L. Hultquist, G. Ferrini, and L. García-Álvarez, Quantifying qubit magic resource with Gottesman-Kitaev-Preskill encoding, Phys. Rev. Lett. 128, 210502 (2022).
  30. In the main text of Ref. [2] the authors claim to have proven supρ pureNε,δP(ρ)=O((1/ε2δ)+d/ε2ln(1/δ)). However, considering their proof in the appendix (in particular the “Truncating bad events” section), the error parameter β introduced there needs to scale as ε in order to estimate the fidelity with the desired accuracy leading to a 1/ε4 scaling of their actual upper bound.
  31. L. Leone, S. F. E. Oliviero, and A. Hamma, Nonstabilizerness determining the hardness of direct fidelity estimation, Phys. Rev. A 107, 022429 (2023).
  32. Naixu Guo, Feng Pan, and Patrick Rebentrost, Estimating properties of a quantum state by importance-sampled operator shadows, ArXiv:quant-ph/2305.09374.
  33. V. V. Sivak, A. Eickbusch, H. Liu, B. Royer, I. Tsioutsios, and M. H. Devoret, Model-free quantum control with reinforcement learning, Phys. Rev. X 12, 011059 (2022).
  34. Ulysse Chabaud, Roohollah Ghobadi, Salman Beigi, and Saleh Rahimi-Keshari, Phase-space negativity as a computational resource for quantum kernel methods, Quantum 8, 1519 (2024).
  35. Barry Simon, The Weyl transform and Lp functions on phase space, Proc. Am. Math. Soc. 116, 1045 (1992).
  36. Jayadev Acharya, Abhilash Dharmavarapu, Yuhan Liu, and Nengkun Yu, Pauli Measurements Are Not Optimal for Single-Copy Tomography, in Proceedings of the 57th Annual ACM Symposium on Theory of Computing (Association for Computing Machinery, New York, NY, USA, 2025), pp. 718–729.
  37. Hsin-Yuan Huang, John Preskill, and Mehdi Soleimanifar, Certifying almost all quantum states with few single-qubit measurements, Nat. Phys. (2025).
  38. Ulysse Chabaud, Tom Douce, Frédéric Grosshans, Elham Kashefi, and Damian Markham, in 15th Conference on the Theory of Quantum Computation, Communication and Cryptography (TQC 2020), Leibniz International Proceedings in Informatics (LIPIcs), edited by Steven T. Flammia (Schloss Dagstuhl—Leibniz-Zentrum für Informatik, Dagstuhl, Germany, 2020), Vol. 158, p. 3:1.
  39. Ulysse Chabaud, Frédéric Grosshans, Elham Kashefi, and Damian Markham, Efficient verification of boson sampling, Quantum 5, 578 (2021).
  40. Varun Upreti and Ulysse Chabaud, An efficient quantum state verification framework and its application to bosonic systems, ArXiv:quant-ph/2411.04688.
  41. Heterodyne measurements are done by performing the POVM ((1/πm)|α⟩⟨α|)α∈Cm defined through the coherent states.
  42. A. I. Lvovsky and M. G. Raymer, Continuous-variable optical quantum-state tomography, Rev. Mod. Phys. 81, 299 (2009).
  43. Homodyne detection is done by measuring the observable Xθ=cos(θ)X+sin(θ)P, where X and P are the standard position and momentum operators and θ is an angle, which can be freely chosen and can be seen as rotating phase space.
  44. Photon-number-resolving measurements are done by performing the measurement corresponding to the positive operator valued measure (POVM) ((1/πm)D(α)|n⟩⟨n|D(α)∗)α∈Cm for different photon numbers n∈N.
  45. Simon Becker, Nilanjana Datta, Ludovico Lami, and Cambyse Rouze, Classical shadow tomography for continuous variables quantum systems, IEEE Trans. Inf. Theory 70, 3427 (2024).
  46. Srilekha Gandhari, Victor V. Albert, Thomas Gerrits, Jacob M. Taylor, and Michael J. Gullans, Precision bounds on continuous-variable state tomography using classical shadows, ArXiv:quant-ph/2211.05149.
  47. As an exemption Refs. [39, 40] do provide a finite sample complexity but only under the restrictive assumption that the target state is a finite superposition of Fock states.
  48. Atharv Joshi, Kyungjoo Noh, and Yvonne Y. Gao, Quantum information processing with bosonic qubits in circuit QED, Quantum Sci. Technol. 6, 033001 (2021).
  49. Nissim Ofek, Andrei Petrenko, Reinier Heeres, Philip Reinhold, Zaki Leghtas, Brian Vlastakis, Yehan Liu, Luigi Frunzio, S. M. Girvin, L. Jiang, Mazyar Mirrahimi, M. H. Devoret, and R. J. Schoelkopf, Extending the lifetime of a quantum bit with error correction in superconducting circuits, Nature 53, 441 (2016).
  50. V. V. Sivak, A. Eickbusch, B. Royer, S. Singh, I. Tsioutsios, S. Ganjam, A. Miano, B. L. Brock, A. Z. Ding, L. Frunzio, S. M. Girvin, R. J. Schoelkopf, and M. H. Devoret, Real-time quantum error correction beyond break-even, Nature 616, 50 (2023).
  51. Francesco Anna Mele, Antonio Anna Mele, Lennart Bittel, Jens Eisert, Vittorio Giovannetti, Ludovico Lami, Lorenzo Leone, and Salvatore F. E. Oliviero, Learning quantum states of continuous variable systems, ArXiv:quant-ph/2405.01431.
  52. This can for example be seen by considering the displaced state ρα=D(α)ρD(α)∗ which satisfies ‖Wρα‖1=‖Wρ‖1 for all α∈Cm but Tr(Nρα)→|α|→∞∞.
  53. Note that the smoothed L1-norm is not a norm itself as it does not satisfy the triangle inequality or faithfulness due to the infimum used.
  54. Density can be seen by defining for c>0 the function f~c=f1{|f|≥c} and noting that by the dominated convergence theorem it approximates f in the L2-norm as limc→0∫Ω|f~c(λ)−f(λ)|2dμ(λ)=limc→0∫{|f|<c}|f(λ)|2dμ(λ)=0. Furthermore, note that for all c>0 we have f~c∈L1(Ω,R) as ∫{|f|≥c}|f(λ)|dμ(λ)≤‖f‖22/c.
  55. Ola Bratteli and Derek W. Robinson, Operator Algebras and Quantum Statistical Mechanics II (Springer, Berlin, Heidelberg, 1997).
  56. Gerald Teschl, Mathematical Methods in Quantum Mechanics: With Applications to Schrödinger Operators, 2nd ed.Graduate Studies in Mathematics (157, American Mathematical Society, 2014), Vol.
  57. R. Werner, Quantum harmonic analysis on phase space, J. Math. Phys. 25, 1404 (1984).
  58. The integral expression (24) is well-defined for χρ being a Schwartz function or more generally in L1(Cm)∩L2(Cm). For general functions in L2(Cm) the Fourier transform is then extended by density in the usual way; see, e.g., Sec 7.1 in Ref. [56].
  59. To be precise, this property holds rigorously for all states ρ such that Wρ∈L1(Cm) (see Proposition 18 in Ref. [64]), which is a proper subset of the set of all states.
  60. R. L. Hudson, When is the Wigner quasi-probability density non-negative? Rep. Math. Phys. 6, 249 (1974).
  61. Francisco Soto and Pierre Claverie, When is the Wigner function of multidimensional systems nonnegative? J. Math. Phys. 24, 97 (1983).
  62. Radim Filip and Ladislav Mišta, Detecting quantum states with a positive Wigner function beyond mixtures of Gaussian states, Phys. Rev. Lett. 106, 200401 (2011).
  63. A. Mandilara, E. Karpov, and N. J. Cerf, Extending Hudson’s theorem to mixed quantum states, Phys. Rev. A 79, 062302 (2009).
  64. M. A. De Gosson, The Wigner Transform, Advanced Textbooks In Mathematics (World Scientific Publishing Company, 2017).
  65. Note that the condition on Yλ uniquely determines its distribution to be P(Yλ=r)=(1+g(λ)/r)/2 and P(Yλ=−r)=(1−g(λ)/r)/2.
  66. Wassily Hoeffding, Probability inequalities for sums of bounded random variables, J. Amer. Statist. Assoc. 58, 13 (1963).
  67. Richard Askey and Stephen Wainger, Mean convergence of expansions in Laguerre and Hermite series, Am. J. Math. 87, 695 (1965).
  68. L. J. Landau, Bessel functions: Monotonicity and bounds, J. London Math. Soc. 61, 197 (2000).
  69. G. Szegö, Orthogonal Polynomials (Colloquium Publications, American Mathematical Society, Rhode island, 1975), https://books.google.fr/books?id=ZOhmnsXlcY0C.
  70. U. Leonhardt and H. Paul, Measuring the quantum state of light, Prog. Quantum Electron. 19, 89 (1995).
  71. Stefan Scheel, Quantum optics. Available at https://www.lkv.uni-rostock.de/storages/uni-rostock/Alle_MNF/Physik_Qms/Lehre_Scheel/quantenoptik/Quantenoptik-Vorlesung4.pdf.
  72. This can be seen by denoting the Bessel function of order n∈N by Jn and using J0′=−J1 and the recurrence relation Jn′=12(Jn−1−Jn+1) [see Eq. (9.1.27) in Ref. [81] ] combined with the fact that |Jn(y)|≤1 for all y∈R [see Eq. (9.1.60) in Ref. [81] ].
  73. T. M. Apostol, Calculus (John Wiley & Sons, New York, 1991), Vol. 1, https://books.google.fr/books?id=o2D4DwAAQBAJ.
  74. Elizabeth Meckes and Mark Meckes, Spectral measures of powers of random matrices, Electron. Commun. Probab. 18, 1 (2013).
  75. This can be seen by infε′∈[0,ε)‖f‖1(ε′)/(ε−ε′)≥(‖f‖1/ε)−Cε−(1−β)=Ω(‖f‖1/ε) together with ‖f‖1(ε)≤‖f‖1.
  76. More precisely, to show that an exponentially decaying function f satisfies Eq. (A6) for all a∈(0,1), we note that ∫{|f|≤δ<e−t|α|}|f(α)|dα≤∫0ln((1/δ)1/t)δdα=δ/tln(1/δ).
  77. Robert Salzmann, Quantitative quantum Zeno and strong damping limits in strong topology, ArXiv:quant-ph/2409.06469.
  78. Andreas Winter, Energy-constrained diamond norm with applications to the uniform continuity of continuous variable channel capacities, ArXiv:quant-ph/1712.10267.
  79. Simon Becker and Nilanjana Datta, Convergence rates for quantum evolution and entropic continuity bounds in infinite dimensions, Commun. Math. Phys. 374, 823 (2019).
  80. Note that finiteness of this integral is not immediately translatable into finiteness of the average photon number Tr(Nρ)=∫Wρ(α)|α|2dα because of the absolute value around the Wigner function Wρ(α). Regardless, finiteness of ∫C|Wρ(α)|E+|α|2 corresponds to fast decay of Wρ(α) for large values of |α|, which we, therefore, interpret as some form of energy constraint.
  81. Milton Abramowitz and Irene A. Stegun, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables (Dover, New York, 1964), 9th Dover Printing, 10th GPO Printing ed.

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