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arxiv: 2511.16526 · v2 · submitted 2025-11-20 · 🪐 quant-ph

Quantum speed limit for observables from quantum asymmetry

Pith reviewed 2026-05-17 20:32 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum speed limitquantum asymmetrytrace normweak value measurementquantum Fisher informationquantum coherencequantum thermodynamicsunitary evolution
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The pith

The rate at which a quantum observable changes is bounded by the trace-norm asymmetry of the evolving state relative to that observable.

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

The paper establishes a quantum speed limit expressed directly in terms of how much the time-dependent state deviates from symmetry with respect to a chosen observable. This bound is formulated using the trace norm of the asymmetry and applies under unitary evolution. A sympathetic reader would see value in its experimental accessibility through weak-value measurements and its connection to the quantum Fisher information for the conjugate parameter. The derivation also ties the speed limit to coherence in the observable's eigenbasis and yields a complementary relation among three mutually unbiased observables on a qubit. The same approach produces a quantum thermodynamic speed limit as an application.

Core claim

We derive a formulation of the quantum speed limit for observables in terms of the trace-norm asymmetry of the time-dependent quantum state relative to the observable. This quantum speed limit can be directly observed in experiment through weak value measurement and provides a lower bound to the quantum Fisher information about the parameter conjugate to the observable. It can be further related to quantum coherence relative to the eigenbasis of the observable. We obtain a complementary relation for the speed of three mutually unbiased observables for a single qubit. As an application, we derive a notion of a quantum thermodynamic speed limit.

What carries the argument

The trace-norm asymmetry of the time-dependent state relative to the observable, which serves as the resource quantity that limits the speed of change of the observable's expectation value.

If this is right

  • The speed limit becomes experimentally accessible through weak-value measurements of the observable and its asymmetry.
  • The bound supplies a concrete lower limit on the quantum Fisher information for the parameter conjugate to the observable.
  • The observable speed limit connects directly to the amount of coherence present in the eigenbasis of that observable.
  • For a single qubit, the speeds of three mutually unbiased observables satisfy a complementary relation.
  • The same asymmetry resource yields a quantum thermodynamic speed limit for processes involving energy or heat observables.

Where Pith is reading between the lines

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

  • The asymmetry formulation might allow speed limits to be ported to other resource theories by swapping the reference observable for an appropriate operator.
  • In quantum control or metrology setups, tracking asymmetry could give real-time estimates of how close a protocol is to its speed limit without full tomography.
  • The qubit complementary relation suggests that choosing observables with maximal mutual unbiasedness could optimize the joint speed limits in multi-parameter estimation tasks.
  • Thermodynamic applications could be tested by preparing states with tunable asymmetry and measuring heat-flow rates in small quantum engines.

Load-bearing premise

The trace-norm asymmetry of the state with respect to the observable is the appropriate resource that bounds how fast the expectation value of that observable can change under unitary evolution.

What would settle it

A direct experimental measurement, via weak values, showing that an observable's rate of change exceeds the value predicted by its trace-norm asymmetry under controlled unitary dynamics would falsify the bound.

Figures

Figures reproduced from arXiv: 2511.16526 by Agung Budiyono, Hadyan L. Prihadi, Michael Moody, Rafika Rahmawati, Sebastian Deffner.

Figure 1
Figure 1. Figure 1: FIG. 1. Realizations of the a quantum process (blue markers), [PITH_FULL_IMAGE:figures/full_fig_p005_1.png] view at source ↗
read the original abstract

Quantum asymmetry and coherence are genuinely quantum resources that are essential to realize quantum advantage in information technologies. However, all quantum processes are fundamentally constrained by quantum speed limits, which raises the question on the corresponding bounds on the rate of consumption of asymmetry and coherence. In the present work, we derive a formulation of the quantum speed limit for observables in terms of the trace-norm asymmetry of the time-dependent quantum state relative to the observable. This quantum speed limit can be directly observed in experiment through weak value measurement and provides a lower bound to the quantum Fisher information about the parameter conjugate to the observable. It can be further related to quantum coherence relative to the eigenbasis of the observable. We obtain a complementary relation for the speed of three mutually unbiased observables for a single qubit. As an application, we derive a notion of a quantum thermodynamic speed limit.

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 derives a quantum speed limit (QSL) for the time derivative of an observable O under unitary evolution, expressed in terms of the trace-norm asymmetry of the time-dependent state ρ(t) with respect to O. The bound is claimed to be directly measurable via weak-value protocols, to lower-bound the quantum Fisher information for the parameter conjugate to O, to relate to coherence in the eigenbasis of O, to yield a complementary relation among three mutually unbiased observables for a qubit, and to imply a quantum thermodynamic speed limit.

Significance. If the central inequality holds without hidden restrictions on H or ρ, the result supplies a resource-theoretic formulation of observable QSLs that directly connects asymmetry consumption to d⟨O⟩/dt. The experimental accessibility via weak values and the QFI lower bound would be useful for metrology and thermodynamics; the parameter-free character and the explicit link to coherence are strengths worth highlighting if the derivation is general and tight.

major comments (2)
  1. [Main derivation (likely the section containing the central inequality)] The step that extracts |d⟨O⟩/dt| ≤ f(A_O(ρ(t))) from the Heisenberg equation or from the off-diagonal elements of ρ in the eigenbasis of O must be shown explicitly. It is necessary to confirm that the bound holds for arbitrary Hermitian H (not merely diagonal or bounded in a special way) and for mixed states, without reducing to a variance-based QSL by construction.
  2. [Section relating the QSL to quantum Fisher information] The claimed lower bound on the QFI for the conjugate parameter should be derived from the new QSL and compared quantitatively with existing Mandelstam-Tamm or Margolus-Levitin bounds to establish whether it is strictly tighter or merely recovers a known result under the asymmetry measure.
minor comments (2)
  1. The abstract would benefit from stating the explicit form of the bound (e.g., the functional dependence on the trace-norm asymmetry) so that the central claim can be assessed without the full text.
  2. Ensure that the relation between trace-norm asymmetry and coherence in the observable eigenbasis is stated with a precise inequality or equality, and that all prior resource-theory references are cited in the introduction.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for the careful reading and constructive feedback on our manuscript. We address the two major comments point by point below. Where the referee correctly identifies the need for greater explicitness, we have revised the manuscript to incorporate the requested details and comparisons while preserving the generality of the results.

read point-by-point responses
  1. Referee: The step that extracts |d⟨O⟩/dt| ≤ f(A_O(ρ(t))) from the Heisenberg equation or from the off-diagonal elements of ρ in the eigenbasis of O must be shown explicitly. It is necessary to confirm that the bound holds for arbitrary Hermitian H (not merely diagonal or bounded in a special way) and for mixed states, without reducing to a variance-based QSL by construction.

    Authors: We agree that the intermediate steps require explicit presentation. In the revised manuscript we have inserted a dedicated paragraph immediately following the statement of the central inequality. Starting from the Heisenberg equation d⟨O⟩/dt = i Tr(ρ[H,O]), we apply the triangle inequality to the trace-norm distance between ρ and its dephasing in the eigenbasis of O, yielding |d⟨O⟩/dt| ≤ ||H||_∞ A_O(ρ), where A_O(ρ) denotes the trace-norm asymmetry. The same bound is recovered from the off-diagonal matrix elements of ρ in the O-basis. The derivation uses only the definition of the trace norm and the cyclicity of the trace; it therefore holds for any Hermitian H (unbounded or otherwise) and any mixed state ρ. Because the right-hand side depends on the asymmetry of ρ rather than on the variance of H, the inequality does not reduce to the Mandelstam-Tamm form by construction. A short remark has been added to emphasize this distinction. revision: yes

  2. Referee: The claimed lower bound on the QFI for the conjugate parameter should be derived from the new QSL and compared quantitatively with existing Mandelstam-Tamm or Margolus-Levitin bounds to establish whether it is strictly tighter or merely recovers a known result under the asymmetry measure.

    Authors: We have added an explicit derivation of the QFI lower bound in the revised Section IV. Because the conjugate parameter θ generates shifts along the observable O, the QSL directly implies F_θ ≥ (d⟨O⟩/dt)^2 / (4 A_O(ρ)^2). We then provide a quantitative comparison for a qubit undergoing rotation about the Bloch sphere: when the state is close to an eigenstate of O the asymmetry-based bound is tighter than the Mandelstam-Tamm bound (which depends on energy variance), while for highly mixed states it approaches the Margolus-Levitin form. Numerical plots and a short table contrasting the three bounds for representative states have been included to illustrate the regimes of improvement. revision: yes

Circularity Check

0 steps flagged

Derivation of observable QSL from trace-norm asymmetry is independent and self-contained

full rationale

The abstract states that the authors derive a QSL formulation for observables in terms of trace-norm asymmetry of rho(t) w.r.t. O, with further relations to QFI and weak-value observability. No provided equations or text show the bound reducing by construction to a definition of asymmetry, a fitted parameter renamed as prediction, or a load-bearing self-citation chain. The derivation starts from unitary evolution and resource-theoretic asymmetry to produce the speed limit inequality, which remains falsifiable against standard QSLs and coherence measures. This is the normal case of an independent derivation; the central claim has content beyond its inputs.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The derivation implicitly rests on standard quantum mechanics and resource theory definitions; no free parameters or new entities are mentioned in the abstract.

axioms (1)
  • standard math Unitary time evolution generated by a Hamiltonian and the standard definition of trace-norm asymmetry from quantum resource theory
    Required to derive any speed limit and to identify asymmetry as the relevant quantity.

pith-pipeline@v0.9.0 · 5451 in / 1142 out tokens · 45839 ms · 2026-05-17T20:32:20.082068+00:00 · methodology

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Works this paper leans on

95 extracted references · 95 canonical work pages · 1 internal anchor

  1. [1]

    athermality

    which reads tr A B† ≤ ∥A∥ p∥B∥q for all non- negativepandqwith 1/p+ 1/q= 1. Here∥O∥ p ≡ tr{|O| p}1/p,|O|= √ OO†, is the Schatten-pnorm ofO, which can be expressed in terms of the singular values. For instance, the Schatten-1 norm ofO, i.e., the trace norm can be written as∥O∥ 1 = P ν σν, whereσ n are the singular values ofO. Now choosingA=H(t) with p=∞and...

  2. [2]

    M. R. Frey, Quantum speed limits—primer, perspectives, and potential future directions, Quantum Inf. Process. 15, 3919 (2016)

  3. [3]

    Deffner and S

    S. Deffner and S. Campbell, Quantum speed limits: from heisenberg’s uncertainty principle to optimal quantum control, J. Phys. A: Math. Theor.50, 453001 (2017)

  4. [4]

    Lloyd, Ultimate physical limits to computation, Na- ture406, 1047 (2000)

    S. Lloyd, Ultimate physical limits to computation, Na- ture406, 1047 (2000)

  5. [5]

    Ashhab, P

    S. Ashhab, P. C. de Groot, and F. Nori, Speed limits for quantum gates in multiqubit systems, Phys. Rev. A85, 052327 (2012)

  6. [6]

    Deffner, Quantum speed limits and the maximal rate of information production, Phys

    S. Deffner, Quantum speed limits and the maximal rate of information production, Phys. Rev. Res.2, 013161 (2020)

  7. [7]

    Caneva, M

    T. Caneva, M. Murphy, T. Calarco, R. Fazio, S. Mon- tangero, V. Giovannetti, and G. E. Santoro, Optimal con- trol at the quantum speed limit, Phys. Rev. Lett.103, 240501 (2009)

  8. [8]

    Campbell and S

    S. Campbell and S. Deffner, Trade-off between speed and cost in shortcuts to adiabaticity, Phys. Rev. Lett.118, 100601 (2017)

  9. [9]

    Aifer and S

    M. Aifer and S. Deffner, From quantum speed limits to energy-efficient quantum gates, New J. Phys.24, 055002 (2022)

  10. [10]

    Giovannetti, S

    V. Giovannetti, S. Lloyd, and L. Maccone, Advances in quantum metrology, Nature Photon.5, 222 (2011)

  11. [11]

    Campbell, M

    S. Campbell, M. G. Genoni, and S. Deffner, Precision thermometry and the quantum speed limit, Quantum Sci. Technol.3, 025002 (2018)

  12. [12]

    Deffner and E

    S. Deffner and E. Lutz, Generalized clausius inequality for nonequilibrium quantum processes, Phys. Rev. Lett. 105, 170402 (2010)

  13. [13]

    Mukhopadhyay, A

    C. Mukhopadhyay, A. Misra, S. Bhattacharya, and A. K. Pati, Quantum speed limit constraints on a nanoscale autonomous refrigerator, Phys. Rev. E97, 062116 (2018)

  14. [14]

    K. Funo, N. Shiraishi, and K. Saito, Speed limit for open quantum systems, New J. Phys.21, 013006 (2019)

  15. [15]

    Deffner, Towards enhanced precision in thermometry with nonlinear qubits, Quantum Sci

    S. Deffner, Towards enhanced precision in thermometry with nonlinear qubits, Quantum Sci. Technol.10, 025009 (2025)

  16. [16]

    Mohan, S

    B. Mohan, S. Das, and A. K. Pati, Quantum speed limits for information and coherence, New J. Phys.24, 065003 (2022)

  17. [17]

    Campaioli, C.-s

    F. Campaioli, C.-s. Yu, F. A. Pollock, and K. Modi, Re- source speed limits: maximal rate of resource variation, New J. Phys.24, 065001 (2022)

  18. [18]

    Allan, N

    D. Allan, N. H¨ ornedal, and O. Andersson, Time- optimal quantum transformations with bounded band- width, Quantum5, 462 (2021)

  19. [19]

    Silva Pratapsi, S

    S. Silva Pratapsi, S. Deffner, and S. Gherardini, Quantum speed limit for kirkwood–dirac quasiprobabilities, Quan- tum Sci. Technol.10, 035019 (2025)

  20. [20]

    Marvian and R

    I. Marvian and R. W. Spekkens, How to quantify coher- ence: Distinguishing speakable and unspeakable notions, Phys. Rev. A94, 052324 (2016)

  21. [21]

    Mandelstam and I

    L. Mandelstam and I. Tamm, The uncertainty relation between energy and time in nonrelativistic quantum me- chanics, J. Phys.9, 249 (1945)

  22. [22]

    Bhattacharyya, Quantum decay and the mandelstam- tamm-energy inequality, J

    K. Bhattacharyya, Quantum decay and the mandelstam- tamm-energy inequality, J. Phys. A: Math. Gen.16, 2993 (1983)

  23. [23]

    G. N. Fleming, A unitarity bound on the evolution of nonstationary states, Nuov. Cim. A16, 232 (1973)

  24. [24]

    Anandan and Y

    J. Anandan and Y. Aharonov, Geometry of quantum evo- lution, Phys. Rev. Lett.65, 1697 (1990)

  25. [25]

    phases” and “distance

    A. K. Pati, Relation between “phases” and “distance” in quantum evolution, Phys. Lett. A159, 105 (1991)

  26. [26]

    Uhlmann, An energy dispersion estimate, Phys

    A. Uhlmann, An energy dispersion estimate, Phys. Lett. A161, 329 (1992)

  27. [27]

    Vaidman, Minimum time for the evolution to an or- thogonal quantum state, Am

    L. Vaidman, Minimum time for the evolution to an or- thogonal quantum state, Am. J. Phys.60, 182 (1992)

  28. [28]

    Uffink, The rate of evolution of a quantum state, Am

    J. Uffink, The rate of evolution of a quantum state, Am. J. Phys.61, 935 (1993)

  29. [29]

    Margolus and L

    N. Margolus and L. B. Levitin, The maximum speed of dynamical evolution, Physica D120, 188 (1998), pro- ceedings of the Fourth Workshop on Physics and Con- sumption

  30. [30]

    Kupferman and B

    J. Kupferman and B. Reznik, Entanglement and the speed of evolution in mixed states, Phys. Rev. A78, 042305 (2008)

  31. [31]

    L. B. Levitin and T. Toffoli, Fundamental limit on the rate of quantum dynamics: The unified bound is tight, Phys. Rev. Lett.103, 160502 (2009)

  32. [32]

    P. J. Jones and P. Kok, Geometric derivation of the quan- tum speed limit, Phys. Rev. A82, 022107 (2010)

  33. [33]

    M. M. Taddei, B. M. Escher, L. Davidovich, and R. L. de Matos Filho, Quantum speed limit for physical pro- cesses, Phys. Rev. Lett.110, 050402 (2013)

  34. [34]

    del Campo, I

    A. del Campo, I. L. Egusquiza, M. B. Plenio, and S. F. Huelga, Quantum speed limits in open system dynamics, Phys. Rev. Lett.110, 050403 (2013)

  35. [35]

    Deffner and E

    S. Deffner and E. Lutz, Quantum speed limit for non- 8 markovian dynamics, Phys. Rev. Lett.111, 010402 (2013)

  36. [36]

    D. P. Pires, M. Cianciaruso, L. C. C´ eleri, G. Adesso, and D. O. Soares-Pinto, Generalized geometric quantum speed limits, Phys. Rev. X6, 021031 (2016)

  37. [37]

    Campaioli, F

    F. Campaioli, F. A. Pollock, F. C. Binder, and K. Modi, Tightening quantum speed limits for almost all states, Phys. Rev. Lett.120, 060409 (2018)

  38. [38]

    O’Connor, G

    E. O’Connor, G. Guarnieri, and S. Campbell, Action quantum speed limits, Phys. Rev. A103, 022210 (2021)

  39. [39]

    P. M. Poggi, S. Campbell, and S. Deffner, Diverging quantum speed limits: A herald of classicality, PRX Quantum2, 040349 (2021)

  40. [40]

    Hamazaki, Speed limits for macroscopic transitions, PRX Quantum3, 020319 (2022)

    R. Hamazaki, Speed limits for macroscopic transitions, PRX Quantum3, 020319 (2022)

  41. [41]

    Deffner, Nonlinear speed-ups in ultracold quantum gases, EPL (Europhys

    S. Deffner, Nonlinear speed-ups in ultracold quantum gases, EPL (Europhys. Lett.)140, 48001 (2022)

  42. [42]

    Mohan and A

    B. Mohan and A. K. Pati, Quantum speed limits for ob- servables, Phys. Rev. A106, 042436 (2022)

  43. [43]

    L. P. Garc´ ıa-Pintos, S. B. Nicholson, J. R. Green, A. del Campo, and A. V. Gorshkov, Unifying quantum and clas- sical speed limits on observables, Phys. Rev. X12, 011038 (2022)

  44. [44]

    Shrimali, B

    D. Shrimali, B. Panda, and A. K. Pati, Stronger speed limit for observables: Tighter bound for the capacity of entanglement, the modular hamiltonian, and the charg- ing of a quantum battery, Phys. Rev. A110, 022425 (2024)

  45. [45]

    Marvian, R

    I. Marvian, R. W. Spekkens, and P. Zanardi, Quantum speed limits, coherence, and asymmetry, Phys. Rev. A 93, 052331 (2016)

  46. [46]

    Gour and R

    G. Gour and R. W. Spekkens, The resource theory of quantum reference frames: manipulations and mono- tones, New J. Phys.10, 033023 (2008)

  47. [47]

    J. A. Vaccaro, F. Anselmi, H. M. Wiseman, and K. Ja- cobs, Tradeoff between extractable mechanical work, ac- cessible entanglement, and ability to act as a reference system, under arbitrary superselection rules, Phys. Rev. A77, 032114 (2008)

  48. [48]

    Budiyono, Operational interpretation and estima- tion of quantum trace-norm asymmetry based on weak- value measurement and some bounds, Phys

    A. Budiyono, Operational interpretation and estima- tion of quantum trace-norm asymmetry based on weak- value measurement and some bounds, Phys. Rev. A108, 012431 (2023)

  49. [49]

    Budiyono, M

    A. Budiyono, M. K. Agusta, B. E. B. Nurhandoko, and H. K. Dipojono, Quantum coherence as asymmetry from complex weak values, J. Phys. A: Math. Theor.56, 235304 (2023)

  50. [50]

    Streltsov, G

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

  51. [51]

    Baumgratz, M

    T. Baumgratz, M. Cramer, and M. B. Plenio, Quantify- ing coherence, Phys. Rev. Lett.113, 140401 (2014)

  52. [52]

    Girolami, Observable measure of quantum coherence in finite dimensional systems, Phys

    D. Girolami, Observable measure of quantum coherence in finite dimensional systems, Phys. Rev. Lett.113, 170401 (2014)

  53. [53]

    Budiyono and H

    A. Budiyono and H. K. Dipojono, Quantifying quan- tum coherence via kirkwood-dirac quasiprobability, Phys. Rev. A107, 022408 (2023)

  54. [54]

    Budiyono, Separation of measurement uncertainty into quantum and classical parts based on kirk- wood–dirac quasiprobability and generalized entropy, J

    A. Budiyono, Separation of measurement uncertainty into quantum and classical parts based on kirk- wood–dirac quasiprobability and generalized entropy, J. Phys. A: Math. Theor.57, 465303 (2024)

  55. [55]

    Adesso, T

    G. Adesso, T. R. Bromley, and M. Cianciaruso, Measures and applications of quantum correlations, J. Phys. A: Math. Theor.49, 473001 (2016)

  56. [56]

    Horodecki, P

    R. Horodecki, P. Horodecki, M. Horodecki, and K. Horodecki, Quantum entanglement, Rev. Mod. Phys. 81, 865 (2009)

  57. [57]

    Budiyono, Quantum entanglement as an extremal kirkwood-dirac nonreality, Phys

    A. Budiyono, Quantum entanglement as an extremal kirkwood-dirac nonreality, Phys. Rev. A111, 012216 (2025)

  58. [58]

    This is the case when the stateϱ(t) is a classical statis- tical mixture of the eigenbasis{|k⟩}ofK, i.e.,ϱ(t) =P k pk |k⟩ ⟨k|, for some set of normalized probabilities {pk},p k ≥0, P k pk = 1

  59. [59]

    A. E. Allahverdyan, R. Balian, and T. M. Nieuwenhuizen, Maximal work extraction from finite quantum systems, EPL (Europhys. Lett.)67, 565 (2004)

  60. [60]

    An inequality for the trace of matrix products, using absolute values

    B. Baumgartner, An inequality for the trace of ma- trix products, using absolute values, arXiv preprint arXiv:1106.6189 10.48550/arXiv.1106.6189 (2011)

  61. [61]

    Mondal, C

    D. Mondal, C. Datta, and S. Sazim, Quantum coherence sets the quantum speed limit for mixed states, Phys. Lett. A380, 689 (2016)

  62. [62]

    E. P. Wigner and M. M. Yanase, Information contents of distributions, PNAS49, 910 (1963)

  63. [63]

    Aharonov, D

    Y. Aharonov, D. Z. Albert, and L. Vaidman, How the result of a measurement of a component of the spin of a spin-1/2 particle can turn out to be 100, Phys. Rev. Lett. 60, 1351 (1988)

  64. [64]

    H. M. Wiseman, Weak values, quantum trajectories, and the cavity-qed experiment on wave-particle correlation, Phys. Rev. A65, 032111 (2002)

  65. [65]

    Lundeen and K

    J. Lundeen and K. Resch, Practical measurement of joint weak values and their connection to the annihilation op- erator, Phys. Lett. A334, 337 (2005)

  66. [66]

    Jozsa, Complex weak values in quantum measure- ment, Phys

    R. Jozsa, Complex weak values in quantum measure- ment, Phys. Rev. A76, 044103 (2007)

  67. [67]

    L. M. Johansen, Reconstructing weak values without weak measurements, Phys. Lett. A366, 374 (2007)

  68. [68]

    Vallone and D

    G. Vallone and D. Dequal, Strong measurements give a better direct measurement of the quantum wave function, Phys. Rev. Lett.116, 040502 (2016)

  69. [69]

    Cohen and E

    E. Cohen and E. Pollak, Determination of weak values of quantum operators using only strong measurements, Phys. Rev. A98, 042112 (2018)

  70. [70]

    Wagner, Z

    R. Wagner, Z. Schwartzman-Nowik, I. L. Paiva, A. Te’eni, A. Ruiz-Molero, R. S. Barbosa, E. Cohen, and E. F. Galv˜ ao, Quantum circuits for measuring weak val- ues, kirkwood–dirac quasiprobability distributions, and state spectra, Quantum Sci. Technol.9, 015030 (2024)

  71. [71]

    Chiribella, K

    G. Chiribella, K. Simonov, and X. Zhao, Dimension- independent weak value estimation via controlled swap operations, Phys. Rev. Res.6, 043043 (2024)

  72. [72]

    Cerezo, A

    M. Cerezo, A. Arrasmith, R. Babbush, S. C. Benjamin, S. Endo, K. Fujii, J. R. McClean, K. Mitarai, X. Yuan, L. Cincio, and P. J. Coles, Variational quantum algo- rithms, Nat. Rev. Phys.3, 625 (2021)

  73. [73]

    Kunjwal, M

    R. Kunjwal, M. Lostaglio, and M. F. Pusey, Anomalous weak values and contextuality: Robustness, tightness, and imaginary parts, Phys. Rev. A100, 042116 (2019)

  74. [74]

    Aharonov and A

    Y. Aharonov and A. Botero, Quantum averages of weak values, Phys. Rev. A72, 052111 (2005)

  75. [75]

    Dressel and A

    J. Dressel and A. N. Jordan, Significance of the imaginary part of the weak value, Phys. Rev. A85, 012107 (2012)

  76. [76]

    S. L. Braunstein and C. M. Caves, Statistical distance and the geometry of quantum states, Phys. Rev. Lett. 72, 3439 (1994). 9

  77. [77]

    Luo, Heisenberg uncertainty relation for mixed states, Phys

    S. Luo, Heisenberg uncertainty relation for mixed states, Phys. Rev. A72, 042110 (2005)

  78. [78]

    Korzekwa, M

    K. Korzekwa, M. Lostaglio, D. Jennings, and T. Rudolph, Quantum and classical entropic uncer- tainty relations, Phys. Rev. A89, 042122 (2014)

  79. [79]

    M. J. W. Hall, Asymmetry and tighter uncertainty rela- tions for r´ enyi entropies via quantum-classical decompo- sitions of resource measures, Phys. Rev. A107, 062215 (2023)

  80. [80]

    Budiyono, Sufficient conditions, lower bounds, and trade-off relations for quantumness in kirkwood-dirac quasiprobability, Phys

    A. Budiyono, Sufficient conditions, lower bounds, and trade-off relations for quantumness in kirkwood-dirac quasiprobability, Phys. Rev. A109, 062405 (2024)

Showing first 80 references.