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arxiv: 2604.16711 · v1 · submitted 2026-04-17 · 🪐 quant-ph

Adversarial quantum teleportation

Pith reviewed 2026-05-10 07:52 UTC · model grok-4.3

classification 🪐 quant-ph
keywords quantum teleportationfidelity thresholdadversarial modelcheating partiesmulti-partite protocolquantum logic circuitsaverage fidelity
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The pith

Adversarial models justify fidelity thresholds of 1/2 and 2/3 for quantum teleportation claims.

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

The paper builds models of quantum teleportation that explicitly include cheating parties who attempt to make unsuccessful protocols appear successful. It shows that the average-fidelity thresholds of 1/2 and 2/3, long used in the field, emerge directly from considering different types of adversaries rather than being chosen arbitrarily. A sympathetic reader cares because this grounds the debate over performance metrics in concrete cheating scenarios, offering a way to evaluate whether a claimed teleportation has truly occurred against potential falsifiers. The work frames the protocol as multi-partite with explicit quantum-logic circuits that distinguish honest from adversarial behavior.

Core claim

By modeling quantum teleportation as a multi-partite protocol that incorporates cheating parties, the average-fidelity thresholds of 1/2 and 2/3 arise naturally depending on the adversary type, providing justification for these values in claims of successful teleportation.

What carries the argument

Adversarial quantum teleportation described as a multi-partite protocol with explicit quantum-logic circuits in both honest and cheating settings.

If this is right

  • Fidelity thresholds gain justification tied to the specific adversary under consideration.
  • The multi-partite circuit approach extends directly to evaluating other quantum-information tasks against cheating.
  • Teleportation claims can be assessed by comparing performance against explicit adversarial circuits rather than fixed rules alone.

Where Pith is reading between the lines

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

  • This framing could guide the design of teleportation protocols that remain robust even when the adversary type is unknown in advance.
  • Similar adversarial modeling might clarify threshold debates in related tasks such as quantum state discrimination.
  • Testing the circuits on small-scale quantum devices could reveal whether the derived thresholds hold under realistic noise.

Load-bearing premise

The constructed adversarial models accurately represent all relevant cheating strategies possible in quantum teleportation protocols.

What would settle it

An experiment showing average fidelity above the threshold yet allowing a defined cheating party to falsely demonstrate successful teleportation would falsify the justification.

Figures

Figures reproduced from arXiv: 2604.16711 by Barry C Sanders, Nehad AttaElmanan AbdElrahim Mabrouk.

Figure 1
Figure 1. Figure 1: Elements of quantum circuits. (a) Single-qubit rota [PITH_FULL_IMAGE:figures/full_fig_p002_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Quantum circuits representing standard single-qubit [PITH_FULL_IMAGE:figures/full_fig_p003_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: Quantum circuits representing teleporting a one-qubit [PITH_FULL_IMAGE:figures/full_fig_p006_3.png] view at source ↗
Figure 6
Figure 6. Figure 6: Quantum circuit representing ℘ AB. A and B trash their qubits. parties execute perfectly, the analogue of Certificate 1 is the following, which replaces Certificate 2. Certificate 2 (Perfect ℘ A1 and ℘ A2). A employs more than zero qubits from D for the QTPs. Of course such a certificate is useless, both because it can only be issued if perfection is attained and also because a certificate that someone is … view at source ↗
Figure 4
Figure 4. Figure 4: Quantum circuits represent two A cheating protocols: [PITH_FULL_IMAGE:figures/full_fig_p007_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: Quantum circuit representing ℘ B. B trashes his qubit and replacew his X-gate by 1 and his Z-gate with by an X￾gate. C / m−1 R(Ψ) / m−1 A C H • X D B [PITH_FULL_IMAGE:figures/full_fig_p007_5.png] view at source ↗
Figure 3
Figure 3. Figure 3: As with C, we write the isometry over m+2 qubits so, in this case, D’s action involves an m-qubit identity operator. D executes the entangling gadget (2.23) as part of D’s overall (m + 2)-qubit transformation 1 m ⊗ [PITH_FULL_IMAGE:figures/full_fig_p008_3.png] view at source ↗
read the original abstract

Claims of successful quantum teleportation are backed up by showing that fidelity exceeds some specified threshold, but whether fidelity is the performance metric and what the threshold should be has been a subject of vigorous debate. We construct adversarial models for quantum teleportation, i.e., involving cheating parties, and show that fidelity thresholds can be justified in the context of the type of adversary trying to prove unsuccessful quantum teleportation has been successful. In particular we show how previously established average-fidelity thresholds of 1/2 and 2/3 arise from our adversarial approach. Mathematically, we describe adversarial quantum teleportation as a multi-partite protocol with explicit quantum-logic circuits in both honest and cheating settings, and our methods are relevant beyond quantum teleportation to other quantum-information gadgets.

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

0 major / 1 minor

Summary. The manuscript develops an adversarial framework for assessing quantum teleportation by incorporating cheating parties into the protocol. Using multi-partite quantum circuits with explicit gates for both honest and adversarial behaviors, it derives the average fidelity thresholds of 1/2 and 2/3 as the critical points separating successful from unsuccessful faking attempts by the adversary. The methods are claimed to generalize to other quantum information tasks.

Significance. This approach is significant because it grounds the choice of fidelity thresholds in the concrete capabilities of an adversary rather than abstract arguments, potentially resolving part of the debate on what constitutes successful teleportation. The provision of explicit circuits is particularly valuable as it enables direct simulation and verification, which is a strong point for the paper. If the thresholds indeed emerge parameter-free from the models, this strengthens the theoretical foundation of the field.

minor comments (1)
  1. Ensure that the quantum circuits are presented with sufficient detail, including the specific gates and qubit connections, to allow readers to reproduce the threshold calculations.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive summary and significance assessment of our manuscript on adversarial quantum teleportation. The review accurately reflects the paper's focus on deriving fidelity thresholds from explicit adversarial models and the provision of multi-partite circuits. No specific major comments were listed in the report, so we provide no point-by-point responses below. We remain available to incorporate any minor revisions once concrete suggestions are supplied.

Circularity Check

0 steps flagged

No significant circularity in derivation chain

full rationale

The paper constructs explicit multi-partite protocols equipped with quantum-logic circuits for honest and adversarial (cheating) parties in quantum teleportation. It shows that the known average-fidelity thresholds of 1/2 and 2/3 emerge directly as the success/failure points for the adversary in faking a valid teleportation outcome. This modeling is independent of prior parameter fits or self-referential definitions; the thresholds are derived from the adversary's explicit capabilities rather than presupposed. No self-definitional loops, fitted inputs renamed as predictions, load-bearing self-citations, or smuggled ansatzes are present in the provided derivation steps. The framework is presented as generalizable beyond teleportation, confirming it is self-contained.

Axiom & Free-Parameter Ledger

0 free parameters · 1 axioms · 0 invented entities

The work relies on standard quantum mechanics and teleportation protocols without introducing new free parameters or entities; the adversarial models are the primary addition.

axioms (1)
  • standard math Standard assumptions of quantum mechanics and quantum information theory for teleportation protocols
    The paper extends existing quantum teleportation concepts with adversarial analysis.

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Reference graph

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