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arXiv:2610.38817

Memory-Induced Limits on Entanglement Distribution

Roberto Benjamin Salazar Vargas, Hayden Zammit, Trevor Spiteri, Gianluca Valentino, Tony J. G. Apollaro, Johann A. Briffa

quant-phSubmitted Oct 28, 2026• Announced Oct 30, 2026• 0 citations
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Abstract

We investigate the operational limits of entanglement distribution through quantum channels reused without reinitialization. Building on an effective repeated-use channel description, we show that residual excitations left in the channel from previous uses act as a memory source that progressively suppresses coherent quantum transmission. To quantify this limitation, we derive an analytical lower bound on the quantum capacity and combine it with the Holevo-Werner semidefinite-programming upper bound. We also provide an analytical criterion to identify entanglement-breaking channels, with thresholds that depend jointly on chain length and reuse. For perfect-state-transfer chains, the resulting capacity window yields tighter estimates than previous bounds, with the relative improvement becoming substantially more pronounced closer to the entanglement-breaking threshold. Moreover, on the second use, our lower bound certifies a maximal relative timing-error tolerance across all chains with internal memory that lies just below 22.63% and is attained by the three-site chain. We further derive a fundamental relative timing-error threshold of 36.41%, above which we analytically guarantee zero unassisted quantum capacity for every chain with internal memory, independent of the number of uses. These results establish a clear benchmark model for repeated entanglement distribution, and identify timing precision, chain length, and memory accumulation as fundamental constraints on scalable quantum-network architectures.

AI Summary

The paper asks how residual excitations affect entanglement distribution when a spin-chain communication channel is reused without resetting its internal sites. It studies an existing effective-channel model for $U(1)$-symmetric quadratic-fermion dynamics, averaging over previous pure inputs. Each use gives a qubit channel comprising dephasing and generalized amplitude damping. The capacity analyzed is that of independent realizations of this fixed, averaged marginal channel—not the capacity of the correlated physical sequence. An analytical achievable-rate expression is obtained by maximizing coherent information over diagonal inputs. A geometric Rényi/PPT semidefinite-programming hierarchy supplies upper bounds, evaluated through level $l=10$ and compared with a previous damping/dephasing bottleneck bound. The exact entanglement-breaking condition is $(1-\gamma_n)(1-\lambda_n)\leq\gamma_n^2p_n(1-p_n)$, from positivity under partial transpose of the two-qubit Choi state. For engineered perfect-state-transfer chains with identical readout timing errors, $\gamma^{(N)}=1-\cos^{2(N-1)}(\pi\delta/2)$. Damping-induced antidegradability guarantees zero unassisted capacity above $\delta_*(N)=\frac{2}{\pi}\arccos(2^{-1/[2(N-1)]})$. For all chains with internal memory ($N\geq3$), the largest such threshold is $36.4057\%$. On the second use, the largest timing-error tolerance certified by the lower bound is $22.6243\%$, attained at $N=3$; its value is numerically optimized, while optimality across lengths is established analytically. Numerical landscapes for $N=3$–$10$ and uses $2$–$16$ track shrinking positive-capacity certification and entanglement-breaking boundaries. Intermediate regions remain unresolved. The conclusions exclude collective coding across physical uses and access to internal memory; they do not rule out recovery through memory control or active reset.

Some signs of AI-generated textIncrementalStrong assumptionsOverclaims

Error found: The claimed zero-capacity guarantee for every timing error above 36.41% requires a restricted domain such as δ∈[0,1], since δ=2 gives perfect transfer again. The abstract's universal-sounding numerical thresholds are established only for the specified engineered spin-chain family with equal readout durations, not for arbitrary chains with internal memory. Appendix B omits square roots in the dephasing Kraus amplitudes, making the printed Kraus representation non-trace-preserving, although its final lower-bound spectrum is correct. Appendix C prints an incorrect weighted geometric-mean definition that gives I instead of X at exponent zero.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
19 pages, 8 figures

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We investigate the operational limits of entanglement distribution through quantum channels reused without reinitialization. Building on an effective repeated-use channel description, we show that residual excitations left in the channel from previous uses act as a memory source that progressively suppresses coherent quantum transmission. To quantify this limitation, we derive an analytical lower bound on the quantum capacity and combine it with the Holevo-Werner semidefinite-programming upper bound. We also provide an analytical criterion to identify entanglement-breaking channels, with thresholds that depend jointly on chain length and reuse. For perfect-state-transfer chains, the resulting capacity window yields tighter estimates than previous bounds, with the relative improvement becoming substantially more pronounced closer to the entanglement-breaking threshold. Moreover, on the second use, our lower bound certifies a maximal relative timing-error tolerance across all chains with internal memory that lies just below 22.63% and is attained by the three-site chain. We further derive a fundamental relative timing-error threshold of 36.41%, above which we analytically guarantee zero unassisted quantum capacity for every chain with internal memory, independent of the number of uses. These results establish a clear benchmark model for repeated entanglement distribution, and identify timing precision, chain length, and memory accumulation as fundamental constraints on scalable quantum-network architectures.
The paper asks how residual excitations affect entanglement distribution when a spin-chain communication channel is reused without resetting its internal sites. It studies an existing effective-channel model for U(1)U(1)U(1)-symmetric quadratic-fermion dynamics, averaging over previous pure inputs. Each use gives a qubit channel comprising dephasing and generalized amplitude damping. The capacity analyzed is that of independent realizations of this fixed, averaged marginal channel—not the capacity of the correlated physical sequence.
An analytical achievable-rate expression is obtained by maximizing coherent information over diagonal inputs. A geometric Rényi/PPT semidefinite-programming hierarchy supplies upper bounds, evaluated through level l=10l=10l=10 and compared with a previous damping/dephasing bottleneck bound. The exact entanglement-breaking condition is (1−γn)(1−λn)≤γn2pn(1−pn)(1-\gamma_n)(1-\lambda_n)\leq\gamma_n^2p_n(1-p_n)(1−γn​)(1−λn​)≤γn2​pn​(1−pn​), from positivity under partial transpose of the two-qubit Choi state.
For engineered perfect-state-transfer chains with identical readout timing errors, γ(N)=1−cos⁡2(N−1)(πδ/2)\gamma^{(N)}=1-\cos^{2(N-1)}(\pi\delta/2)γ(N)=1−cos2(N−1)(πδ/2). Damping-induced antidegradability guarantees zero unassisted capacity above δ∗(N)=2πarccos⁡(2−1/[2(N−1)])\delta_*(N)=\frac{2}{\pi}\arccos(2^{-1/[2(N-1)]})δ∗​(N)=π2​arccos(2−1/[2(N−1)]). For all chains with internal memory (N≥3N\geq3N≥3), the largest such threshold is 36.4057%36.4057\%36.4057%. On the second use, the largest timing-error tolerance certified by the lower bound is 22.6243%22.6243\%22.6243%, attained at N=3N=3N=3; its value is numerically optimized, while optimality across lengths is established analytically.
Numerical landscapes for N=3N=3N=3–101010 and uses 222–161616 track shrinking positive-capacity certification and entanglement-breaking boundaries. Intermediate regions remain unresolved. The conclusions exclude collective coding across physical uses and access to internal memory; they do not rule out recovery through memory control or active reset.
Reliable distribution of quantum entanglement over long distances is a central challenge in quantum information science, fundamentally limited by decoherence in noisy communication channels. In this work, we investigate the asymptotic limits of entanglement distribution across homogeneous linear repeater chains with arbitrary intermediate LOCC processing. We establish a strict dichotomy: the asymptotic preservation of entanglement over arbitrarily long distances is possible if and only if the underlying quantum channel admits a correctable subspace. For channels lacking such a subspace, we prove that the transmitted state converges exponentially fast to the set of separable states, rendering standard LOCC filtering insufficient. To counteract this exponential degradation, we analyze ``networks'' employing parallel channel uses per link. We derive a fundamental lower bound on the required number of parallel channel uses per elementary link, proving that for broad classes of channels without a correctable subspace, the number of parallel channels per link must scale at least logarithmically with the number of intermediate stations to sustain a non-zero amount of entanglement. This provides a code-independent bound for the number of physical links for the considered homogeneous one-way architecture. For depolarizing noise below the corresponding coding threshold, the logarithmic lower bound is achievable.
In this paper we study quantum communication channels with correlated noise effects, i.e., quantum channels with memory. We derive a model for correlated noise channels that includes a channel memory state. We examine the case where the memory is finite, and derive bounds on the classical and quantum capacities. For the entanglement-assisted and unassisted classical capacities it is shown that these bounds are attainable for certain classes of channel. Also, we show that the structure of any finite-memory state is unimportant in the asymptotic limit, and specifically, for a perfect finite-memory channel where no information is lost to the environment, achieving the upper bound implies that the channel is asymptotically noiseless.
We consider quantum and private communications assisted by repeaters, from the basic scenario of a single repeater chain to the general case of an arbitrarily-complex quantum network, where systems may be routed through single or multiple paths. In this context, we investigate the ultimate rates at which two end-parties may transmit quantum information, distribute entanglement, or generate secret keys. These end-to-end capacities are defined by optimizing over the most general adaptive protocols that are allowed by quantum mechanics. Combining techniques from quantum information and classical network theory, we derive single-letter upper bounds for the end-to-end capacities in repeater chains and quantum networks connected by arbitrary quantum channels, establishing exact formulas under basic decoherence models, including bosonic lossy channels, quantum-limited amplifiers, dephasing and erasure channels. For the converse part, we adopt a teleportation-inspired simulation of a quantum network which leads to upper bounds in terms of the relative entropy of entanglement. For the lower bounds we combine point-to-point quantum protocols with classical network algorithms. Depending on the type of routing (single or multiple), optimal strategies corresponds to finding the widest path or the maximum flow in the quantum network. Our theory can also be extended to simultaneous quantum communication between multiple senders and receivers.
Long-distance entanglement distribution requires error correction protocols to compensate for qubit decoherence in quantum memories and noise introduced during entanglement swapping. We argue that repeater chains with error-correction capabilities should exploit more than one physical platform, combining the complementary strengths of different quantum memory technologies into a single hybrid repeater architecture. An important constituent of such an architecture is a hybrid repeater which combines type-1 memories, characterized by fast entanglement generation rates and suitability for multiplexing, and type-2 memories that offer long coherence times and low two-qubit gate error rates. Taking the resource-intensive nature of hybrid nodes into account, we propose and analyze repeater chains in which only a subset of nodes need to be hybrid, while the remaining nodes are simpler first-generation repeaters with no error-correction capability. Through detailed Monte Carlo simulations of fault-tolerant encoded repeater chain protocols based on the three-qubit phase-flip repetition code, the [[7,1,3]][[7,1,3]][[7,1,3]] Steane code, and the [[9,1,3]][[9,1,3]][[9,1,3]] Shor code, we demonstrate that these hybrid architectures outperform pure architectures based on a single memory platform in terms of end-to-end entanglement distribution rate. In our study we develop a full circuit-level noise model of our architectures and examine the impact of an imperfect interface between the two platforms on our hybrid architecture. We also develop a modified version of the swap-as-soon-as-possible policy with multiplexing, more suited to our architecture where some nodes perform error-correction while others do not. This modified policy significantly reduces the information storage time in memory qubits relative to the previously considered swap policies in encoded repeater chains.
The throughput is an important performance metric of entangled qubit distribution quantum networks, and may be characterized by the number of distributed entangled qubit pairs per second (ebps). It is measured over physical quantum network connections using specialized instruments, including photonic entanglement sources and single photon detectors. Extensive theory has been developed to estimate the entangled qubit capacity of quantum channels using abstractions of physical connections. These two quantities both characterize the throughput performance but in different ways, and typically have been hard to relate to each other in concrete terms, in part due to the lack of precise measurements with matching analytical models and derivations. We describe measurements on a physical testbed with fiber connections of lengths 0-75 kilometers. We obtain the normalized analytic capacity estimates using the transmissivity approximations derived using single photon coincidence measurements, and convert them to bounds on throughput (measured in ebps) using a multiplier derived from co-located detector measurements. The results indicate consistent throughput measurements upper-bounded by their analytical capacity estimates across all connections. We show that previous capacity estimates using light measurements are below ebps measurements for some connections, due to the inclusion of non-representative decrease of light levels outside C-band with distance.
In quantum mechanics, a fundamental law prevents quantum communications to simultaneously achieve high rates and long distances. This limitation is well known for point-to-point protocols, where two parties are directly connected by a quantum channel, but not yet fully understood in protocols with quantum repeaters. Here we solve this problem bounding the ultimate rates for transmitting quantum information, entanglement and secret keys via quantum repeaters. We derive single-letter upper bounds for the end-to-end capacities achievable by the most general (adaptive) protocols of quantum and private communication, from a single repeater chain to an arbitrarily complex quantum network, where systems may be routed through single or multiple paths. We analytically establish these capacities under fundamental noise models, including bosonic loss which is the most important for optical communications. In this way, our results provide the ultimate benchmarks for testing the optimal performance of repeater-assisted quantum communications.