Interference visibility as a witness of preparation contextuality via overlap inequalities
Pith reviewed 2026-05-19 16:39 UTC · model grok-4.3
The pith
Pairwise visibility measurements in multi-path interferometers witness preparation contextuality via violated overlap inequalities.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Under ideal symmetric conditions, interference visibility directly encodes state overlaps, without requiring tomography or SWAP tests. For three paths, any jointly diagonalizable (coherence-free) description must satisfy V12² + V23² - V13² ≤ 1, where Vij are two-path visibilities. Pure qubit detector states violate this bound, achieving a maximal value of 5/4. The generalization yields the tight qubit bound Sn^max = n cos²(π/2n) - 1 for all n ≥ 3, achieved by coplanar pure qubit states with uniform angular separation π/n. Under the operational equivalences used in overlap-based generalized noncontextuality frameworks, violations of these visibility inequalities witness preparation contextual
What carries the argument
Visibility inequalities derived from pairwise measurements that bound possible state overlaps in jointly diagonalizable descriptions of n-path interferometers.
Load-bearing premise
The system operates under ideal symmetric conditions with jointly diagonalizable coherence-free descriptions that respect the operational equivalences of overlap-based noncontextuality frameworks.
What would settle it
Measure the three pairwise visibilities in a symmetric three-path interferometer prepared with a pure qubit state and check whether their squares satisfy V12² + V23² - V13² > 1.
Figures
read the original abstract
We show that standard multi-path interferometry, using only pairwise visibility measurements, provides an operational route to tests of preparation noncontextuality. Under ideal symmetric conditions, interference visibility directly encodes state overlaps, without requiring tomography or SWAP tests. For three paths, any jointly diagonalizable (coherence-free) description must satisfy $V_{12}^2+V_{23}^2-V_{13}^2\le 1$, where $V_{ij}$ are two-path visibilities. Pure qubit detector states violate this bound, achieving a maximal value of $5/4$. We generalize to arbitrary $n$-path interferometers and derive the tight qubit bound $S_n^{\max}=n\cos^2(\pi/2n)-1$ for all $n\ge3$, achieved by coplanar pure qubit states with uniform angular separation $\pi/n$. A robustness analysis yields explicit experimental thresholds. Under the operational equivalences used in overlap-based generalized noncontextuality frameworks, violations of these visibility inequalities also witness preparation contextuality. For $n$-cycle inequalities, only the pairwise visibilities appearing in the cycle need to be measured.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper shows that pairwise interference visibility measurements in multi-path interferometers provide an operational witness for preparation noncontextuality via overlap inequalities. Under ideal symmetric conditions, visibilities directly encode state overlaps without tomography or SWAP tests. For three paths, any jointly diagonalizable description satisfies V_{12}^2 + V_{23}^2 - V_{13}^2 ≤ 1, which pure qubit states violate up to a value of 5/4. This is generalized to n-path interferometers yielding the tight qubit bound S_n^max = n cos^2(π/2n) - 1 for n ≥ 3, achieved by coplanar pure states with uniform angular separation π/n. A robustness analysis supplies explicit experimental thresholds, and violations witness preparation contextuality under the operational equivalences of overlap-based generalized noncontextuality frameworks. For n-cycle inequalities, only the relevant pairwise visibilities need to be measured.
Significance. If the central derivations hold, this constitutes a useful operational advance by linking standard interferometric observables directly to preparation noncontextuality tests. The explicit qubit bounds, generalization to arbitrary n, and provision of robustness thresholds are strengths that facilitate experimental implementation in photonic systems. The manuscript supplies clean inequality derivations from overlap relations and falsifiable visibility predictions, which enhance its value for quantum foundations research.
minor comments (3)
- In the section deriving the three-path inequality, explicitly number and reference the key overlap-to-visibility mapping equations to improve traceability of the steps from operational equivalences to the bound V_{12}^2 + V_{23}^2 - V_{13}^2 ≤ 1.
- The robustness analysis should include a brief table or plot summarizing the experimental visibility thresholds as a function of noise parameters for quick reference by experimental groups.
- Clarify the notation for S_n^max in the generalization section by providing its explicit definition immediately before the bound is stated, rather than relying primarily on the abstract.
Simulated Author's Rebuttal
We thank the referee for their positive summary and recommendation of minor revision. The assessment correctly captures the main results on visibility inequalities as witnesses of preparation contextuality.
Circularity Check
No significant circularity; derivation self-contained
full rationale
The paper maps pairwise visibilities to state overlaps under explicit ideal symmetric conditions, derives the inequality V12² + V23² - V13² ≤ 1 for jointly diagonalizable descriptions directly from those overlap relations, exhibits explicit violation by pure qubit states, and obtains the general bound Sn^max = n cos²(π/2n) - 1 via standard trigonometric maximization over coplanar states. These steps are algebraic and geometric calculations independent of the target contextuality conclusion. The final link to preparation noncontextuality is stated as following from pre-existing operational equivalences in overlap-based generalized noncontextuality frameworks rather than being presupposed or fitted within the present derivation. No self-citation chain, ansatz smuggling, or reduction of a claimed prediction to a fitted input is present in the provided derivation chain.
Axiom & Free-Parameter Ledger
axioms (2)
- domain assumption Jointly diagonalizable (coherence-free) descriptions must satisfy the visibility inequality under ideal symmetric conditions.
- domain assumption Operational equivalences in overlap-based generalized noncontextuality frameworks allow visibility violations to witness preparation contextuality.
Reference graph
Works this paper leans on
-
[1]
T. Baumgratz, M. Cramer, and M. B. Plenio, Quantify- ing coherence, Phys. Rev. Lett.113, 140401 (2014)
work page 2014
-
[2]
S. Designolle, R. Uola, K. Luoma, and N. Brunner, Set coherence: Basis-independent quantification of quantum coherence, Phys. Rev. Lett.126, 220404 (2021)
work page 2021
-
[3]
E. F. Galv˜ ao and D. J. Brod, Quantum and classical bounds for two-state overlaps, Phys. Rev. A101, 062110 (2020)
work page 2020
- [4]
-
[5]
R. W. Spekkens, Contextuality for preparations, trans- formations, and unsharp measurements, Phys. Rev. A 71, 052108 (2005)
work page 2005
-
[6]
M. D. Mazurek, M. F. Pusey, R. Kunjwal, K. J. Resch, and R. W. Spekkens, An experimental test of noncontex- tuality without unphysical idealizations, Nature Commu- nications7, 11780 (2016)
work page 2016
-
[7]
A. K. Ekert, C. M. Alves, D. K. L. Oi, M. Horodecki, P. Horodecki, and L. C. Kwek, Direct estimations of lin- ear and nonlinear functionals of a quantum state, Phys. Rev. Lett.88, 217901 (2002)
work page 2002
-
[8]
Qureshi, Interference visibility and wave-particle du- ality in multipath interference, Phys
T. Qureshi, Interference visibility and wave-particle du- ality in multipath interference, Phys. Rev. A100, 042105 (2019)
work page 2019
-
[9]
M. N. Bera, T. Qureshi, M. A. Siddiqui, and A. K. Pati, Duality of quantum coherence and path distinguishabil- ity, Phys. Rev. A92, 012118 (2015)
work page 2015
-
[10]
T. Qureshi and M. A. Siddiqui, Wave–particle duality in n-path interference, Annals of Physics385, 598 (2017)
work page 2017
- [11]
- [12]
-
[13]
M. A. Siddiqui and T. Qureshi, Three-slit interference: A duality relation, Progress of Theoretical and Experi- 9 mental Physics2015, 083A02 (2015)
work page 2015
- [14]
-
[15]
A. K. Roy, N. Pathania, N. K. Chandra, P. K. Panigrahi, and T. Qureshi, Coherence, path predictability, andi concurrence: A triality, Phys. Rev. A105, 032209 (2022)
work page 2022
-
[16]
J. C. F. Matthews, A. Politi, A. Stefanov, and J. L. O’Brien, Manipulation of multiphoton entanglement in waveguide quantum circuits, Nature Photonics3, 346 (2009)
work page 2009
-
[17]
H. Heo, K. Kwon, D. Lee, H.-S. Jang, S. Kim, H. Shin, Y.-S. Kim, S.-W. Han, and H. Jung, Classical and quan- tum experiments using hybrid si3n4-linbo3 photonic chip, IEEE Photonics Technology Letters37, 173 (2025)
work page 2025
-
[18]
M. F. Pusey, Robust preparation noncontextuality in- equalities in the simplest scenario, Phys. Rev. A98, 022112 (2018)
work page 2018
-
[19]
D. Schmid and R. W. Spekkens, Contextual advantage for state discrimination, Phys. Rev. X8, 011015 (2018)
work page 2018
-
[20]
S. Boyd and L. Vandenberghe,Convex Optimization (Cambridge University Press, 2004)
work page 2004
-
[21]
A. A. Klyachko, M. A. Can, S. Binicio˘ glu, and A. S. Shu- movsky, Simple test for hidden variables in spin-1 sys- tems, Phys. Rev. Lett.101, 020403 (2008)
work page 2008
- [22]
-
[23]
T. Giordani, C. Esposito, F. Hoch, G. Carvacho, D. J. Brod, E. F. Galv˜ ao, N. Spagnolo, and F. Sciarrino, Wit- nesses of coherence and dimension from multiphoton in- distinguishability tests, Phys. Rev. Res.3, 023031 (2021)
work page 2021
- [24]
discussion (0)
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