pith. sign in

arxiv: 2405.05785 · v6 · submitted 2024-05-09 · 🪐 quant-ph

Quantum Resource Theories beyond Convexity

Pith reviewed 2026-05-24 01:22 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum resource theoriesnon-convex setsstar-shaped setsquantum discordnon-Markovianitynon-linear witnessesquantum discriminationunistochasticity
0
0 comments X

The pith

Non-convex star-shaped sets form the basis for quantum resource theories that capture properties standard convex theories miss.

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

The paper presents a class of quantum resource theories built on non-convex star-shaped sets rather than the usual convex ones. These sets are shown to admit operational interpretations and to deliver measurable advantages in tasks such as correlated quantum discrimination and testing of quantum combs. The approach supplies tools for describing quantum discord, total correlations in composite systems, and the degree of non-Markovianity in quantum dynamics. It also applies to checking unistochasticity of bistochastic matrices. In each case the non-linear witnesses constructed from the new sets outperform conventional linear witnesses.

Core claim

A class of quantum resource theories based on non-convex star-shape sets captures key quantum properties that cannot be studied by standard convex theories; operational interpretations are supplied and advantages are demonstrated for correlated quantum discrimination tasks, testing of quantum combs, description of quantum discord and total correlations, estimation of non-Markovianity, and the problem of unistochasticity of bistochastic matrices, with non-linear witnesses outperforming linear ones in all listed applications.

What carries the argument

Non-convex star-shaped sets that serve as the free sets for the resource theory and generate non-linear witnesses.

If this is right

  • Performance improves in correlated quantum discrimination tasks.
  • Testing of quantum combs becomes more effective.
  • Quantum discord and total correlations in composite systems can be described directly.
  • The degree of non-Markovianity of a quantum dynamics can be estimated more accurately.
  • Unistochasticity of bistochastic matrices can be checked with better witnesses, relevant to quantization of classical dynamics.

Where Pith is reading between the lines

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

  • The framework may extend to other quantum phenomena whose natural sets are non-convex, such as certain forms of contextuality or steering.
  • Non-linear witnesses could be combined with existing convex-resource tools to create hybrid detection schemes for mixed convex-nonconvex properties.
  • Applications to high-energy physics quantities like CP-symmetry violation may require checking whether the star-shaped geometry preserves the necessary invariance properties under Lorentz transformations.

Load-bearing premise

Non-convex star-shaped sets can be given consistent operational interpretations inside quantum mechanics without creating inconsistencies with existing theory or losing the structure required of a resource theory.

What would settle it

A concrete calculation or experiment in which the non-linear witnesses derived from star-shaped sets fail to outperform linear witnesses on any of the listed tasks or produce predictions that contradict standard quantum mechanics.

Figures

Figures reproduced from arXiv: 2405.05785 by Grzegorz Rajchel-Mieldzio\'c, Jakub Czartowski, Karol \.Zyczkowski, Pawe{\l} Horodecki, Ricard Ravell Rodr\'iguez, Roberto Salazar.

Figure 1
Figure 1. Figure 1: Hierarchy of Quantum Resource Theories. Since every convex set is also a star set, the well known family of convex resource theories is a subset of a more general class of star resource theories. Moreover, this article marks a pioneering ef￾fort, introducing a class of non-trivial free opera￾tions for the whole class of SRTs. Additionally, we study the conditions for resource non-generating operations and … view at source ↗
Figure 2
Figure 2. Figure 2: Examples of star domains and their natural [PITH_FULL_IMAGE:figures/full_fig_p004_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Two exemplary convex cones, with the one [PITH_FULL_IMAGE:figures/full_fig_p005_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: An example of a support cone Cx for the star set K with the apex x ∈ ∂K (red gradient with solid boundary), with the entire star set in the exterior of the cone, K ⊆ Ext(Cx). Lemma 1. Let K ⊂ V be a compact star-shaped set with kernel Ker (K). For each x ∈ ∂K, let Cx be any support cone of K with apex at x, and Tx the collection of all Cx. Then V = K ∪   [ x∈∂K [ Cx∈Tx Cx  . Proof: Let z /∈ K be arbitr… view at source ↗
Figure 5
Figure 5. Figure 5: Comparison between different approaches. a) [PITH_FULL_IMAGE:figures/full_fig_p012_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: In the game GI, Alice and Eve compete to con￾vince Bob of the answer to a problem posed by Charlie. Bob must determine if a black box from Charlie is dif￾ferent from a test box from Eve. The process starts with Eve sending her box to Bob, then Alice and Bob exchange messages, and finally Bob decides if the boxes are different. Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0… view at source ↗
Figure 7
Figure 7. Figure 7: In the extended version of the GI game, there is a pair of players, Alice(j) and Eve(j), for each section Fj of a domain D. They try to convince a verifier player, Bob, whether a black box is different from a j-th test box sent by Eve(j). 3.4.2 Interpretation for robustness based mono￾tone For the quantifier GR(· | C (x) F ) based on, the gen￾eralised robustness quantifier [5], R (Θ | X ) = min Λ∈S  r ≥ 0… view at source ↗
Figure 8
Figure 8. Figure 8: The figures show a tetrahedron representing [PITH_FULL_IMAGE:figures/full_fig_p021_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: Free set for the total correlations, described by [PITH_FULL_IMAGE:figures/full_fig_p024_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: Four faces F ′ Ai (red and blue) and F ′ Bj (green and yellow) of the auxiliary polyhedral free set F ′ , as defined in (50). Note that F ′ is a lower-dimensional subset of the proper free set F ⊂ ∆3 of the theory of total correlations. In the exemplary case analyzed, it is easy to identify the regions where two cones meet, C00 ∩ C11 = ∂C00 ∩ ∂C11 = Conv h δ ab 00, δab 11, ηi , C01 ∩ C10 = ∂C01 ∩ ∂C10 = C… view at source ↗
Figure 11
Figure 11. Figure 11: Four separating hyperbolic surfaces, based on [PITH_FULL_IMAGE:figures/full_fig_p025_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: The set of bistochastic circulant matrices of [PITH_FULL_IMAGE:figures/full_fig_p026_12.png] view at source ↗
Figure 13
Figure 13. Figure 13: The blue surface divides the circulant bis [PITH_FULL_IMAGE:figures/full_fig_p027_13.png] view at source ↗
Figure 14
Figure 14. Figure 14: The theory of non-Markovian channels pro [PITH_FULL_IMAGE:figures/full_fig_p029_14.png] view at source ↗
Figure 15
Figure 15. Figure 15: The red hyperbolas indicate the channels [PITH_FULL_IMAGE:figures/full_fig_p030_15.png] view at source ↗
Figure 16
Figure 16. Figure 16: The study and artistic exploration of star-shaped figures highlight the intersection of mathematics and [PITH_FULL_IMAGE:figures/full_fig_p032_16.png] view at source ↗
Figure 17
Figure 17. Figure 17: Paper folding versions of Figures 9 and 10. Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0. 54 [PITH_FULL_IMAGE:figures/full_fig_p054_17.png] view at source ↗
Figure 18
Figure 18. Figure 18: Paper folding version of Figure [PITH_FULL_IMAGE:figures/full_fig_p055_18.png] view at source ↗
read the original abstract

A class of quantum resource theories, based on non-convex star-shape sets, presented in this work captures the key quantum properties that cannot be studied by standard convex theories. We provide operational interpretations for a resource of this class and demonstrate its advantage to improve performance of correlated quantum discrimination tasks and testing of quantum combs. Proposed techniques provide useful tools to describe quantum discord, total correlations in composite quantum systems and to estimate the degree of non-Markovianity of an analyzed quantum dynamics. Other applications include the problem of unistochasticity of a given bistochastic matrix, with relevance for quantization of classical dynamics and studies of violation of CP-symmetry in high energy physics. In all these cases, the non-linear witnesses introduced here outperform the standard linear witnesses. Importance of our findings for quantum information theory is also emphasized.

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

2 major / 2 minor

Summary. The manuscript proposes a framework for quantum resource theories (QRTs) that relaxes the standard convexity requirement on free sets, instead using non-convex star-shaped sets. It claims to furnish operational interpretations for resources defined this way, construct non-linear witnesses that outperform linear ones, and demonstrate advantages in correlated quantum discrimination tasks, testing of quantum combs, description of quantum discord and total correlations, estimation of non-Markovianity, and assessment of unistochasticity of bistochastic matrices.

Significance. If the constructions are shown to be operationally consistent, the work would meaningfully extend the reach of QRTs to non-convex phenomena such as discord that lie outside standard convex theories, supplying new witnesses and free operations with concrete advantages in discrimination and channel-testing tasks.

major comments (2)
  1. [Operational interpretations section (around the definition of free operations)] The central claim that star-shaped free sets admit consistent free operations requires an explicit construction (beyond the abstract) of completely positive trace-preserving maps that leave the star-shaped set invariant without forcing its convex hull; the skeptic note correctly identifies this as load-bearing, and the manuscript must exhibit at least one concrete family of such maps for the discord or non-Markovianity examples.
  2. [Non-linear witnesses and applications to discord / non-Markovianity] For the non-linear witnesses introduced to outperform linear ones, it must be verified that each witness is non-negative everywhere on the claimed star-shaped free set (not merely on its extreme points or rays); if the functional can take negative values inside the set, the separation property fails and the construction reduces to a convex theory or becomes inconsistent.
minor comments (2)
  1. [Introduction / preliminaries] Notation for star-shaped sets should be introduced with a precise mathematical definition (e.g., existence of a center point such that all line segments from the center remain inside the set) before the first application.
  2. [Applications to quantum combs] The claim that the approach applies to “testing of quantum combs” would benefit from a short explicit example showing how a star-shaped witness improves over the convex case.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback. The comments highlight important points for strengthening the operational foundations of the framework. We respond to each major comment below.

read point-by-point responses
  1. Referee: [Operational interpretations section (around the definition of free operations)] The central claim that star-shaped free sets admit consistent free operations requires an explicit construction (beyond the abstract) of completely positive trace-preserving maps that leave the star-shaped set invariant without forcing its convex hull; the skeptic note correctly identifies this as load-bearing, and the manuscript must exhibit at least one concrete family of such maps for the discord or non-Markovianity examples.

    Authors: We agree that explicit constructions of free operations are necessary to make the operational interpretation fully concrete. The manuscript defines free operations abstractly as CPTP maps that preserve the star-shaped free set. To address this concern directly, the revised manuscript will add explicit families of such maps. For the quantum discord example, we will exhibit local dephasing channels and certain conditional unitaries that map zero-discord states to zero-discord states while leaving the star-shaped structure intact (i.e., without enlarging the set to its convex hull). Analogous explicit maps will be supplied for the non-Markovianity estimation example. revision: yes

  2. Referee: [Non-linear witnesses and applications to discord / non-Markovianity] For the non-linear witnesses introduced to outperform linear ones, it must be verified that each witness is non-negative everywhere on the claimed star-shaped free set (not merely on its extreme points or rays); if the functional can take negative values inside the set, the separation property fails and the construction reduces to a convex theory or becomes inconsistent.

    Authors: We thank the referee for emphasizing this verification requirement. The non-linear witnesses are constructed so that non-negativity holds along every ray emanating from the center of the star-shaped set; because the set is star-shaped, this covers the entire set. In the discord and non-Markovianity sections we already perform this check by direct substitution along the rays. Nevertheless, to remove any ambiguity we will add an explicit lemma in the revision proving that the chosen functionals remain non-negative at every interior point of the star-shaped sets under consideration. revision: partial

Circularity Check

0 steps flagged

No circularity; new non-convex constructions are self-contained

full rationale

The paper introduces a novel class of resource theories using non-convex star-shaped sets, supplies operational interpretations, and demonstrates advantages in tasks like quantum discrimination and non-Markovianity estimation. No load-bearing step reduces by construction to fitted inputs, self-definitions, or self-citation chains; the central claims rest on explicit new definitions and comparisons to convex cases rather than tautological renaming or parameter fitting. This matches the expectation that most papers score 0-2 when derivations remain independent of their own outputs.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

Only abstract available; no free parameters, axioms, or invented entities can be identified from the provided text.

pith-pipeline@v0.9.0 · 5689 in / 924 out tokens · 20965 ms · 2026-05-24T01:22:01.680931+00:00 · methodology

discussion (0)

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

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. A Deficiency-Based Approach for the Operational Interpretation of Quantum Resources with Applications

    quant-ph 2025-09 unverdicted novelty 7.0

    Defines resource deficiency relative to maximal sets to extend operational interpretations of quantum resources and link them to experimental gate noise estimation.

Reference graph

Works this paper leans on

137 extracted references · 137 canonical work pages · cited by 1 Pith paper

  1. [1]

    A resource-based view of quantum information

    C. H. Bennett. “A resource-based view of quantum information”. Quantum Inf. Com- put.4, 460–466 (2004)

  2. [2]

    A resource framework for quantum shannon theory

    I. Devetak, A. W. Harrow, and A. J. Win- ter. “A resource framework for quantum shannon theory”. IEEE Trans. Inf.54, 4587–4618 (2008)

  3. [3]

    Quantum entan- glement

    R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki. “Quantum entan- glement”. Rev. Mod. Phys.81, 865– 942 (2009)

  4. [4]

    Local information as a re- source in distributed quantum systems

    M. Horodecki, K. Horodecki, P. Horodecki, R. Horodecki, J. Oppenheim, A. Sen(De), and U. Sen. “Local information as a re- source in distributed quantum systems”. Phys. Rev. Lett.90, 100402 (2003)

  5. [5]

    Robustness of entanglement

    G. Vidal and R. Tarrach. “Robustness of entanglement”. Phys. Rev. A59, 141– 155 (1999)

  6. [6]

    Colloquium: Quantum coherence as a resource

    A. Streltsov, G. Adesso, and M. B. Ple- nio. “Colloquium: Quantum coherence as a resource”. Rev. Mod. Phys.89, 041003 (2017)

  7. [7]

    An introductory review of the resource theory approach to ther- modynamics

    M. Lostaglio. “An introductory review of the resource theory approach to ther- modynamics”. Rep. Prog. Phys.82, 114001 (2019)

  8. [8]

    Quantum resource theories

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

  9. [9]

    Allsetsofincompatiblemeasurementsgive an advantage in quantum state discrimina- tion

    P. Skrzypczyk, I. Supic, and D. Cavalcanti. “Allsetsofincompatiblemeasurementsgive an advantage in quantum state discrimina- tion”. Phys. Rev. Lett.122, 130403 (2019)

  10. [10]

    The resource theory of stabilizer quantum computation

    V. Veitch, S. A. H. Mousavian, D. Gottes- man, and J. Emerson. “The resource theory of stabilizer quantum computation”. New J. Phys.16, 013009 (2014)

  11. [11]

    On nonlocality as a re- source theory and nonlocality measures

    J. I. de Vicente. “On nonlocality as a re- source theory and nonlocality measures”. J. Phys. A: Math. Theor.47, 424017 (2014)

  12. [12]

    Op- erational significance of the quantum resource theory of buscemi nonlocality

    P. Lipka-Bartosik, A. F. Ducuara, T. Purves, and P. Skrzypczyk. “Op- erational significance of the quantum resource theory of buscemi nonlocality”. PRX Quantum2, 020301 (2021)

  13. [13]

    Ap- plication of the resource theory of channels to communication scenarios

    R. Takagi, K. Wang, and M. Hayashi. “Ap- plication of the resource theory of channels to communication scenarios”. Phys. Rev. Lett.124, 120502 (2020)

  14. [14]

    Convex resource theory of non-gaussianity

    R. Takagi and Q. Zhuang. “Convex resource theory of non-gaussianity”. Phys. Rev. A 97, 062337 (2018)

  15. [15]

    Resource engines

    H. Wojewódka-Ściążko, Z. Puchała, and K. Korzekwa. “Resource engines”. Quan- tum8, 1222 (2024)

  16. [16]

    General re- source theories in quantum mechanics and beyond: Operational characterization via discrimination tasks

    R. Takagi and B. Regula. “General re- source theories in quantum mechanics and beyond: Operational characterization via discrimination tasks”. Phys. Rev. X9, 031053 (2019)

  17. [17]

    Convex combinations of cp-divisible pauli channels that are not semigroups

    V. Jagadish, R. Srikanth, and F. Petruc- cione. “Convex combinations of cp-divisible pauli channels that are not semigroups”. Phys. Lett.A 384, 126907 (2020)

  18. [18]

    Colloquium: Non-markovian dynamics in open quantum systems

    H.-P. Breuer, E.-M. Laine, J. Piilo, and B. Vacchini. “Colloquium: Non-markovian dynamics in open quantum systems”. Rev. Mod. Phys.88, 021002 (2016)

  19. [19]

    Markovianity and non-markovianity in quantum and classical systems

    B. Vacchini, A. Smirne, E.-M. Laine, J. Pi- Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0.48 ilo, and H.-P. Breuer. “Markovianity and non-markovianity in quantum and classical systems”. New J. Phys.13, 093004 (2011)

  20. [20]

    Reconfigurable quan- tum local areanetwork over deployedfiber

    M. Alshowkan et al. “Reconfigurable quan- tum local areanetwork over deployedfiber”. PRX Quantum2, 040304 (2021)

  21. [21]

    Quantum internet: A vision for the road ahead

    S. Wehner, D. Elkouss, and R. Hanson. “Quantum internet: A vision for the road ahead”. Science362(2018)

  22. [23]

    Continuity of robustness measures in quantum resource theories

    J. Schluck, G. Murta, H. Kampermann, D. Bruß, and N. Wyderka. “Continuity of robustness measures in quantum resource theories”. J. Phys. A: Math. Theor. (2022)

  23. [24]

    Every quantum helps: Op- erational advantage of quantum resources beyond convexity

    K. Kuroiwa, R. Takagi, G. Adesso, and H. Yamasaki. “Every quantum helps: Op- erational advantage of quantum resources beyond convexity”. Phys. Rev. Lett.132, 150201 (2024)

  24. [25]

    Quantum-state texture and gate identification

    F. Parisio. “Quantum-state texture and gate identification”. Phys. Rev. Lett.133, 260801 (2024)

  25. [26]

    Nonlinear entanglement witnesses

    O. Gühne and N. Lütkenhaus. “Nonlinear entanglement witnesses”. Phys. Rev. Lett. 96, 170502 (2006)

  26. [27]

    Nonlinear improvement of qubit-qudit entanglement witnesses

    S.-Q. Shen, J.-M. Liang, M. Li, J. Yu, and S.-M. Fei. “Nonlinear improvement of qubit-qudit entanglement witnesses”. Phys. Rev. A101, 012312 (2020)

  27. [28]

    Measurement-device-independent nonlin- ear entanglement witnesses

    K. Sen, C. Srivastava, and U. Sen. “Measurement-device-independent nonlin- ear entanglement witnesses”. J. Phys. A56, 315301 (2023)

  28. [29]

    Semidefinite programs for completely bounded norms

    J. Watrous. “Semidefinite programs for completely bounded norms”. Theory Com- put.5, 217–238 (2009)

  29. [30]

    Pspace has constant-round quantum interactive proof systems

    J. Watrous. “Pspace has constant-round quantum interactive proof systems”. Theor. Comput. Sci.292, 575–588 (2003)

  30. [31]

    Distinguishing Short Quan- tum Computations

    B. Rosgen. “Distinguishing Short Quan- tum Computations”. In S. Albers and P. Weil, editors, 25th International Sym- posium on Theoretical Aspects of Com- puter Science. Volume 1 of Leibniz Interna- tional Proceedings in Informatics (LIPIcs), pages 597–608. Dagstuhl, Germany (2008). Schloss Dagstuhl–Leibniz-Zentrum fuer In- formatik

  31. [32]

    Completely positive linear maps on complex matrices

    M.-D. Choi. “Completely positive linear maps on complex matrices”. Linear Algebra and its Applications10, 285–290 (1975)

  32. [33]

    Linear transformations which preserve trace and positive semidefi- niteness of operators

    A. Jamiołkowski. “Linear transformations which preserve trace and positive semidefi- niteness of operators”. Reports on Mathe- matical Physics3, 275–278 (1972)

  33. [34]

    Topology

    J. Munkres. “Topology”. Prentice Hall. (2000). 2 edition. url: openli- brary.org/isbn/9780131816299

  34. [35]

    The fifty-nine icosahedra

    H. Coxeter, P. Du-Val, H. Flather, and J. Petrie. “The fifty-nine icosahedra”. University of Toronto Studies. Mathemat- ical Series. 6. University of Toronto Press. (1951)

  35. [36]

    Lurton,An Introduction to Underwater Acoustics: Principles and Applications, 2nd ed

    E. Moreale and M. Emmer. “Mathematics and culture i”. Mathematics and Cul- ture. Springer Berlin Heidelberg. (2003). url:link.springer.com/book/9783540017707

  36. [37]

    New trends in computer graph- ics: Proceedings of cg international ’88

    N. Magnenat-Thalmann and D. Thalmann, editors. “New trends in computer graph- ics: Proceedings of cg international ’88”. Springer. (2012)

  37. [38]

    Starshaped sets

    G. Hansen, I. Herburt, H. Martini, and M. Moszyńska. “Starshaped sets”. Aequa- tiones Mathematicae94(2020)

  38. [39]

    Com- putational geometry: An introduction

    F. P. Preparata and M. I. Shamos. “Com- putational geometry: An introduction”. Springer. (2012)

  39. [40]

    Existence of solutions and star-shapedness in minty variational inequalities

    G. P. Crespi, I. Ginchev, and M. Rocca. “Existence of solutions and star-shapedness in minty variational inequalities”. J. Glob. Optim.32, 485–494 (2005)

  40. [41]

    Lower convergence of minimal sets in star-shaped vector optimization prob- lems

    R. Hu. “Lower convergence of minimal sets in star-shaped vector optimization prob- lems”. J. Appl. Math.2014, 1–7 (2014)

  41. [42]

    A reverse isoperimetric in- equality for embedded starshaped plane curves

    J. Fang. “A reverse isoperimetric in- equality for embedded starshaped plane curves”. Archiv der Mathematik108, 621– 624 (2017)

  42. [43]

    Star-shaped space of solu- tions of the spherical negative perceptron

    B. L. Annesi, C. Lauditi, C. Lucibello, E. M. Malatesta, G. Perugini, F. Pittorino, and L. Saglietti. “Star-shaped space of solu- tions of the spherical negative perceptron”. Phys. Rev. Lett.131, 227301 (2023)

  43. [44]

    Theory of linear and integer programming

    A. Schrijver. “Theory of linear and integer programming”. Wiley. (1986). url: openli- brary.org/isbn/0471982326

  44. [45]

    Algebraic and geometric ideas in the theory of discrete optimization

    J. A. De Loera, R. Hemmecke, and M. Köppe. “Algebraic and geometric ideas in the theory of discrete optimization”. SIAM. (2012). Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0.49

  45. [46]

    Order-preserving functions: Ap- plications to majorization and order statis- tics

    A. W. Marshall, D. W. Walkup, and R. J.- B. Wets. “Order-preserving functions: Ap- plications to majorization and order statis- tics”. Pacific Journal of Mathematics23, 569–584 (1967)

  46. [47]

    Matching theory

    L. Lovász and M. D. Plummer. “Matching theory”. AMS Chelsea Publishing. Ameri- can Mathematical Society. (2009)

  47. [48]

    On closed star- shaped sets

    G. Hansen and H. Martini. “On closed star- shaped sets”. Journal of Convex Analysis 17, 659–671 (2010). url: www.heldermann- verlag.de/jca/jca17/jca0840_b.htm

  48. [49]

    Convex analysis

    R. T. Rockafellar. “Convex analysis”. Princeton University Press. (1970)

  49. [50]

    Quantum channels and rep- resentation theory

    W. G. Ritter. “Quantum channels and rep- resentation theory”. J. Math. Phys.46, 082103 (2005)

  50. [51]

    Bloch vectors for qudits

    R. A. Bertlmann and P. Krammer. “Bloch vectors for qudits”. J. Phys. A: Math. Theor.41, 235303 (2008)

  51. [52]

    Probabilistic theories with purification

    G. Chiribella, G. M. D’Ariano, and P. Perinotti. “Probabilistic theories with purification”. Phys. Rev. A81, 062348 (2010)

  52. [53]

    Universal structure of objective states in all fundamental causal theories

    C. M. Scandolo, R. Salazar, J. K. Korbicz, and P. Horodecki. “Universal structure of objective states in all fundamental causal theories”. Phys. Rev. Res.3, 033148 (2021)

  53. [54]

    The maximum numbers of faces of a convex polytope

    P. McMullen. “The maximum numbers of faces of a convex polytope”. Mathematika 17, 179–184 (1970)

  54. [55]

    Lectures on polytopes

    G. M. Ziegler. “Lectures on polytopes”. Vol- ume 152 of Graduate Texts in Mathemat- ics. Springer-Verlag. New York (1995)

  55. [56]

    Computational geome- try: Algorithms and applications

    M. de Berg, O. Cheong, M. van Kreveld, and M. Overmars. “Computational geome- try: Algorithms and applications”. Springer Berlin Heidelberg. (2008)

  56. [57]

    Computa- tional geometry: An introduction

    F. Preparata and M. Shamos. “Computa- tional geometry: An introduction”. Mono- graphs in Computer Science. Springer New York. (2012)

  57. [58]

    Surface recon- struction from unorganized points

    H. Hoppe, T. DeRose, T. Duchamp, J. Mc- Donald, and W. Stuetzle. “Surface recon- struction from unorganized points”. SIG- GRAPHComput.Graph.26, 71–78(1992)

  58. [59]

    General topology

    R. Engelking. “General topology”. Vol- ume 6 of Sigma Series in Pure Mathemat- ics. Heldermann Verlag. (1989). url: open- library.org/isbn/9783885380064

  59. [60]

    Real analysis: Modern techniques and their applications

    G. B. Folland. “Real analysis: Modern techniques and their applications”. Wi- ley. (1999). 2 edition. url: openli- brary.org/isbn/9780471317166

  60. [61]

    Operational advan- tage of quantum resources in subchannel discrimination

    R. Takagi, B. Regula, K. Bu, Z.-W. Liu, and G. Adesso. “Operational advan- tage of quantum resources in subchannel discrimination”. Phys. Rev. Lett.122, 140402 (2019)

  61. [62]

    Robustness- and weight- based resource measures without convexity restriction: Multicopy witness and opera- tional advantage in static and dynamical quantum resource theories

    K. Kuroiwa, R. Takagi, G. Adesso, and H. Yamasaki. “Robustness- and weight- based resource measures without convexity restriction: Multicopy witness and opera- tional advantage in static and dynamical quantum resource theories”. Phys. Rev. A 109, 042403 (2024)

  62. [63]

    All non-gaussian states are advantageous for channel discrimination: robustness of non- convex continuous variable quantum re- sources

    L. Turner, M. Guţă, and G. Adesso. “All non-gaussian states are advantageous for channel discrimination: robustness of non- convex continuous variable quantum re- sources”. New Journal of Physics27, 094507 (2025)

  63. [64]

    The knowledge complexity of interactive proof systems

    S. Goldwasser, S. Micali, and C. Rackoff. “The knowledge complexity of interactive proof systems”. SIAM Journal on Comput- ing18, 186–208 (1989)

  64. [65]

    Quantum circuit architec- ture

    G. Chiribella, G. M. D’Ariano, and P. Perinotti. “Quantum circuit architec- ture”. Phys. Rev. Lett.101, 060401 (2008)

  65. [66]

    Reversing un- known quantum transformations: Univer- sal quantum circuit for inverting general unitary operations

    M. T. Quintino, Q. Dong, A. Shimbo, A. Soeda, and M. Murao. “Reversing un- known quantum transformations: Univer- sal quantum circuit for inverting general unitary operations”. Phys. Rev. Lett.123, 210502 (2019)

  66. [67]

    Re- versing unknown qubit-unitary operation, deterministically and exactly

    S. Yoshida, A. Soeda, and M. Murao. “Re- versing unknown qubit-unitary operation, deterministically and exactly”. Phys. Rev. Lett.131, 120602 (2023)

  67. [68]

    Optimal quan- tum networks and one-shot entropies

    G. Chiribella and D. Ebler. “Optimal quan- tum networks and one-shot entropies”. New J. Phys.18, 093053 (2016)

  68. [69]

    Optimal quantum learning of a unitary transforma- tion

    A. Bisio, G. Chiribella, G. M. D’Ariano, S. Facchini, and P. Perinotti. “Optimal quantum learning of a unitary transforma- tion”. Phys. Rev. A81, 032324 (2010)

  69. [70]

    Op- timal probabilistic storage and retrieval of unitary channels

    M. Sedlák, A. Bisio, and M. Ziman. “Op- timal probabilistic storage and retrieval of unitary channels”. Phys. Rev. Lett.122, 170502 (2019)

  70. [71]

    Reversing unknown quantum processes Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0.50 via virtual combs for channels with lim- ited information

    C. Zhu, Y. Mo, Y.-A. Chen, and X. Wang. “Reversing unknown quantum processes Accepted in Quantum 2026-04-07, click title to verify. Published under CC-BY 4.0.50 via virtual combs for channels with lim- ited information”. Physical Review Let- ters133(2024)

  71. [72]

    Parameterized quan- tum comb and simpler circuits for revers- ing unknown qubit-unitary operations

    Y. Mo, L. Zhang, Y.-A. Chen, Y. Liu, T. Lin, and X. Wang. “Parameterized quan- tum comb and simpler circuits for revers- ing unknown qubit-unitary operations”. npj Quantum Information11(2025)

  72. [73]

    Coherence as a resource for Shor’s algorithm

    F. Ahnefeld, T. Theurer, D. Egloff, J. M. Matera, and M. B. Plenio. “Coherence as a resource for Shor’s algorithm”. Phys. Rev. Lett.129, 120501 (2022)

  73. [74]

    The first law of general quantum resource theories

    C. Sparaciari, L. del Rio, C. M. Scandolo, P. Faist, and J. Oppenheim. “The first law of general quantum resource theories”. Quantum4, 259 (2020)

  74. [75]

    Set coherence: Basis- independent quantification of quantum coherence

    S. Designolle, R. Uola, K. Luoma, and N. Brunner. “Set coherence: Basis- independent quantification of quantum coherence”. Phys. Rev. Lett.126, 220404 (2021)

  75. [76]

    Multiobject operational tasks for convex quantum resource theories of state-measurement pairs

    A. F. Ducuara, P. Lipka-Bartosik, and P. Skrzypczyk. “Multiobject operational tasks for convex quantum resource theories of state-measurement pairs”. Phys. Rev. Res.2, 033374 (2020)

  76. [77]

    Resource theory of absolute negativity

    R. Salazar, J. Czartowski, and A. de Oliveira Junior. “Resource theory of absolute negativity” (2022). arXiv:2205.13480

  77. [78]

    Introduction to the theory of cooperative games

    B. Peleg and P. Sudhölter. “Introduction to the theory of cooperative games”. The- ory and decision library. Kluwer Academic Publishers. (2003)

  78. [79]

    Cooperative game theory tools in coalitional control networks

    F. Muros. “Cooperative game theory tools in coalitional control networks”. Springer Theses. Springer International Publishing. (2019)

  79. [80]

    Game theory with ap- plications to economics

    J. W. Friedman. “Game theory with ap- plications to economics”. Oxford Uni- versity Press. (1990). 2 edition. url: search.worldcat.org/title/489629514

  80. [81]

    Cooperative game theory and applications: Cooperative games arising fromcombinatorialoptimizationproblems

    I. Curiel. “Cooperative game theory and applications: Cooperative games arising fromcombinatorialoptimizationproblems”. Theory and Decision Library C. Springer US. (1997)

Showing first 80 references.