REVIEW 2 major objections 5 minor 64 references
Improving quantum channel discrimination with resourceful states
T0 review · 2 major / 5 minor · reviewed 2026-08-10 · deepseek-v4-flash
Pith's one-line read In any resource theory of quantum states, the generalized robustness of a state is exactly the maximum factor by which it improves one-shot quantum channel discrimination over the best free state.
desk verdict The main equality G=1+R is correct and significant, but the bound-resource characterization in Section III is wrong for non-closed free sets and the abstract overclaims as a result. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is the generalized robustness $R_F(\rho)=\min\{\lambda\ge 0:(\rho+\lambda\tau)/(1+\lambda)\in F,\ \tau\in\mathrm{Den}_A\}$, together with its Lagrange dual $R_F(\rho)=\max\{\operatorname{Tr}(x\rho)-1: x\ge 0,\ \operatorname{Tr}(x\omega)\le 1\ \forall\omega\in F\}$. The lower-bound direction uses the dual optimizer $x^\star$ to define an effect $e=x^\star/\|x^\star\|_\infty$ and a family of group-covariant channels built from generalized Pauli-$X$ shifts; a symmetrization step ensures the success-probability ratio for this family collapses to $\operatorname{Tr}(e\rho)/\sup_{\omega\in F}\operatorname{Tr}(e\omega)$, which is at least $1+R_F(\rho)$ by duality. The auxiliary-system extension replaces the simple measurement by a maximally entangled state and a decomposition into subchannels, with the free-set condition guaranteeing that local operations on the auxiliary system keep free states free.
What would settle it
Compute $R_F(\rho)$ for a small finite-dimensional convex free set and state by solving the dual program, construct the paper's channel ensemble from the optimizer, and check the measured success-probability ratio; a ratio strictly larger than $1+R_F(\rho)$ would refute Theorem 1, while the theorem predicts the constructed ensemble reaches the bound.
Extended reading notes
Core claim
On the paper's own terms, the central discovery is an identity: the discrimination power $G(\rho,F)=\sup_{\{p_n,\Lambda_n\}}P_S(\rho;\{p_n,\Lambda_n\})/\sup_{\omega\in F}P_S(\omega;\{p_n,\Lambda_n\})$ satisfies $G(\rho,F)=1+R_F(\rho)$ for every convex free-state set $F$, and $G(\rho,F)=1+R_{\operatorname{co}F}(\rho)$ for every set $F$. When an auxiliary system $C$ is used, the statement becomes $G_C(\rho,F)=1+R_{\operatorname{co}F_C}(\rho)$, where $F_C$ is the set obtained from $F$ by applying arbitrary local channels on $C$. The proof constructs explicit channel ensembles from the optimizer of a dual convex program, showing the bound is attainable, and it identifies the states that give no discrimination advantage, the bound resource states, as precisely the states in the convex hull of the free set.
Load-bearing premise
The load-bearing premise is the standard strong-duality fact that the convex program defining generalized robustness attains its optimum for every closed convex free set containing a full-rank state, because the explicit channel ensemble is built from that optimizer; the auxiliary-system version also assumes the free set is preserved by local operations on the ancilla, or else the statement is read with the enlarged set $F_C$.
Editorial extensions
If this is right
- In every convex resource theory, the generalized robustness is not merely a mathematical quantifier: it is the exact factor by which a resourceful state can outperform all free states in a one-shot channel-discrimination test.
- A non-free state is useless for one-shot channel discrimination exactly when it lies in the convex hull of the free set; if the free set is convex and closed, every resource state is useful in some discrimination task.
- Allowing an auxiliary system does not escape the robustness bound: the ancilla-assisted discrimination power is still $1+$ robustness, now computed against $\operatorname{co}F_C$, so ancillas enlarge the relevant free hull rather than bypass the formula.
- Because robustness is the optimal value of a convex program, the discrimination power can be obtained by standard convex-optimization methods in any finite-dimensional resource theory, not only in the special theories previously solved.
- The equality $G_C(\rho,F)=G(\rho,F_C)$ gives a criterion for when ancillas help: the ancilla-assisted and bare discrimination powers coincide for every state exactly when $\operatorname{co}F=\operatorname{co}F_C$.
Reading between the lines
- An extension the paper leaves implicit is the multi-shot or adaptive setting: the proof here is one-shot, and a natural conjecture, which is my inference rather than the paper's, is that the corresponding long-run advantage would be governed by a regularized robustness.
- The explicit dual-optimizer construction suggests an experimental recipe for saturating the bound with a finite channel ensemble whose size is set by the spectral norm of the optimizer; the paper does not spell this out.
- For nonconvex resource theories, the theorem says that only the convex hull of the free set matters for this task, which implies that 'bound' resources in any such theory are exactly the states inside that hull; testing this against particular nonconvex resources such as magic or imaginarity would be a further application beyond the paper's own case studies.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper studies single-shot quantum channel discrimination and asks how much the maximum average success probability can be improved by using a resource state ρ instead of the best free state. The main quantity is the discrimination power G(ρ,F), defined as the supremum over channel discrimination ensembles of the ratio between the success probability with ρ and that with the best free state. Theorem 1 states that for any convex free set F, G(ρ,F)=1+R_F(ρ), where R_F is the generalized robustness. Corollary 2 extends this to arbitrary (possibly nonconvex) F via G(ρ,F)=G(ρ,coF)=1+R_coF(ρ). Theorem 3 extends the equality to protocols with an auxiliary system C when the free set preserves operations on C, and Corollary 4 gives the general auxiliary-system formula GC(ρ,F)=1+R_coFC(ρ). The paper also characterizes 'bound resource states' (resource states with G=1) and discusses the difference between G and the previously studied quantity H defined in Eq. (8). The proofs are detailed and mostly self-contained, with appendices covering group-covariant measurements, the auxiliary-system construction, and degeneracies when no positive-definite free state exists.
Significance. If the central equalities hold, the paper resolves a natural open question from Ref. [41] by giving the generalized robustness an exact operational meaning as the maximum attainable advantage in one-shot channel discrimination, both with and without auxiliary systems. This is a clean and broadly applicable result: it unifies earlier special-case results for entanglement, coherence, asymmetry, and steering, and it provides a concrete recipe for constructing discrimination ensembles that achieve the bound. The auxiliary-system result is particularly valuable because such exact quantifications were previously known only in special cases. The paper also usefully clarifies the distinction between the discrimination power G and the earlier measure H. The mathematical core of Theorems 1 and 3 appears sound and the proofs are carefully structured. However, the paper's advertised 'full characterization' of resource states is stated too broadly: the bound-resource-state characterization in Section III is false for non-closed free sets, and this needs correction before the paper can be accepted.
major comments (2)
- [Section III, paragraph after Corollary 2] The statement 'ρ ∉ F being a bound resource state is equivalent to ρ ∈ co F' is false when co F is not closed. Counterexample: let F be the qubit state space minus the pure state |0⟩⟨0|. This F is convex, contains positive-definite states, and satisfies co F = F. For ρ = |0⟩⟨0| we have ρ ∉ F and ρ ∉ co F. However, for every λ > 0 the state (ρ + λ|1⟩⟨1|)/(1+λ) is a non-extreme mixed state lying in F, so R_coF(ρ) = 0. Corollary 2 then gives G(ρ,F) = 1, making ρ a bound resource state by the paper's own definition, even though ρ ∉ co F. The correct equivalence is ρ ∈ cl(co F) \ F. This error propagates to the abstract's claim that 'resources can be fully characterized' for arbitrary (possibly non-closed) free sets and to Figure 1, whose gray areas should be cl(co F) \ F and cl(co FC) \ F rather than co F \ F and co FC \ F. The main equalities of Theorem 1 and Corollary 2 are not affected, but the characterization claim needs to be revised.
- [Abstract and Section III, bound-state characterization] The paper claims that 'there are no bound resource states if and only if F is convex and closed.' This biconditional is in fact correct, but the reasoning given in Section III is incomplete: the proof uses the erroneous equivalence ρ ∈ co F instead of ρ ∈ cl(co F). Since the 'if' direction is immediate and the 'only if' direction follows from R_coF(ρ) = 0 iff ρ ∈ cl(co F), the statement should be derived from the closure-corrected characterization. The current text, as written, gives a false intermediate statement that could mislead readers about the role of topological closure in nonconvex resource theories.
minor comments (5)
- [Theorem 1 proof, Eq. (5)] The proof assumes the existence of an optimal solution x⋆ of the dual problem (5) and uses the equality Tr(x⋆ρ) = 1 + R_F(ρ). This is a standard strong-duality result for closed convex F containing a positive-definite state, but it is cited from Ref. [49] rather than proved. Since the proof has already reduced to closed F, a brief explicit statement that Slater's condition guarantees attainment would make the argument self-contained at this point.
- [Theorem 1 proof, first paragraph] The identities G(ρ,F) = G(ρ,cl F) and R_F(ρ) = R_clF(ρ) are asserted without proof. They are true because the success probability and the feasibility condition in Eq. (3) are continuous in the state, but a one-sentence justification would improve readability.
- [Theorem 3 and Appendix C, notation] The symbol C is used both for the auxiliary system in the discrimination problem and for the output system of the subchannels Λ̃_n in Lemma 6 and Lemma 7. This overloading makes the proof of Theorem 3 significantly harder to follow; renaming one of the two systems (e.g., calling the channel output system D) would clarify the construction.
- [Eq. (7) and Lemma 6] The channels in Eq. (7) and the subchannels in Lemma 6 involve denominators N−1. The proof chooses N large enough (N ≥ 2), but this is not stated explicitly at the point of definition; adding 'with N ≥ 2' would avoid a momentary division-by-zero concern.
- [Appendix B, Lemma 5] In the proof that Π^sym is a measurement, the line 'U_h(I_NB) = I_NB' appears after summing over g; the text is correct but could be compressed. More importantly, the equality PS(σ,Π;·) = PS(σ,Π^sym;·) is derived for equal priors, which is used later; this restriction should be mentioned in the lemma statement for clarity.
Circularity Check
No significant circularity: G and robustness are independently defined, and the lower-bound proof explicitly constructs channels from the dual optimizer rather than assuming the equality.
full rationale
The central claims are self-contained in the relevant sense. The discrimination power G(rho,F) in Eq. (2) and the robustness R_F(rho) in Eq. (3) are defined independently, and Theorem 1 proves equality in both directions. The upper bound uses only the defining mixture property of R_F. The lower bound takes the dual optimizer x* of the standard robustness optimization problem in Eq. (5) and explicitly constructs a covariant collection of channels in Eq. (7) for which the success-probability ratio reaches Tr(x*rho), so the equality is not assumed by construction. No free parameter is fitted to the predicted quantity, and no prediction is renamed as a definition. The only imported mathematical ingredient is the Lagrange-dual characterization of R_F, cited as an external, standard convex-optimization fact from Ref. [49]; that reference is not authored by this paper's author and does not itself contain the target equality. The same dual characterization, together with explicit subchannel constructions, is used for the auxiliary-system extension in Theorem 3 and Corollary 4. The single self-citation, Ref. [14], concerns a different upper/lower bound result and is not load-bearing for the present theorems. There is a separate correctness concern that the Section III claim identifying bound resource states with membership in coF is false for non-closed free sets, since a state can have zero robustness without lying in coF; that is a mathematical caveat, not a circularity, and does not affect the circularity score.
Assumptions & free parameters
assumptions (3)
- domain assumption Finite-dimensional Hilbert spaces for all systems A, B, and C.
- standard math Strong duality holds between the robustness primal problem in Eq. (3) and its Lagrange dual in Eq. (5).
- domain assumption F contains at least one positive definite matrix, or the general case is handled through convex hulls as in Appendix D.
Cite this review
Pith. "Pith review of Improving quantum channel discrimination with resourceful states." pith.science (2026). https://pith.science/paper/EGIXBM5P
@misc{pith2026250109205,
author = {Pith},
title = {Pith review of: Improving quantum channel discrimination with resourceful states},
year = {2026},
howpublished = {\url{https://pith.science/paper/EGIXBM5P}},
note = {Machine review of arXiv:2501.09205}
}
read the original abstract
One of the key issues in quantum discrimination problems is understanding the extent of the advantages in discrimination performance when using resource states compared to resourceless states. We show that in any resource theory of states, which may not be convex, the extent to which the maximum average success probability can be improved in quantum channel discrimination problems without using auxiliary systems can be precisely quantified by the robustness measure. This result offers an intuitive operational meaning of the robustness measure in any convex resource theory. Furthermore, we demonstrate that the robustness measure can also quantify the improvement in channel discrimination problems that use auxiliary systems. Using these findings, resources can be fully characterized to achieve higher success probabilities than any state without the given resource in channel discrimination problems.
Figures
Reference graph
Works this paper leans on
-
[49]
R. Takagi and B. Regula, General resource theories in quan- tum mechanics and beyond: operational characterization via discrimination tasks, Phys. Rev. X 9, 031053 (2019)
work page 2019
-
[51]
Regula, Convex geometry of quantum resource quantifica- tion, J
B. Regula, Convex geometry of quantum resource quantifica- tion, J. Phys. A: Math. Theor. 51, 045303 (2017)
work page 2017
-
[41]
Takagi, K
R. Takagi, K. Wang, and M. Hayashi, Application of the re- source theory of channels to communication scenarios, Phys. Rev. Lett. 124, 120502 (2020)
2020
-
[1]
Assume that F is not empty so that G(ρ, F) and RF(ρ) are well-defined for at least one state ρ∈ DenA
Without considering auxiliary systems Let us consider the set of free statesF of an arbitrary system A. Assume that F is not empty so that G(ρ, F) and RF(ρ) are well-defined for at least one state ρ∈ DenA. For any subset T of DenA, let S T be the set of all ρ∈ DenA such that there existsω∈ T and a positive real number c satisfying cρ≤ ω. S T = DenA is equ...
-
[2]
Assume that F is not empty; then, the following corollary holds
Considering auxiliary systems For any two systems A and C, let us consider the set of free states F of the composite system A⊗ C. Assume that F is not empty; then, the following corollary holds. Corollary 9 For any ρ ∈ DenA⊗C, (1) ρ ∈ S co FC, (2) Rco FC(ρ)<∞, and (3) GC(ρ, FC)<∞ are all equivalent. Proof Substituting FC for F in Lemma 8 gives (1)⇔ (2). I...
-
[3]
Gisin and R
N. Gisin and R. Thew, Quantum communication, Nat. Photon- ics 1, 165 (2007)
2007
-
[4]
C. L. Degen, F. Reinhard, and P. Cappellaro, Quantum sensing, Rev. Mod. Phys. 89, 035002 (2017)
2017
-
[5]
Gisin, G
N. Gisin, G. Ribordy, W. Tittel, and H. Zbinden, Quantum cryp- tography, Rev. Mod. Phys.74, 145 (2002)
2002
Show all 64 references
-
[6]
Acin, Statistical distinguishability between unitary opera- tions, Phys
A. Acin, Statistical distinguishability between unitary opera- tions, Phys. Rev. Lett. 87, 177901 (2001)
2001
-
[7]
M. F. Sacchi, Optimal discrimination of quantum operations, Phys. Rev. A 71, 062340 (2005)
2005
-
[8]
M. F. Sacchi, Entanglement can enhance the distinguishability of entanglement-breaking channels, Phys. Rev. A 72, 014305 (2005)
2005
-
[9]
Li and D
L. Li and D. Qiu, Optimal discrimination between quantum op- erations, J. Phys. A: Math. Theor. 41, 335302 (2008)
2008
-
[10]
Matthews, M
W. Matthews, M. Piani, and J. Watrous, Entanglement in chan- nel discrimination with restricted measurements, Phys. Rev. A 82, 032302 (2010)
2010
-
[11]
Chiribella, Optimal networks for quantum metrology: semidefinite programs and product rules, New J
G. Chiribella, Optimal networks for quantum metrology: semidefinite programs and product rules, New J. Phys. 14, 125008 (2012)
2012
-
[12]
Sedl ´ak and M
M. Sedl ´ak and M. Ziman, Optimal single-shot strategies for discrimination of quantum measurements, Phys. Rev. A 90, 052312 (2014)
2014
-
[13]
Pirandola and C
S. Pirandola and C. Lupo, Ultimate precision of adaptive noise estimation, Phys. Rev. Lett. 118, 100502 (2017)
2017
-
[14]
Puchała, Ł
Z. Puchała, Ł. Pawela, A. Krawiec, and R. Kukulski, Strate- gies for optimal single-shot discrimination of quantum mea- surements, Phys. Rev. A 98, 042103 (2018)
2018
-
[15]
Pirandola, R
S. Pirandola, R. Laurenza, C. Lupo, and J. L. Pereira, Funda- mental limits to quantum channel discrimination, npj Quantum Inf. 5, 50 (2019)
2019
-
[16]
Nakahira and K
K. Nakahira and K. Kato, Simple upper and lower bounds on the ultimate success probability for discriminating arbitrary finite-dimensional quantum processes, Phys. Rev. Lett. 126, 200502 (2021)
2021
-
[17]
Piani and J
M. Piani and J. Watrous, All entangled states are useful for channel discrimination, Phys. Rev. Lett. 102, 250501 (2009)
2009
-
[18]
Baumgratz, M
T. Baumgratz, M. Cramer, and M. B. Plenio, Quantifying co- herence, Phys. Rev. Lett. 113, 140401 (2014)
2014
-
[19]
Winter and D
A. Winter and D. Yang, Operational resource theory of coher- ence, Phys. Rev. Lett. 116, 120404 (2016)
2016
-
[20]
Streltsov, G
A. Streltsov, G. Adesso, and M. B. Plenio, Colloquium: Quan- tum coherence as a resource, Rev. Mod. Phys. 89, 041003 (2017)
2017
-
[21]
Theurer, N
T. Theurer, N. Killoran, D. Eglo ff, and M. B. Plenio, Resource theory of superposition, Phys. Rev. Lett. 119, 230401 (2017)
2017
-
[22]
Gour and R
G. Gour and R. W. Spekkens, The resource theory of quantum reference frames: manipulations and monotones, New J. Phys. 10, 033023 (2008). 12
2008
-
[23]
Marvian and R
I. Marvian and R. W. Spekkens, How to quantify coherence: Distinguishing speakable and unspeakable notions, Phys. Rev. A 94, 052324 (2016)
2016
-
[24]
Veitch, S
V . Veitch, S. H. Mousavian, D. Gottesman, and J. Emerson, The resource theory of stabilizer quantum computation, New J. Phys. 16, 013009 (2014)
2014
-
[25]
Howard and E
M. Howard and E. Campbell, Application of a resource the- ory for magic states to fault-tolerant quantum computing, Phys. Rev. Lett. 118, 090501 (2017)
2017
-
[26]
M. G. Genoni, M. G. Paris, and K. Banaszek, Quantifying the non-gaussian character of a quantum state by quantum relative entropy, Phys. Rev. A78, 060303 (2008)
2008
-
[27]
Takagi and Q
R. Takagi and Q. Zhuang, Convex resource theory of non- gaussianity, Phys. Rev. A97, 062337 (2018)
2018
-
[28]
Albarelli, M
F. Albarelli, M. G. Genoni, M. G. Paris, and A. Ferraro, Re- source theory of quantum non-gaussianity and wigner negativ- ity, Phys. Rev. A98, 052350 (2018)
2018
-
[29]
Wakakuwa, Operational resource theory of non- markovianity, arXiv preprint arXiv:1709.07248 (2017)
E. Wakakuwa, Operational resource theory of non- markovianity, arXiv preprint arXiv:1709.07248 (2017)
2017 arXiv
-
[30]
Bhattacharya, B
S. Bhattacharya, B. Bhattacharya, and A. S. Majumdar, Convex resource theory of non-markovianity, J. Phys. A: Math. Theor. 54, 035302 (2020)
2020
-
[31]
F. G. Brandao, M. Horodecki, J. Oppenheim, J. M. Renes, and R. W. Spekkens, Resource theory of quantum states out of ther- mal equilibrium, Phys. Rev. Lett. 111, 250404 (2013)
2013
-
[32]
G. Gour, M. P. M ¨uller, V . Narasimhachar, R. W. Spekkens, and N. Y . Halpern, The resource theory of informational nonequi- librium in thermodynamics, Phys. Rep. 583, 1 (2015)
2015
-
[33]
K.-D. Wu, T. V . Kondra, S. Rana, C. M. Scandolo, G.-Y . Xiang, C.-F. Li, G.-C. Guo, and A. Streltsov, Operational resource the- ory of imaginarity, Phys. Rev. Lett.126, 090401 (2021)
2021
-
[34]
S. Xue, J. Guo, P. Li, M. Ye, and Y . Li, Quantification of re- source theory of imaginarity, Quant. Inf. Proc. 20, 1 (2021)
2021
-
[35]
Carmeli, T
C. Carmeli, T. Heinosaari, and A. Toigo, State discrimina- tion with postmeasurement information and incompatibility of quantum measurements, Phys. Rev. A 98, 012126 (2018)
2018
-
[36]
Carmeli, T
C. Carmeli, T. Heinosaari, and A. Toigo, Quantum incompati- bility witnesses, Phys. Rev. Lett. 122, 130402 (2019)
2019
-
[37]
Skrzypczyk, I
P. Skrzypczyk, I. ˇSupi´c, and D. Cavalcanti, All sets of incom- patible measurements give an advantage in quantum state dis- crimination, Phys. Rev. Lett. 122, 130403 (2019)
2019
-
[38]
R. Uola, T. Kraft, J. Shang, X.-D. Yu, and O. G ¨uhne, Quanti- fying quantum resources with conic programming, Phys. Rev. Lett. 122, 130404 (2019)
2019
-
[39]
Skrzypczyk and N
P. Skrzypczyk and N. Linden, Robustness of measurement, dis- crimination games, and accessible information, Phys. Rev. Lett. 122, 140403 (2019)
2019
-
[40]
L. Li, K. Bu, and Z.-W. Liu, Quantifying the resource content of quantum channels: An operational approach, Phys. Rev. A 101, 022335 (2020)
2020
-
[42]
Hsieh, B
C.-Y . Hsieh, B. Stratton, C.-H. Wu, and H.-Y . Ku, Dynamical resource theory of incompatibility preservability, Phys. Rev. A 111, 022422 (2025)
2025
-
[43]
Takagi, B
R. Takagi, B. Regula, K. Bu, Z.-W. Liu, and G. Adesso, Opera- tional advantage of quantum resources in subchannel discrimi- nation, Phys. Rev. Lett. 122, 140402 (2019)
2019
-
[44]
J. Bae, D. Chru ´sci´nski, and M. Piani, More entanglement im- plies higher performance in channel discrimination tasks, Phys. Rev. Lett. 122, 140404 (2019)
2019
-
[45]
Piani and J
M. Piani and J. Watrous, Necessary and su fficient quantum in- formation characterization of einstein-podolsky-rosen steering, Phys. Rev. Lett. 114, 060404 (2015)
2015
-
[46]
Napoli, T
C. Napoli, T. R. Bromley, M. Cianciaruso, M. Piani, N. John- ston, and G. Adesso, Robustness of coherence: an operational and observable measure of quantum coherence, Phys. Rev. Lett. 116, 150502 (2016)
2016
-
[47]
K. Bu, U. Singh, S.-M. Fei, A. K. Pati, and J. Wu, Maximum relative entropy of coherence: an operational coherence mea- sure, Phys. Rev. Lett. 119, 150405 (2017)
2017
-
[48]
Piani, M
M. Piani, M. Cianciaruso, T. R. Bromley, C. Napoli, N. John- ston, and G. Adesso, Robustness of asymmetry and coherence of quantum states, Phys. Rev. A 93, 042107 (2016)
2016
-
[50]
Watrous, The Theory of Quantum Information (Cambridge University Press, Cambridge, 2018)
J. Watrous, The Theory of Quantum Information (Cambridge University Press, Cambridge, 2018)
2018
-
[52]
Regula, L
B. Regula, L. Lami, G. Ferrari, and R. Takagi, Operational quantification of continuous-variable quantum resources, Phys. Rev. Lett. 126, 110403 (2021)
2021
-
[53]
Kuroiwa, R
K. Kuroiwa, R. Takagi, G. Adesso, and H. Yamasaki, Every quantum helps: Operational advantage of quantum resources beyond convexity, Phys. Rev. Lett.132, 150201 (2024)
2024
-
[54]
Turner, M
L. Turner, M. Guta, and G. Adesso, All non-gaussian states are advantageous for channel discrimination: Robustness of non- convex continuous variable quantum resources, arXiv preprint arXiv:2412.13011 (2024)
2024
-
[55]
L. Lami, B. Regula, R. Takagi, and G. Ferrari, Framework for resource quantification in infinite-dimensional general proba- bilistic theories, Phys. Rev. A 103, 032424 (2021)
2021
-
[56]
B. M. Terhal and P. Horodecki, Schmidt number for density matrices, Phys. Rev. A 61, 040301 (2000)
2000
-
[57]
C. H. Bennett, D. P. DiVincenzo, J. A. Smolin, and W. K. Woot- ters, Mixed-state entanglement and quantum error correction, Phys. Rev. A 54, 3824 (1996)
1996
-
[58]
Vidal and R
G. Vidal and R. F. Werner, Computable measure of entangle- ment, Phys. Rev. A 65, 032314 (2002)
2002
-
[59]
M. B. Plenio, Logarithmic negativity: a full entanglement monotone that is not convex, Phys. Rev. Lett. 95, 090503 (2005)
2005
-
[60]
S. A. Hill and W. K. Wootters, Entanglement of a pair of quan- tum bits, Phys. Rev. Lett. 78, 5022 (1997)
1997
-
[61]
H. M. Wiseman, S. J. Jones, and A. C. Doherty, Steering, entan- glement, nonlocality, and the einstein-podolsky-rosen paradox, Phys. Rev. Lett. 98, 140402 (2007)
2007
-
[62]
J. S. Bell, On the einstein podolsky rosen paradox, Physics (Long Island City, NY) 1, 195 (1964)
1964
-
[63]
Gallego and L
R. Gallego and L. Aolita, Resource theory of steering, Phys. Rev. X 5, 041008 (2015)
2015
-
[64]
Pramanik, Y .-W
T. Pramanik, Y .-W. Cho, S.-W. Han, S.-Y . Lee, Y .-S. Kim, and S. Moon, Revealing hidden quantum steerability using local fil- tering operations, Phys. Rev. A 99, 030101 (2019)
2019
Reviewed August 10, 2026 · model on record in the stance chip above.
Discussion (0). Continue with ORCID to comment.