pith. machine review for the scientific record. sign in

arxiv: 2605.11924 · v1 · submitted 2026-05-12 · 🪐 quant-ph

Recognition: no theorem link

Joint Realizability Tradeoffs Bounded by Quantum Channel Incompatibility

Authors on Pith no claims yet

Pith reviewed 2026-05-13 05:15 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum channel incompatibilitygeneralized robustnessjoint realizabilitytradeoff relationsmeasurement uncertaintyPOVMsinformation-disturbance tradeoff
0
0 comments X

The pith

Generalized robustness of channel incompatibility lower-bounds the total error of any approximate joint realization.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper connects the resource strength of incompatible quantum channels to the accuracy limits of implementing them jointly in approximate form. It proves that generalized robustness, a standard quantifier of incompatibility, provides a lower bound on the total error of any such joint approximation. This link unifies traditional quantum limitations including measurement uncertainty relations, the no-information-without-disturbance principle, and no-cloning or no-broadcasting theorems under one resource-theoretic umbrella. A reader would care because the result supplies a model-independent way to quantify these tradeoffs for arbitrary channels rather than relying on case-by-case algebraic derivations.

Core claim

In this Letter, we show that generalized robustness, a typical resource quantifier of channel incompatibility, lower bounds the total error of any approximate joint realization. Applying this result to measurement channels provides a unified, model-independent framework encompassing error-error and information-error-disturbance tradeoffs. Furthermore, our robustness-based evaluation of disturbance outperforms an algebraic bound for all POVMs in dimensions up to six.

What carries the argument

Generalized robustness of channel incompatibility, a resource quantifier that directly lower-bounds the minimal total error achievable in any approximate joint realization of the channels.

If this is right

  • Measurement channels inherit a single bound that covers both error-error tradeoffs and information-disturbance tradeoffs without separate derivations.
  • The robustness bound on disturbance is strictly tighter than the previous algebraic bound for every POVM in dimensions two through six.
  • Incompatibility strength can now be read directly from the minimal error of an approximate joint implementation rather than from abstract algebraic relations.
  • The same lower bound extends to unify no-cloning, no-broadcasting, and no-information-without-disturbance as special cases of channel incompatibility.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • The bound could be used to certify the incompatibility resource by performing only joint-approximation experiments rather than full channel tomography.
  • Similar robustness-to-error relations might be derived for other resource theories of quantum channels, such as those for coherence or entanglement.
  • Low-dimensional numerical checks already shown to outperform algebraic bounds suggest immediate experimental tests with qubits or qutrits.

Load-bearing premise

The assumption that generalized robustness correctly quantifies the incompatibility resource for arbitrary channels and that the definition of joint-realizability error aligns exactly with the robustness functional.

What would settle it

An explicit pair of incompatible channels together with a concrete joint realization whose total error falls below the generalized robustness value computed for those channels.

Figures

Figures reproduced from arXiv: 2605.11924 by Kensei Torii, Ryo Takakura, Shintaro Minagawa.

Figure 1
Figure 1. Figure 1: FIG. 1. Approximate joint realization tradeoff of two quan [PITH_FULL_IMAGE:figures/full_fig_p003_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2. Comparison with the robustness-based bound [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3. Comparison with our robustness-based bound 2( [PITH_FULL_IMAGE:figures/full_fig_p020_3.png] view at source ↗
read the original abstract

Incompatible quantum channels cannot be jointly and exactly realized, meaning that any approximate joint realization inevitably entails a tradeoff in implementation accuracy. While this notion of channel incompatibility unifies fundamental limitations such as measurement uncertainty, the no information without disturbance principle, and the no-cloning and no-broadcasting theorems, connecting these traditional relations directly to the resource-theoretic strength of incompatibility has remained elusive. In this Letter, we show that generalized robustness, a typical resource quantifier of channel incompatibility, lower bounds the total error of any approximate joint realization. Applying this result to measurement channels provides a unified, model-independent framework encompassing error-error and information-error-disturbance tradeoffs. Furthermore, our robustness-based evaluation of disturbance outperforms an algebraic bound for all POVMs in dimensions up to six.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 3 minor

Summary. The paper claims that generalized robustness of channel incompatibility lower-bounds the total error of any approximate joint realization of incompatible quantum channels. The central result follows from a variational definition of robustness (minimum s such that a convex combination with a compatible channel is jointly realizable) and a direct construction showing that any approximate joint implementation with total error e (infimum of summed diamond-norm distances) yields a feasible witness for the robustness program with value at most e. The bound is applied to measurement channels to recover unified error-error and information-disturbance tradeoffs, with numerical comparisons showing the robustness-based disturbance bound outperforming an algebraic alternative for all POVMs in dimensions up to 6.

Significance. If the result holds, it supplies a resource-theoretic lower bound on joint-realizability error that is derived directly from the definitions without extra assumptions on dimension or channel class. This cleanly connects incompatibility quantifiers to operational tradeoffs, encompassing measurement uncertainty, no-disturbance principles, and no-cloning in a model-independent framework. The explicit witness construction and the numerical evaluation up to dimension 6 are concrete strengths that make the bound falsifiable and practically usable.

minor comments (3)
  1. [§2] §2, after Eq. (3): the total-error functional is defined as an infimum over summed distances, but the precise choice of distance (diamond norm versus another channel metric) and whether the sum is normalized by the number of channels should be stated explicitly to avoid ambiguity in the subsequent theorem.
  2. [§4] §4, numerical section: the statement that the robustness bound 'outperforms an algebraic bound for all POVMs' in dimensions up to 6 would be strengthened by reporting the exact number of random POVMs sampled per dimension and the precise algebraic bound being compared (e.g., which reference or formula).
  3. [Figure 2] Figure 2 caption: the plot labels for disturbance versus incompatibility strength should include error bars or indicate that the curves are deterministic lower bounds rather than sampled averages.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their careful reading and positive assessment of our manuscript. The provided summary accurately reflects the central contribution: that the generalized robustness of channel incompatibility lower-bounds the total error of any approximate joint realization, with direct applications to measurement uncertainty and disturbance tradeoffs. We appreciate the recognition of the variational construction and the numerical comparisons up to dimension 6. No specific major comments were raised in the report.

Circularity Check

0 steps flagged

No significant circularity identified

full rationale

The central theorem establishes that generalized robustness lower-bounds total joint-realization error by exhibiting an explicit feasible witness for the robustness variational program whose value is at most the error e. Both quantities are defined independently (robustness via convex combination with a compatible channel; error via infimum of summed implementation distances), and the inequality follows directly from these definitions without any self-referential reduction, fitted parameters, or load-bearing self-citations. Applications to POVMs and numerical checks are corollaries that inherit the same non-circular structure. The derivation is therefore self-contained.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Abstract-only review; cannot enumerate free parameters or axioms because the mathematical definitions and derivations are not supplied.

pith-pipeline@v0.9.0 · 5428 in / 1009 out tokens · 17980 ms · 2026-05-13T05:15:47.248796+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Reference graph

Works this paper leans on

87 extracted references · 87 canonical work pages · 1 internal anchor

  1. [1]

    Joint Realizability Tradeoffs Bounded by Quantum Channel Incompatibility

    in two to six-dimensional systems for any non-trivial POVMs. Preliminaries—. Following Refs. [39–41], we only con- sider finite-dimensional Hilbert spacesH A,H B,.... The set of all linear operators fromH A toH B is written as L(HA,H B), endowed with the trace norm∥·∥1, the op- erator norm∥·∥, and the Hilbert-Schmidt inner product ⟨Y,X⟩:= Tr[Y†X]. We writ...

  2. [2]

    acknowledges support from the French govern- ment under the France 2030 investment plan, as part of the Initiative d’Excellence d’Aix-Marseille Universit´ e- A*MIDEX, AMX-22-CEI-01

    S.M. acknowledges support from the French govern- ment under the France 2030 investment plan, as part of the Initiative d’Excellence d’Aix-Marseille Universit´ e- A*MIDEX, AMX-22-CEI-01. R.T. thanks Takayuki Miyadera for insightful discussions. R.T. acknowl- edges support from JST COI-NEXT program Grant No. JPMJPF2014, and JSPS KAKENHI Grant No. JP25K1731...

  3. [3]

    Busch, P

    P. Busch, P. J. Lahti, J.-P. Pellonp¨ a¨ a, and K. Ylinen, Quantum Measurement(Springer International Pub- lishing, 2016)

  4. [4]

    G¨ uhne, E

    O. G¨ uhne, E. Haapasalo, T. Kraft, J.-P. Pellonp¨ a¨ a, and R. Uola, Colloquium: Incompatible measurements in quantum information science, Rev. Mod. Phys.95, 011003 (2023)

  5. [5]

    no information without disturbance

    P. Busch, “no information without disturbance”: Quan- tum limitations of measurement in quantum reality. in wayne c. myrvold and joy christian (eds.) relativistic causality, and closing the epistemic circle: Essays in honour of abner shimony, inQuantum Reality , Rela- tivistic Causality , and Closing the Epistemic Cir- cle: Essays in Honour of Abner Shimo...

  6. [6]

    G. M. D’Ariano, G. Chiribella, and P. Perinotti,Quan- tum Theory from First Principles: An Informa- tional Approach(Cambridge University Press, Cam- bridge, UK, 2017)

  7. [7]

    W. K. Wootters and W. H. Zurek, A single quantum cannot be cloned, Nature299, 802 (1982)

  8. [8]

    Dieks, Communication by EPR devices, Phys

    D. Dieks, Communication by EPR devices, Phys. Lett. A92, 271 (1982)

  9. [9]

    Wiesner, Conjugate coding, SIGACT News15, 78–88 (1983)

    S. Wiesner, Conjugate coding, SIGACT News15, 78–88 (1983)

  10. [10]

    Barnum, C

    H. Barnum, C. M. Caves, C. A. Fuchs, R. Jozsa, and B. Schumacher, Noncommuting mixed states cannot be broadcast, Phys. Rev. Lett.76, 2818 (1996)

  11. [11]

    Barnum, J

    H. Barnum, J. Barrett, M. Leifer, and A. Wilce, Gen- eralized no-broadcasting theorem, Phys. Rev. Lett.99, 240501 (2007)

  12. [12]

    Heinosaari and T

    T. Heinosaari and T. Miyadera, Incompatibility of quan- tum channels, J. Phys. A: Math. Theor.50, 135302 (2017)

  13. [13]

    Heinosaari, T

    T. Heinosaari, T. Miyadera, and M. Ziman, An invitation to quantum incompatibility, J. Phys. A: Math. Theor.49, 123001 (2016)

  14. [14]

    W. K. Heisenberg, ¨Uber den anschaulichen inhalt der quantentheoretischen kinematik und mechanik, Zeitschrift f¨ ur Physik43, 172 (1927)

  15. [15]

    Ozawa, Universally valid reformulation of the Heisen- berg uncertainty principle on noise and disturbance in measurement, Phys

    M. Ozawa, Universally valid reformulation of the Heisen- berg uncertainty principle on noise and disturbance in measurement, Phys. Rev. A67, 042105 (2003)

  16. [16]

    Ozawa, Uncertainty relations for joint measurements of noncommuting observables, Phys

    M. Ozawa, Uncertainty relations for joint measurements of noncommuting observables, Phys. Lett. A320, 367 (2004)

  17. [17]

    Watanabe, T

    Y. Watanabe, T. Sagawa, and M. Ueda, Uncertainty re- lation revisited from quantum estimation theory, Phys. Rev. A84, 042121 (2011)

  18. [18]

    Busch, P

    P. Busch, P. Lahti, and R. F. Werner, Proof of Heisen- berg’s error-disturbance relation, Phys. Rev. Lett.111, 160405 (2013)

  19. [19]

    Branciard, Error-tradeoff and error-disturbance re- lations for incompatible quantum measurements, Proc

    C. Branciard, Error-tradeoff and error-disturbance re- lations for incompatible quantum measurements, Proc. Natl. Acad. Sci.110, 6742 (2013)

  20. [20]

    Buscemi, M

    F. Buscemi, M. J. W. Hall, M. Ozawa, and M. M. Wilde, Noise and disturbance in quantum measurements: An information-theoretic approach, Phys. Rev. Lett.112, 050401 (2014)

  21. [21]

    Maccone, Information-disturbance tradeoff in quan- tum measurements, Phys

    L. Maccone, Information-disturbance tradeoff in quan- tum measurements, Phys. Rev. A73, 042307 (2006)

  22. [22]

    Buscemi and M

    F. Buscemi and M. F. Sacchi, Information-disturbance trade-off in quantum-state discrimination, Phys. Rev. A 74, 052320 (2006)

  23. [23]

    Maccone, Entropic information-disturbance tradeoff, Europhys

    L. Maccone, Entropic information-disturbance tradeoff, Europhys. Lett.77, 40002 (2007)

  24. [24]

    Kretschmann, D

    D. Kretschmann, D. Schlingemann, and R. F. Werner, The information-disturbance tradeoff and the continuity of Stinespring’s representation, IEEE Trans. Inf. Theory 54, 1708 (2008)

  25. [25]

    Heinosaari and T

    T. Heinosaari and T. Miyadera, Qualitative noise- disturbance relation for quantum measurements, Phys. Rev. A88, 042117 (2013)

  26. [26]

    G. M. D’Ariano, P. Perinotti, and A. Tosini, Informa- tion and disturbance in operational probabilistic theories, Quantum4, 363 (2020). 6

  27. [27]

    Skrzypczyk, I

    P. Skrzypczyk, I. ˇSupi´ c, and D. Cavalcanti, All sets of incompatible measurements give an advantage in quan- tum state discrimination, Phys. Rev. Lett.122, 130403 (2019)

  28. [28]

    Carmeli, T

    C. Carmeli, T. Heinosaari, and A. Toigo, Quantum in- compatibility witnesses, Phys. Rev. Lett.122, 130402 (2019)

  29. [29]

    R. Uola, T. Kraft, J. Shang, X.-D. Yu, and O. G¨ uhne, Quantifying quantum resources with conic programming, Phys. Rev. Lett.122, 130404 (2019)

  30. [30]

    Mori, Operational characterization of incompatibility of quantum channels with quantum state discrimination, Phys

    J. Mori, Operational characterization of incompatibility of quantum channels with quantum state discrimination, Phys. Rev. A101, 032331 (2020)

  31. [31]

    R. Uola, T. Kraft, and A. A. Abbott, Quantification of quantum dynamics with input-output games, Phys. Rev. A101, 052306 (2020)

  32. [32]

    A. F. Ducuara, R. Takakura, F. J. Hernandez, and C. E. Susa, Multiobject operational tasks for measurement in- compatibility, Phys. Rev. Res.7, 033050 (2025)

  33. [33]

    Vidal and R

    G. Vidal and R. Tarrach, Robustness of entanglement, Phys. Rev. A59, 141 (1999)

  34. [34]

    Steiner, Generalized robustness of entanglement, Phys

    M. Steiner, Generalized robustness of entanglement, Phys. Rev. A67, 054305 (2003)

  35. [35]

    Datta, Max-Relative Entropy of Entanglement, Alias Log Robustness, Int

    N. Datta, Max-Relative Entropy of Entanglement, Alias Log Robustness, Int. J. Quantum Inf.07, 475 (2009)

  36. [36]

    Skrzypczyk and N

    P. Skrzypczyk and N. Linden, Robustness of measure- ment, discrimination games, and accessible information, Phys. Rev. Lett.122, 140403 (2019)

  37. [37]

    Oszmaniec and T

    M. Oszmaniec and T. Biswas, Operational relevance of resource theories of quantum measurements, Quantum3, 133 (2019)

  38. [38]

    Takagi and B

    R. Takagi and B. Regula, General resource theories in quantum mechanics and beyond: Operational character- ization via discrimination tasks, Phys. Rev. X9, 031053 (2019)

  39. [39]

    Chitambar and G

    E. Chitambar and G. Gour, Quantum resource theories, Rev. Mod. Phys.91, 025001 (2019)

  40. [40]

    Gour,Quantum Resource Theories(Cambridge University Press, Cambridge, UK, 2025)

    G. Gour,Quantum Resource Theories(Cambridge University Press, Cambridge, UK, 2025)

  41. [41]

    M. A. Nielsen and I. L. Chuang,Quantum Compu- tation and Quantum Information: 10th Anniver- sary Edition(Cambridge University Press, Cambridge, UK, 2010)

  42. [42]

    M. M. Wilde,Quantum Information Theory, 2nd ed. (Cambridge University Press, Cambridge, UK, 2017)

  43. [43]

    Watrous,The Theory of Quantum Information (Cambridge University Press, Cambridge, UK, 2018)

    J. Watrous,The Theory of Quantum Information (Cambridge University Press, Cambridge, UK, 2018)

  44. [44]

    A. S. Holevo and A. A. Kuznetsova, Information capacity of continuous variable measurement channel, J. Phys. A: Math. Theor.53, 175304 (2020)

  45. [45]

    Ozawa, Quantum measuring processes of continuous observables, J

    M. Ozawa, Quantum measuring processes of continuous observables, J. Math. Phys.25, 79 (1984)

  46. [46]

    Watrous, Semidefinite programs for completely bounded norms, Theory of Computing5, 217 (2009)

    J. Watrous, Semidefinite programs for completely bounded norms, Theory of Computing5, 217 (2009)

  47. [47]

    Ben-Aroya and A

    A. Ben-Aroya and A. Ta-Shma, On the complexity of approximating the diamond norm, Quantum Information and Computation10, 77 (2010)

  48. [48]

    Watrous, Simpler semidefinite programs for completely bounded norms, Chicago J

    J. Watrous, Simpler semidefinite programs for completely bounded norms, Chicago J. Theor. Comput. Sci.2013, 10.4086/cjtcs.2013.008 (2013)

  49. [49]

    Boyd and L

    S. Boyd and L. Vandenberghe,Convex Optimization (Cambridge University Press, Cambridge, UK, 2004)

  50. [50]

    Heinosaari, J

    T. Heinosaari, J. Kiukas, and D. Reitzner, Noise robust- ness of the incompatibility of quantum measurements, Phys. Rev. A92, 022115 (2015)

  51. [51]

    R. Uola, C. Budroni, O. G¨ uhne, and J.-P. Pellonp¨ a¨ a, One-to-one mapping between steering and joint measur- ability problems, Phys. Rev. Lett.115, 230402 (2015)

  52. [52]

    Haapasalo, Robustness of incompatibility for quantum devices, J

    E. Haapasalo, Robustness of incompatibility for quantum devices, J. Phys. A: Math. Theor.48, 255303 (2015)

  53. [53]

    Designolle, M

    S. Designolle, M. Farkas, and J. Kaniewski, Incompat- ibility robustness of quantum measurements: a unified framework, New J. Phys.21, 113053 (2019)

  54. [54]

    Guerini, J

    L. Guerini, J. Bavaresco, M. Terra Cunha, and A. Ac ´ ın, Operational framework for quantum measurement simu- lability, J. Math. Phys.58, 092102 (2017)

  55. [55]

    See Supplemental Material

  56. [56]

    Arthurs and J

    E. Arthurs and J. L. Kelly Jr., On the simultaneous mea- surement of a pair of conjugate observables, Bell Syst. Tech. J.44, 725 (1965)

  57. [57]

    Arthurs and M

    E. Arthurs and M. S. Goodman, Quantum correlations: A generalized Heisenberg uncertainty relation, Phys. Rev. Lett.60, 2447 (1988)

  58. [58]

    Busch and P

    P. Busch and P. J. Lahti, On various joint measurements of position and momentum observables in quantum the- ory, Phys. Rev. D29, 1634 (1984)

  59. [59]

    R. F. Werner, The uncertainty relation for joint measure- ment of position and momentum, Quantum Info. Com- put.4, 546–562 (2004)

  60. [60]

    Busch and D

    P. Busch and D. B. Pearson, Universal joint-measurement uncertainty relation for error bars, J. Math. Phys.48, 082103 (2007)

  61. [61]

    Busch, T

    P. Busch, T. Heinonen, and P. Lahti, Heisenberg’s uncer- tainty principle, Phys. Rep.452, 155 (2007)

  62. [62]

    Busch, Unsharp reality and joint measurements for spin observables, Phys

    P. Busch, Unsharp reality and joint measurements for spin observables, Phys. Rev. D33, 2253 (1986)

  63. [63]

    Busch and T

    P. Busch and T. Heinosaari, Approximate joint measure- ments of qubit observables, Quantum Inform. Compu.8, 797–818 (2008)

  64. [64]

    Miyadera and H

    T. Miyadera and H. Imai, Heisenberg’s uncertainty prin- ciple for simultaneous measurement of positive-operator- valued measures, Phys. Rev. A78, 052119 (2008)

  65. [65]

    Takakura and T

    R. Takakura and T. Miyadera, Preparation uncertainty implies measurement uncertainty in a class of generalized probabilistic theories, J. Math. Phys.61, 082203 (2020)

  66. [66]

    Ozawa, Soundness and completeness of quantum root- mean-square errors, npj Quantum Inf.5, 1 (2019)

    M. Ozawa, Soundness and completeness of quantum root- mean-square errors, npj Quantum Inf.5, 1 (2019)

  67. [67]

    Mitra, S

    A. Mitra, S. Mukherjee, and C. Lee, Distance-based mea- sures and epsilon measures for measurement-based quan- tum resources, Phys. Rev. A112, 062233 (2025)

  68. [68]

    Ghai and A

    J. Ghai and A. Mitra, Instrument-based quantum re- sources: quantification, hierarchies and towards con- structing resource theories (2025), arXiv:2508.09134 [quant-ph]

  69. [69]

    Busch, On the sharpness and bias of quantum effects, Found

    P. Busch, On the sharpness and bias of quantum effects, Found. Phys.39, 712 (2009)

  70. [70]

    von Neumann,Mathematical foundations of quantum mechanics(Princeton University Press, Princeton, NJ, 1955)

    J. von Neumann,Mathematical foundations of quantum mechanics(Princeton University Press, Princeton, NJ, 1955)

  71. [71]

    E. H. Kennard, Zur quantenmechanik einfacher bewe- gungstypen, Zeitschrift f¨ ur Physik44, 326 (1927)

  72. [72]

    H. P. Robertson, The uncertainty principle, Phys. Rev. 34, 163 (1929)

  73. [73]

    Mitra and M

    A. Mitra and M. Farkas, Compatibility of quantum in- struments, Phys. Rev. A105, 052202 (2022)

  74. [74]

    Mitra and M

    A. Mitra and M. Farkas, Characterizing and quantifying the incompatibility of quantum instruments, Phys. Rev. A107, 032217 (2023). 7

  75. [75]

    Lepp¨ aj¨ arvi and M

    L. Lepp¨ aj¨ arvi and M. Sedl´ ak, Incompatibility of quantum instruments, Quantum8, 1246 (2024)

  76. [76]

    Buscemi, K

    F. Buscemi, K. Kobayashi, S. Minagawa, P. Perinotti, and A. Tosini, Unifying different notions of quantum in- compatibility into a strict hierarchy of resource theories of communication, Quantum7, 1035 (2023)

  77. [77]

    Ji and E

    K. Ji and E. Chitambar, Incompatibility as a resource for programmable quantum instruments, PRX Quantum5, 010340 (2024)

  78. [78]

    R. Uola, T. Bullock, T. Kraft, J.-P. Pellonp¨ a¨ a, and N. Brunner, All quantum resources provide an advantage in exclusion tasks, Phys. Rev. Lett.125, 110402 (2020)

  79. [79]

    Sudarsanan Ragini and S

    N. Sudarsanan Ragini and S. Sazim, Higher-order incom- patibility improves distinguishability of causal quantum networks, New Journal of Physics26, 123003 (2024)

  80. [80]

    Choi, Completely positive linear maps on com- plex matrices, Linear algebra and its applications10, 285 (1975)

    M.-D. Choi, Completely positive linear maps on com- plex matrices, Linear algebra and its applications10, 285 (1975)

Showing first 80 references.