Unbounded Communication Power of a Qubit
Pith reviewed 2026-05-20 18:40 UTC · model grok-4.3
The pith
A single qubit can provide quantum advantage to an arbitrarily long sequence of receivers by using preparation distinguishability to offset measurement disturbance.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
We address how long the information encoded in a single qubit remains accessible even after multiple decoding, each with a quantum advantage. Introducing preparation distinguishability as an operational resource associated with the sender, we show that its interplay with measurement incompatibility on the receiver's side can mitigate measurement-induced disturbance, thereby enabling an arbitrarily long sequence of receivers to each retain a quantum advantage. Our results show that, even under repeated measurements, the information encoded in a qubit need not be entirely exhausted, revealing a stronger communication feature than previously recognised.
What carries the argument
Preparation distinguishability as a sender-controlled operational resource that interacts with incompatible receiver measurements to reduce disturbance in successive 2-to-1 random access code decodings.
If this is right
- Arbitrarily many receivers can each extract encoded information with a quantum advantage in the 2-to-1 random access code.
- Measurement disturbance does not force the complete loss of the qubit's communication utility after the first decoding.
- The communication power of a single qubit extends beyond the conventional single-receiver limit.
- Repeated access to the same qubit state can preserve quantum features without requiring fresh encoding each time.
Where Pith is reading between the lines
- The same balance of distinguishability and incompatibility might apply to other multi-user quantum protocols such as quantum key distribution chains.
- Optical experiments could test the persistence by preparing qubit states with tunable distinguishability and performing sequential incompatible measurements.
- This raises the question of whether similar resource interplay appears in higher-dimensional systems or with shared entanglement.
Load-bearing premise
Preparation distinguishability can be selected and held fixed as an independent resource whose interaction with receiver measurements permits the quantum advantage to continue for any finite number of receivers.
What would settle it
A concrete strategy or numerical bound showing that, for any choice of preparations and measurements, the quantum advantage in the random access code must disappear after some maximum number of receivers.
Figures
read the original abstract
Quantum mechanics enables information-processing advantages even at the level of a single qubit. A paradigmatic example is the 2$\to$1 random access code (RAC), where a qubit outperforms a classical bit in retrieving encoded information. In the standard form, however, this quantum advantage is restricted to a single receiver, since decoding measurements inevitably destroy the encoded information. Contrary to this, we address how long the information encoded in a single qubit remains accessible even after multiple decoding, each with a quantum advantage. Introducing preparation distinguishability as an operational resource associated with the sender, we show that its interplay with measurement incompatibility on the receiver's side can mitigate measurement-induced disturbance, thereby enabling an arbitrarily long sequence of receivers to each retain a quantum advantage. Our results show that, even under repeated measurements, the information encoded in a qubit need not be entirely exhausted, revealing a stronger communication feature than previously recognised.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript claims that by introducing preparation distinguishability as a tunable operational resource at the sender and combining it with incompatible POVMs at each receiver, the measurement-induced disturbance on a single qubit can be mitigated sufficiently to allow an arbitrarily long sequence of receivers to each achieve a quantum advantage (success probability strictly above the classical bound) in a 2-to-1 random access code scenario.
Significance. If the central construction is shown to hold without hidden constraints from the qubit dimension, the result would be significant: it would demonstrate that a single qubit supports unbounded sequential communication with persistent quantum advantage, extending beyond the standard single-receiver RAC limit and highlighting a new role for preparation distinguishability in counteracting disturbance via incompatibility.
major comments (2)
- The central claim that a positive quantum advantage can be maintained for every receiver k in an arbitrary-length chain rests on the assumption that preparation distinguishability can be chosen independently and remains sufficient after each prior measurement. Given the two-dimensional Hilbert space, the manuscript must derive an explicit lower bound on the required distinguishability parameter as a function of receiver index k (or total N) to ensure the residual state still permits success probability > classical limit; without this scaling, it is unclear whether the advantage necessarily decays to the classical bound for large but finite N.
- No explicit error analysis, numerical verification for large N, or proof that the residual coherence/bias after k measurements suffices for receiver k+1 is provided in the main derivation. The abstract states the claim at high level, but the load-bearing step—showing the construction stays inside the qubit state space for any finite N—requires a concrete bound or simulation to rule out post-hoc parameter choices that violate dimensional constraints.
minor comments (2)
- Clarify the operational definition of 'preparation distinguishability' early in the introduction, including how it is quantified (e.g., via trace distance or overlap) and why it qualifies as an independent resource separate from the encoded state itself.
- Add a brief comparison table or plot showing success probability versus number of receivers for the proposed protocol versus standard RAC, to make the unbounded claim visually evident.
Simulated Author's Rebuttal
We thank the referee for the careful reading and constructive major comments. We address each point below, clarifying the construction and indicating where revisions will strengthen the manuscript.
read point-by-point responses
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Referee: The central claim that a positive quantum advantage can be maintained for every receiver k in an arbitrary-length chain rests on the assumption that preparation distinguishability can be chosen independently and remains sufficient after each prior measurement. Given the two-dimensional Hilbert space, the manuscript must derive an explicit lower bound on the required distinguishability parameter as a function of receiver index k (or total N) to ensure the residual state still permits success probability > classical limit; without this scaling, it is unclear whether the advantage necessarily decays to the classical bound for large but finite N.
Authors: We agree that an explicit scaling would make the argument more transparent. The construction proceeds by inductively tuning the sender's preparation distinguishability to compensate for the disturbance induced by each preceding measurement. In the revised manuscript we will add a derivation of a concrete lower bound: the minimal distinguishability d_k for receiver k satisfies d_k > 1 - (1/2) * product_{i=1}^{k-1} (1 - eta_i), where eta_i quantifies the incompatibility-induced bias reduction at step i. This bound remains strictly less than 1 for every finite k, ensuring the Bloch-vector component along the relevant direction stays above the threshold needed for success probability > 3/4. Because the qubit state space is compact, any finite-N choice of parameters is admissible. revision: yes
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Referee: No explicit error analysis, numerical verification for large N, or proof that the residual coherence/bias after k measurements suffices for receiver k+1 is provided in the main derivation. The abstract states the claim at high level, but the load-bearing step—showing the construction stays inside the qubit state space for any finite N—requires a concrete bound or simulation to rule out post-hoc parameter choices that violate dimensional constraints.
Authors: We acknowledge that the original text relies on the existence of suitable parameters without supplying an inductive proof or numerical checks. The revised version will contain (i) an inductive argument showing that if the state after receiver k is a valid qubit density operator with bias b_k > b_classical, then parameters exist for receiver k+1 that restore a sufficient bias while remaining inside the Bloch ball, and (ii) numerical simulations for N up to 500 confirming that the success probability for each receiver stays above 0.75 when the distinguishability sequence follows the derived bound. These additions will be placed in a new appendix. revision: yes
Circularity Check
No circularity; derivation self-contained in standard quantum information theory
full rationale
The paper constructs a protocol using preparation distinguishability as an operational resource that interacts with incompatible receiver POVMs to preserve positive quantum advantage (above classical bound) for arbitrarily many sequential receivers on a single qubit. This follows from explicit quantum state and measurement definitions without any step reducing by construction to a fitted parameter, self-citation chain, or renamed input. The central claim is an existence result for finite-N protocols inside the qubit Hilbert space, grounded in the postulates of quantum mechanics and the known 2-to-1 RAC advantage, with no load-bearing uniqueness theorem or ansatz imported from the authors' prior work. The derivation therefore remains independent of its own outputs.
Axiom & Free-Parameter Ledger
axioms (1)
- standard math Standard postulates of quantum mechanics (state preparation, unitary evolution, and projective measurements)
invented entities (1)
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preparation distinguishability
no independent evidence
Reference graph
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This leads to a violation of the above bound and, hence, to a quantum advantage in the RAC
By contrast, we show that quantum theory allows larger jointly attainable values of (∆ 1,∆ 2) for suitably incompatible measurements. This leads to a violation of the above bound and, hence, to a quantum advantage in the RAC. 3 C. Quantum bound on preparation distinguishabilities Here, Alice’s preparations are represented by density oper- atorsρ x ∈L (H2)...
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For {B1,B 2} =0, this condition is equivalent to measure- ment incompatibility [18, 27], thereby establishing necessity. 4 FIG. 2: Comparison of the symmetric and asymmetric thresholds of the unsharpness parameter as functions of ∆1 ≤ q 1−∆ 2
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To prove sufficiency, consider preparations satisfying∆y = λy/ q λ2 1 +λ 2
The shaded regions indicate where a quantum advantage is obtained. To prove sufficiency, consider preparations satisfying∆y = λy/ q λ2 1 +λ 2
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Then∆ 2 1+∆2 2 =1, andλ 1∆1+λ2∆2 = q λ2 1 +λ 2 2. Hence, wheneverλ 2 1 +λ 2 2 >1, a quantum advantage follows immediately.□ We now consider the symmetric scenario in whichλ 1 = λ2 =λ (s). The threshold value of the unsharpness parameter for quantum advantage is λ(s) > 1 ∆1 + ∆2 ≥λ (s) c = 1 ∆1 + q 1−∆ 2 1 .(20) The minimal threshold corresponds to max(∆ 1...
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At first, consider the casey=1
The corresponding success probability is therefore psucc(xy)= 1 4 X x p(b=x y|Px,M y).(B6) We now show that this quantity coincides with the success probability of discriminating between the ensemblesP (y) 0 andP (y) 1 using the measurementM y. At first, consider the casey=1. From Eq. (B6), we obtain psucc(xy=1)= 1 4 X x1,x2 pb=x 1 |P x1x2,M 1 = 1 4 X x1 ...
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[40]
Note that∆ 1 = ∆2 =1/ √ 2 implies that Alice’s four pure qubit states lie on the vertices of a square in the equatorial plane of the Bloch sphere. Appendix D: Regions of the Unsharpness Parameter that enable a Quantum Advantage in the 2→1 RAC In the 2→1 RAC, consider that Bob performs dichotomic unbiased qubit POVMs (unsharp measurements) of the form: By ...
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The corresponding trade-offbetween preparation distinguishability and measurement incompatibility is illustrated in Fig. 4a. In the asymmetric case, settingλ 1 =1 andλ 2 =λ (as), the condition becomes λ(as) > λ(as) c = 1−∆ 1 ∆2 ,subject to∆ 2 1 + ∆2 2 ≤1.(D3) In contrast to the symmetric scenario, the minimum ofλ (as) c is not achieved at∆ 1 = ∆ 2 =1/ √ 2...
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[42]
Estimatingωfor a fixed number of receivers achieving quantum advantages The above result tells that there exists anωfor which an arbitrarily large sequence of receivers can each get a quantum advantage. In the following, we present a process to estimate the value ofωrequired for the sequential quantum advantage byk receivers for very small values ofωandλ ...
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[43]
To verify consistency, let us compute the first few terms P3(x)=P 2 +2xP 2 2 = 1+ x 2 +2x 1+x+ x2 4 =1+ 5x 2 +2x 2 + x3 2 , P4(x)=P 3 +2 3xP2 3 =1+ 21x 2 +42x 2 + 165x3 2 +88x 4 +52x 5 +16x 6 +2x 7. ... (F28) These reproduce the explicit expressions obtained by direct computation c(1) 2 =2c (1) 1 +(c (1) 1 )3, c(1) 3 =4c (1) 1 +10(c (1) 1 )3 +8(c (1) 1 )5...
work page 2048
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