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arXiv:2610.15317

Receiver-Constrained Recovery Placement for Encoded-Qutrit Teleportation under Monitored Decay

Yifan Shi, Duan Wang, Quanzhen Ding, He Zhang, Da-Wei Luo, Ting Yu

quant-phSubmitted Oct 11, 2026• Announced Oct 13, 2026• 0 citations
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Abstract

Using established probabilistic measurement-reversal theory, we study recovery placement in encoded-qutrit teleportation under monitored decay. We characterize the success advantage of reversing a no-jump map only on the encoded support and compare two receiver capabilities. The restricted-map construction applies to general finite-dimensional supports; explicit timing results are obtained for a coherent V-type sender, a $Λ$-type receiver, and $S=\{0,2\}$, within a prescribed family of maximal exact sender reversals. With one outcome-independent full-space receiver filter, we maximize success probability at fixed total time subject to a minimum success-weighted conditional fidelity. A single preassigned recovery time yields up to three duration-dependent regimes: no sender reversal, the earliest feasible intermediate reversal, and final-time reversal. If recovery times may be randomized independently of the input and only the pooled successful ensemble must meet the fidelity requirement, the optimum over all such timing distributions mixes the two endpoints for $ΓT \ge (\ln 3)/2$. With Bell-outcome-dependent nonunitary receiver recovery, each accepted full-column-rank transfer branch can instead be reversed exactly. For the same model and sender-operation family, omitting sender reversal uniquely maximizes the exact-teleportation success probability for every finite $T>0$ at positive decay rate. Partial pathway coherence further distinguishes relative support gain from absolute recovery success: the long-time dark-state plateau survives only for fully coherent decay. These results show how receiver control capabilities and the meaning of the fidelity constraint determine whether intermediate sender recovery is useful.

AI Summary

The paper asks when a heralded sender-side reversal should be applied during encoded-state teleportation under monitored decay, and how the answer depends on receiver control and the fidelity constraint. It applies established probabilistic reversal theory to the restricted no-jump map $K_0Q$, giving optimal exact-recovery probability $\sigma_{\min}^2(K_0Q)$. This equals the full-space bound precisely when the encoded support intersects the minimum right-singular subspace. Explicit timing results concern a coherent $V$-type sender, a $\Lambda$-type receiver, and support $S=\{0,2\}$. With one fixed full-space receiver inverse, convexity and endpoint comparisons solve success maximization subject to a minimum success-weighted conditional fidelity: a single preassigned timing can favor no sender reversal, the earliest feasible intermediate reversal, or final-time reversal. If only pooled fidelity is constrained, optimization over all input-independent timing distributions yields an endpoint mixture for $\Gamma T\geq(\ln3)/2$. At $\Gamma T=2$ and fidelity $0.86$, randomization increases success from $1.01180\%$ to $1.28759\%$. With Bell-outcome-dependent nonunitary receiver recovery, each full-column-rank transfer branch is exactly reversible. Closed branch singular values show that omitting sender reversal uniquely maximizes success for every finite $T>0$ at positive decay rate within the prescribed sender family; success is $17.8933\%$ at $\Gamma T=2$. Timing claims assume ideal monitoring, independent Markovian baths, a noiseless resource partner, fixed encoding and Bell basis, and maximal exact sender reversals—not arbitrary controls. Partial pathway coherence removes the long-time recovery plateau. The supporting non-Markovian example treats uninterrupted evolution only; intermediate interventions require a multi-time description.

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22 pages, 6 figures

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Using established probabilistic measurement-reversal theory, we study recovery placement in encoded-qutrit teleportation under monitored decay. We characterize the success advantage of reversing a no-jump map only on the encoded support and compare two receiver capabilities. The restricted-map construction applies to general finite-dimensional supports; explicit timing results are obtained for a coherent V-type sender, a ΛΛΛ-type receiver, and S={0,2}S=\{0,2\}S={0,2}, within a prescribed family of maximal exact sender reversals. With one outcome-independent full-space receiver filter, we maximize success probability at fixed total time subject to a minimum success-weighted conditional fidelity. A single preassigned recovery time yields up to three duration-dependent regimes: no sender reversal, the earliest feasible intermediate reversal, and final-time reversal. If recovery times may be randomized independently of the input and only the pooled successful ensemble must meet the fidelity requirement, the optimum over all such timing distributions mixes the two endpoints for ΓT≥(ln⁡3)/2ΓT \ge (\ln 3)/2ΓT≥(ln3)/2. With Bell-outcome-dependent nonunitary receiver recovery, each accepted full-column-rank transfer branch can instead be reversed exactly. For the same model and sender-operation family, omitting sender reversal uniquely maximizes the exact-teleportation success probability for every finite T>0T>0T>0 at positive decay rate. Partial pathway coherence further distinguishes relative support gain from absolute recovery success: the long-time dark-state plateau survives only for fully coherent decay. These results show how receiver control capabilities and the meaning of the fidelity constraint determine whether intermediate sender recovery is useful.
The paper asks when a heralded sender-side reversal should be applied during encoded-state teleportation under monitored decay, and how the answer depends on receiver control and the fidelity constraint. It applies established probabilistic reversal theory to the restricted no-jump map K0QK_0QK0​Q, giving optimal exact-recovery probability σmin⁡2(K0Q)\sigma_{\min}^2(K_0Q)σmin2​(K0​Q). This equals the full-space bound precisely when the encoded support intersects the minimum right-singular subspace.
Explicit timing results concern a coherent VVV-type sender, a Λ\LambdaΛ-type receiver, and support S={0,2}S=\{0,2\}S={0,2}. With one fixed full-space receiver inverse, convexity and endpoint comparisons solve success maximization subject to a minimum success-weighted conditional fidelity: a single preassigned timing can favor no sender reversal, the earliest feasible intermediate reversal, or final-time reversal. If only pooled fidelity is constrained, optimization over all input-independent timing distributions yields an endpoint mixture for ΓT≥(ln⁡3)/2\Gamma T\geq(\ln3)/2ΓT≥(ln3)/2. At ΓT=2\Gamma T=2ΓT=2 and fidelity 0.860.860.86, randomization increases success from 1.01180%1.01180\%1.01180% to 1.28759%1.28759\%1.28759%.
With Bell-outcome-dependent nonunitary receiver recovery, each full-column-rank transfer branch is exactly reversible. Closed branch singular values show that omitting sender reversal uniquely maximizes success for every finite T>0T>0T>0 at positive decay rate within the prescribed sender family; success is 17.8933%17.8933\%17.8933% at ΓT=2\Gamma T=2ΓT=2.
Timing claims assume ideal monitoring, independent Markovian baths, a noiseless resource partner, fixed encoding and Bell basis, and maximal exact sender reversals—not arbitrary controls. Partial pathway coherence removes the long-time recovery plateau. The supporting non-Markovian example treats uninterrupted evolution only; intermediate interventions require a multi-time description.
In practical quantum communication, quantum channels are inevitably affected by noise and decoherence, leading to their degradation into non-maximally entangled or even mixed states. As a result, conventional quantum teleportation schemes based on non-maximally entangled channels are inherently probabilistic and cannot simultaneously achieve unit fidelity and unit success probability. To address this issue, we exploit the structural degrees of freedom of high-dimensional partially entangled channels and construct an asymmetric joint measurement basis matched to the Schmidt-coefficient distribution of the channel, thereby proposing a controlled multi-output perfect quantum teleportation scheme. First, based on a three-dimensional partially entangled five-qutrit channel, a controlled two-output teleportation model for unknown single-qubit states is established. Perfect transmission with both unit fidelity and unit success probability is achieved through the controller’s projective measurement, the sender’s asymmetric joint measurement, and the receivers’ corresponding local recovery operations. On this basis, the scheme is generalized to arbitrary d-dimensional partially entangled channels and further extended from the two-output configuration to the multi-output scenario. Our analysis shows that, when the two largest Schmidt coefficients of the channel are equal, deterministic perfect teleportation with both unit fidelity and unit success probability can still be achieved using non-maximally entangled resources. The proposed scheme is more consistent with realistic quantum communication environments and provides a theoretical foundation for efficient and controllable quantum information distribution in complex quantum networks.
Through a detailed study of nondestructive controlled quantum teleportation (NCQT) with two outputs in three-dimensional and high-dimensional Hilbert spaces, we propose an NCQT scheme that synchronously and probabilistically teleports N arbitrary unknown d-dimensional single-particle states from one sender to N different receivers under the supervision of a controller, by using a d-dimensional partially entangled (2N+1)-particle state as the quantum channel. The protocol succeeds if and only if all receivers recover their respective target states, and the optimal success probability of the N-output NCQT is determined by the minimum superposition coefficient of each product two-qudit state in the partially entangled channel. In our scheme, each receiver introduces an auxiliary qubit to assist in the local recovery test. When the auxiliary-qubit measurement outcome is |0⟩, the receiver can restore the target state; when the outcome is |1⟩, the corresponding unknown original state is retained by the sender. Accordingly, the N-output controlled teleportation process can be repeated as many times as additional quantum channels are available after a failed attempt. The results show that weakly entangled channels can still realize N-output controlled teleportation through sufficiently many repetitions, whereas strongly entangled channels require only a small number of repetitions to achieve the same goal.
Abstract Driven by the development of quantum communication networks toward multi-user and high-security scenarios, this paper investigates controlled cyclic teleportation (CCT) in high-dimensional systems with diverse control modes. Three peer-level control models and two hierarchical control models are investigated, each with three users and three controllers. The corresponding CCT protocols are designed by establishing suitable entangled channels from an initial nine-qudit state. Classical information encoding is skillfully employed to reduce the classical communication overhead. Under the authorization of the controllers, each sender can deterministically teleport an arbitrary single-qudit state to her adjacent receiver. The receivers’ recovery operations are given by general expressions that explicitly reveal the dependence on the measurement outcomes. In addition, we systematically analyze the influence of amplitude damping noise in the three-dimensional system and improve the fidelity using environment-assisted measurement (EAM). Given favorable environmental measurement outcomes and successful reversal operations, the EAM strategy can conditionally restore unit fidelity under the optimal reversal condition, with the corresponding success probability explicitly quantified. Compared with existing CCT protocols, the proposed protocols are applicable to arbitrary-dimensional quantum states, support richer control modes within a unified framework, and provide quantitatively characterized anti-noise performance.
Very recently, Lee et al. proposed a secure quantum teleportation protocol to transfer shared quantum secret between multiple parties in a network [Phys. Rev. Lett. 124 060501 (2020)]. This quantum network is encoded with a maximally entangled GHZ state. In this paper, we consider a partially entangled GHZ state as the entanglement channel, where it can achieve, probabilistically, unity fidelity transfer of the state. Two kinds of strategies are given. One arises when an auxiliary particle is introduced and a general evolution at any receiver’s location is then adopted. The other one involves performing a single generalized Bell-state measurement at the location of any sender. This could allow the receivers to recover the transmitted state with a certain probability, in which only the local Pauli operators are performed, instead of introducing an auxiliary particle. In addition, the successful probability is provided, which is determined by the degree of entanglement of the partially multipartite entangled state. Moreover, the proposed protocol is robust against the bit and phase flip noise.
Abstract In this contribution, we investigated the possibility of teleporting classical/quantum masked information, which may coded either in a single qubit or qutrit. For this purpose, different systems are used as quantum channels; two-qubit, three-qubit, two qutrit systems, and different protocols are applied. All the teleported masked information are retrieved as masked states at the receiver station. The number of operations that may be performed by the receiver are limited. It is shown that, one can teleport masked classical information with maximum fidelity, while for quantum information the maximization depends on the weight parameter of the tele-ported state. Teleporting the total masked state is better than teleporting its marginals, where the fidelity of total masked state is maximum. However, the fidelity of teleporting masking quantum information via three qubit systems may be maximized by controlling the weight of the initial masked state and the polarization of the mediator. In some cases, the receiver need to diagonalize the final teleported state to maximize its fidelity, and consequently reduces the required local operations.
Quantum teleportation is a fundamental protocol in quantum information science, whose performance is conventionally evaluated under the assumption of ideal Bell-state measurements. In realistic implementations, however, joint measurements are often imperfect and can deviate from maximally entangled bases due to coherent errors in entangling operations. In this work, we analytically show how the entanglement of joint measurements determines teleportation performance, and we propose a strategy to overcome the limitations imposed by partially entangled joint measurements to recover the unit teleportation fidelity with a nonzero success probability. This is achieved by optimizing a reversing operation on the teleported state to compensate for the known coherent deformation of the Bell-state measurement. We then derive an exact equation revealing a quantitative relation between measurement entanglement, channel entanglement, and the success probability to realize the unit-fidelity two-qubit teleportation. We illustrate our results using elegant joint measurements and realistic coherent error models arising from imperfect entangling operations in quantum systems. Our work provides fundamental insight into the role of measurement entanglement in quantum teleportation and offers a practical framework for achieving faithful teleportation without requiring substantial modifications to existing hardware.