Local Marking of Locally Implementable Unitary Operations
Pith reviewed 2026-05-10 17:16 UTC · model grok-4.3
The pith
There exist globally distinguishable tripartite product unitaries that cannot be locally marked using only LOCC.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
In the setting of locally implementable unitaries drawn from a known finite set, there exist tripartite product unitaries that are globally distinguishable yet cannot be marked by any protocol restricted to local operations and classical communication. Local distinguishability implies local marking, but local marking does not imply local or global distinguishability. Marking a subset of product unitaries does not entail the capacity to mark a larger subset. The hierarchy between entangled and product probes differs between the local-marking task and ordinary discrimination.
What carries the argument
A concrete set of globally distinguishable tripartite product unitaries that admit no LOCC marking protocol.
If this is right
- Local distinguishability of unitaries guarantees local markability, but local markability does not guarantee distinguishability.
- Marking is not equivalent to discrimination for unitary operations.
- The ability to mark a subset of product unitaries does not imply the ability to mark a larger subset.
- The relative power of entangled versus product probes differs between local marking and standard discrimination.
Where Pith is reading between the lines
- Distributed quantum networks may need supplementary resources beyond LOCC to identify certain classes of operations even when those operations are product and globally distinguishable.
- The separation between marking and discrimination suggests new ways to quantify communication cost in quantum process identification tasks.
- Small-scale implementations of the constructed unitaries could be used to test whether real devices require global coherence for marking where LOCC fails.
Load-bearing premise
The unitaries are drawn from a known finite set of locally implementable operations and the only resources allowed for identification are local operations plus classical communication.
What would settle it
Existence of any LOCC protocol that, for the constructed set, correctly identifies which unitary was applied with probability strictly above random guessing.
read the original abstract
We investigate the task of local marking for locally implementable unitary operations. In this setting, multipartite quantum unitary channels, chosen randomly from a known set, are distributed among spatially separated parties without revealing their identities. The objective is to correctly identify (mark) the applied process using only local operations supplemented with classical communication (LOCC). While local distinguishability implies local marking, local marking does not guarantee either local or even global distinguishability of a set of unitaries. Thus the task of marking is not equivalent to the task of discrimination. We demonstrate a stronger manifestation of nonlocality without entanglement by constructing a set of globally distinguishable tripartite product unitaries that cannot be locally marked. In contrast to state marking, we find that marking a subset of product unitaries does not imply the ability to mark a larger subset. Finally, we explore the hierarchy of probes-entangled and product-in the context of local marking with respect to the standard discrimination scenario.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper introduces the task of local marking of locally implementable unitary operations, where parties must identify an unknown unitary channel drawn from a known finite set using only LOCC. It establishes that local distinguishability implies local marking but not conversely, provides an explicit construction of globally distinguishable tripartite product unitaries that admit no LOCC marking protocol, shows that subset marking does not imply superset marking for product unitaries (in contrast to states), and compares the hierarchy of entangled versus product probes in marking versus standard discrimination.
Significance. If the central construction and impossibility result hold, the work is significant for separating marking from discrimination in the context of unitary channels and for exhibiting a stronger form of nonlocality without entanglement that is specific to operations rather than states. The explicit construction together with exhaustive enumeration of local strategies supplies a concrete, verifiable example that can be checked by direct computation on the finite set, strengthening the case that product unitaries can display nonlocal identification features beyond those captured by discrimination alone.
minor comments (2)
- The exhaustive enumeration of LOCC strategies in the impossibility proof is complete for the finite set, but a compact table listing the distinct local measurement choices and their outcomes would improve readability without altering the argument.
- Notation for the sets of product unitaries and the marking success criterion is introduced clearly in the definitions, yet a brief reminder of the precise LOCC resource constraints (number of rounds, classical communication direction) at the start of the construction section would aid readers unfamiliar with the distinction from discrimination.
Simulated Author's Rebuttal
We thank the referee for the positive summary, significance assessment, and recommendation of minor revision. We are pleased that the central construction of globally distinguishable tripartite product unitaries without LOCC marking, along with the separation between marking and discrimination, is viewed as a stronger manifestation of nonlocality without entanglement specific to operations.
Circularity Check
No significant circularity
full rationale
The paper presents an explicit construction of a finite set of tripartite product unitaries that are globally distinguishable yet admit no LOCC marking protocol. Marking and discrimination are defined separately; the impossibility result follows from exhaustive enumeration of local strategies on that finite set. No equations, fitted parameters, or derivations appear that reduce to their own inputs by construction. No load-bearing self-citations or ansatzes are invoked. The argument is self-contained against the stated definitions and the enumerated cases.
Axiom & Free-Parameter Ledger
axioms (1)
- standard math Standard quantum mechanics and LOCC framework
Reference graph
Works this paper leans on
-
[1]
=eig (V′A 1 )†(V′A 2 ) ·eig (V′B 1 )†(V′B 2 ) = n 1,e −i(α 1+α3) o · n 1,e −i(α 2+α4) o = n 1,e −i(α 1+α3),e −i(α 2+α4),e −i(α 1+α2+α3+α4) o . (8) Sinceα 1 +α 2 +α 3 +α 4 <π, convex combination of above four eigenvalues does not include the origin. Hence, the two unitaries are indistinguishable. For local marking, suppose Alice starts the protocol. The ma...
-
[2]
(23) By normalization,R 1 +R 2 +R 3 =1
Consequently, ⟨ψp|(Z A 3 )†ZA 3 ⊗(Z A 1 )†ZA 2 ⊗(Z A 2 )†ZA 1 ⊗1⊗1⊗1|ψ p⟩ = 1 ∑ i,j,j ′,k,k′,l,m,n=0 C∗ i,j,k,l,m,n Cij ′k′lmn ⟨j|(Z A 1 )†ZA 2 |j ′⟩ ⟨k|(Z A 2 )†ZA 1 |k′⟩ = 1 ∑ i,j,k,l,m,n=0 |Ci,j,k,l,m,n |2 ⟨j|(Z A 1 )†ZA 2 |j⟩ ⟨k|(Z A 2 )†ZA 1 |k⟩ =1(R 1) +i(R 2)−i(R 3), (22) where R1 = ∑ i,l,m,n (|Ci,j=0,k=0,l,m,n |2 +|C i,j=1,k=1,l,m,n |2), R2 = ∑ i,...
-
[3]
If we put these values ofR 2 andR 3 into (24), the expres- sion reduces to non-zero value. That indicates first two unitaries are not distinguishable with|ϕ p⟩, which suc- cessfully distinguishes last two unitaries. That proves the impossibility of common probing state to distin- guish six unitaries and subsequently, implies the failure of 3-LM of the uni...
-
[4]
Quantum state discrimination and its applications,
Joonwoo Bae and Leong-Chuan Kwek, “Quantum state discrimination and its applications,” Journal of Physics A: Mathematical and Theoretical48, 083001 (2015)
work page 2015
-
[5]
Quantum state discrimination and se- lected applications,
J ´anos A Bergou, “Quantum state discrimination and se- lected applications,” Journal of Physics: Conference Se- ries84, 012001 (2007)
work page 2007
-
[6]
Unbounded quantum advantage in communica- tion complexity measured by distinguishability,
Satyaki Manna, Anubhav Chaturvedi, and Debashis Saha, “Unbounded quantum advantage in communica- tion complexity measured by distinguishability,” Phys. Rev. Res.6, 043269 (2024)
work page 2024
-
[7]
Entanglement assisted communication complexity mea- sured by distinguishability,
Satyaki Manna, Ankush Pandit, and Debashis Saha, “Entanglement assisted communication complexity mea- sured by distinguishability,” (2026), arXiv:2603.19105 [quant-ph]
-
[8]
Ankush Pandit, Soumyabrata Hazra, Satyaki Manna, Anubhav Chaturvedi, and Debashis Saha, “Limits of classical correlations and quantum advantages under (anti-)distinguishability constraints in multipartite com- munication,” Phys. Rev. A113, 032433 (2026)
work page 2026
-
[9]
Quantum advantages in multiparty communication,
Ankush Pandit, “Quantum advantages in multiparty communication,” (2025), arXiv:2512.05538 [quant-ph]
-
[10]
Nonlocality, asym- metry, and distinguishing bipartite states,
Jonathan Walgate and Lucien Hardy, “Nonlocality, asym- metry, and distinguishing bipartite states,” Phys. Rev. Lett.89, 147901 (2002)
work page 2002
-
[11]
Quantum nonlocality without entanglement,
Charles H. Bennett, David P . DiVincenzo, Christopher A. Fuchs, Tal Mor, Eric Rains, Peter W. Shor, John A. Smolin, and William K. Wootters, “Quantum nonlocality without entanglement,” Phys. Rev. A59, 1070–1091 (1999)
work page 1999
-
[12]
Local distinguishability of multipartite orthogonal quantum states,
Jonathan Walgate, Anthony J. Short, Lucien Hardy, and Vlatko Vedral, “Local distinguishability of multipartite orthogonal quantum states,” Phys. Rev. Lett.85, 4972– 4975 (2000)
work page 2000
-
[13]
Optimal local discrimination of two multipartite pure states,
S Virmani, M.F Sacchi, M.B Plenio, and D Markham, “Optimal local discrimination of two multipartite pure states,” Physics Letters A288, 62–68 (2001)
work page 2001
-
[14]
John Watrous, “Bipartite subspaces having no bases dis- tinguishable by local operations and classical communi- cation,” Phys. Rev. Lett.95, 080505 (2005)
work page 2005
-
[15]
Strong quantum nonlo- cality without entanglement,
Saronath Halder, Manik Banik, Sristy Agrawal, and Somshubhro Bandyopadhyay, “Strong quantum nonlo- cality without entanglement,” Phys. Rev. Lett.122, 040403 (2019)
work page 2019
-
[16]
Activating strong nonlocality from lo- cal sets: An elimination paradigm,
Subhendu B. Ghosh, Tathagata Gupta, Ardra A. V ., Anan- damay Das Bhowmik, Sutapa Saha, Tamal Guha, and Amit Mukherjee, “Activating strong nonlocality from lo- cal sets: An elimination paradigm,” Phys. Rev. A106, L010202 (2022)
work page 2022
-
[17]
Nonlocality without entanglement: Quantum theory and beyond,
Some Sankar Bhattacharya, Sutapa Saha, Tamal Guha, and Manik Banik, “Nonlocality without entanglement: Quantum theory and beyond,” Phys. Rev. Res.2, 012068 (2020)
work page 2020
-
[18]
Nonlocality without entanglement in exclusion of quantum states,
Satyaki Manna and Anandamay Das Bhowmik, “Non- locality without entanglement in exclusion of quantum states,” (2026), arXiv:2602.15452 [quant-ph]
-
[19]
Global vs. local dis- crimination of locally implementable multipartite unitaries,
Satyaki Manna, Sneha Suresh, Anandamay Das Bhowmik, and Debashis Saha, “Global vs. local dis- crimination of locally implementable multipartite unitaries,” (2025), arXiv:2509.10430 [quant-ph]. 8
-
[20]
Strong quantum nonlocality and unextendibility without entanglement in N-partite systems with oddN,
Yiyun He, Fei Shi, and Xiande Zhang, “Strong quantum nonlocality and unextendibility without entanglement in N-partite systems with oddN,” Quantum8, 1349 (2024)
work page 2024
-
[21]
Multipartite nonlocality with- out entanglement in many dimensions,
J. Niset and N. J. Cerf, “Multipartite nonlocality with- out entanglement in many dimensions,” Phys. Rev. A74, 052103 (2006)
work page 2006
-
[22]
Samrat Sen, Edwin Peter Lobo, Sahil Gopalkrishna Naik, Ram Krishna Patra, Tathagata Gupta, Subhendu B. Ghosh, Sutapa Saha, Mir Alimuddin, Tamal Guha, Some Sankar Bhattacharya, and Manik Banik, “Local quantum state marking,” Phys. Rev. A105, 032407 (2022)
work page 2022
-
[23]
Conclusive local state marking: More non- locality with no entanglement,
Samrat Sen, “Conclusive local state marking: More non- locality with no entanglement,” Phys. Rev. A112, 052225 (2025)
work page 2025
-
[24]
Quantum computations: algorithms and er- ror correction,
A Yu Kitaev, “Quantum computations: algorithms and er- ror correction,” Russian Mathematical Surveys52, 1191 (1997)
work page 1997
-
[25]
Statistical distinguishability between unitary operations,
A. Ac ´ın, “Statistical distinguishability between unitary operations,” Phys. Rev. Lett.87, 177901 (2001)
work page 2001
-
[26]
Per- fect distinguishability of quantum operations,
Runyao Duan, Yuan Feng, and Mingsheng Ying, “Per- fect distinguishability of quantum operations,” Phys. Rev. Lett.103, 210501 (2009)
work page 2009
-
[27]
All entangled states are useful for channel discrimination,
Marco Piani and John Watrous, “All entangled states are useful for channel discrimination,” Phys. Rev. Lett.102, 250501 (2009)
work page 2009
-
[28]
Perfect discrimination of quantum measurements using entangled systems,
Chandan Datta, Tanmoy Biswas, Debashis Saha, and Remigiusz Augusiak, “Perfect discrimination of quantum measurements using entangled systems,” New Journal of Physics23, 043021 (2021)
work page 2021
-
[29]
Single-shot distinguisha- bility and antidistinguishability of quantum measure- ments,
Satyaki Manna, Sneha Suresh, Manan Singh Kach- hawaha, and Debashis Saha, “Single-shot distinguisha- bility and antidistinguishability of quantum measure- ments,” Phys. Rev. A111, 022221 (2025)
work page 2025
-
[30]
Single- shot antidistinguishability of unitary operations,
Satyaki Manna and Anandamay Das Bhowmik, “Single- shot antidistinguishability of unitary operations,” Phys. Rev. A113, 022218 (2026)
work page 2026
-
[31]
Limitation of maximally entangled probes for single-shot distinguishability of unitaries,
Satyaki Manna, Anandamay Das Bhowmik, and De- bashis Saha, “Limitation of maximally entangled probes for single-shot distinguishability of unitaries,” Phys. Rev. A112, 042215 (2025)
work page 2025
-
[32]
Satyaki Manna, “Alld⊗ddimensional entangled states are useful for the antidiscrimination of quantum mea- surements whendis even,” (2025), arXiv:2510.26255 [quant-ph]
-
[33]
Funda- mental limits to quantum channel discrimination,
S. Pirandola, R. Laurenza, C. Lupo, and et al., “Funda- mental limits to quantum channel discrimination,” npj Quantum Inf 5 (2019), 10.1038/s41534-019-0162-y
-
[34]
Adaptive versus nonadaptive strate- gies for quantum channel discrimination,
Aram W. Harrow, Avinatan Hassidim, Debbie W. Leung, and John Watrous, “Adaptive versus nonadaptive strate- gies for quantum channel discrimination,” Phys. Rev. A 81, 032339 (2010)
work page 2010
-
[35]
Entan- glement is not necessary for perfect discrimination be- tween unitary operations,
Runyao Duan, Yuan Feng, and Mingsheng Ying, “Entan- glement is not necessary for perfect discrimination be- tween unitary operations,” Phys. Rev. Lett.98, 100503 (2007)
work page 2007
-
[36]
Improved discrimination of unitary transfor- mations by entangled probes,
G Mauro D’Ariano, Paoloplacido Lo Presti, and Matteo G A Paris, “Improved discrimination of unitary transfor- mations by entangled probes,” Journal of Optics B: Quan- tum and Semiclassical Optics4, S273 (2002)
work page 2002
-
[37]
Lo- cal distinguishability of multipartite unitary operations,
Runyao Duan, Yuan Feng, and Mingsheng Ying, “Lo- cal distinguishability of multipartite unitary operations,” Phys. Rev. Lett.100, 020503 (2008)
work page 2008
-
[38]
Distinguishability and indistinguishability by local operations and classical communication,
Heng Fan, “Distinguishability and indistinguishability by local operations and classical communication,” Phys. Rev. Lett.92, 177905 (2004)
work page 2004
-
[39]
Communi- cation via one- and two-particle operators on einstein- podolsky-rosen states,
Charles H. Bennett and Stephen J. Wiesner, “Communi- cation via one- and two-particle operators on einstein- podolsky-rosen states,” Phys. Rev. Lett.69, 2881–2884 (1992)
work page 1992
-
[40]
Distributed quantum dense cod- ing,
D. Bruß, G. M. D’Ariano, M. Lewenstein, C. Macchiavello, A. Sen(De), and U. Sen, “Distributed quantum dense cod- ing,” Phys. Rev. Lett.93, 210501 (2004)
work page 2004
-
[41]
Pseudo- random unitary operators for quantum informa- tion processing,
Joseph Emerson, Yaakov S. Weinstein, Marcos Sara- ceno, Seth Lloyd, and David G. Cory, “Pseudo- random unitary operators for quantum informa- tion processing,” Science302, 2098–2100 (2003), https://www.science.org/doi/pdf/10.1126/science.1090790
-
[42]
Unitary application of the quantum error correction codes,
You Bo, Xu Ke, and Wu Xiao-Hua, “Unitary application of the quantum error correction codes,” Communications in Theoretical Physics58, 377 (2012)
work page 2012
-
[43]
Quantum cryptography based on bell’s theorem,
Artur K. Ekert, “Quantum cryptography based on bell’s theorem,” Phys. Rev. Lett.67, 661–663 (1991)
work page 1991
-
[44]
Query complexity of unitary operation discrimination,
Xiaowei Huang and Lvzhou Li, “Query complexity of unitary operation discrimination,” Physica A: Statistical Mechanics and its Applications604, 127863 (2022)
work page 2022
discussion (0)
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