A building block of quantum repeaters for scalable quantum networks
Quantum networks, integrating quantum communication, quantum metrology, and distributed quantum computing, could provide secure and efficient information transfer, high-resolution sensing, and an exponential speed-up in information processing. Deterministic entanglement distribution over long distances is a prerequisite for scalable quantum networks, enabling the utilization of device-independent quantum key distribution (DI-QKD) and quantum teleportation to achieve secure and efficient information transfer. However, the exponential photon loss in optical fibres prohibits efficient and deterministic entanglement distribution. Quantum repeaters, incorporating entanglement swapping and entanglement purification with quantum memories, offer the most promising means to overcome this limitation in fibre-based quantum networks. Despite numerous pioneering efforts toward realizing quantum repeaters, a critical bottleneck remains, as remote memory-memory entanglement suffers from decoherence more rapidly than it can be established and purified over long distances. We overcome this by developing long-lived trapped-ion memories, an efficient telecom interface, and a high-visibility single-photon entanglement protocol. This allows us to establish and maintain memory-memory entanglement over a 10 km fibre within the average entanglement establishment time for the same distance. As a direct application, we demonstrate metropolitan-scale DI-QKD, distilling 1,917 secret keys out of 4.05*10^5 Bell pairs over 10 km. We further report a positive key rate over 101 km in the asymptotic limit, extending the achievable distance by more than two orders of magnitude. Our work provides a critical building block for quantum repeaters and marks an important step toward scalable quantum networks.
💡 Research Summary
Quantum networks promise secure communication, high‑resolution sensing, and exponential speed‑up for distributed computing, but their scalability hinges on deterministic entanglement distribution over long distances. Optical‑fiber loss grows exponentially with distance, making direct photon transmission infeasible for metropolitan or intercity scales. Quantum repeaters—nodes that store quantum states in memories, perform entanglement swapping, and apply purification—are the leading solution, yet a persistent bottleneck has been the rapid decoherence of remote memory‑memory entanglement, which typically decays faster than it can be generated and purified.
In this work the authors present a complete experimental platform that overcomes this limitation. They combine three key technologies: (1) long‑lived 40Ca⁺ ion qubits with coherence times exceeding 500 ms, (2) a low‑noise, high‑efficiency telecom interface based on periodically poled lithium niobate waveguides that converts 393 nm ion‑emitted photons to the 1550 nm band with 28 % overall transmission and background noise reduced to 35 counts s⁻¹, and (3) a single‑photon entanglement protocol (SPEP) together with wavelength‑division and time‑division multiplexing to actively stabilise the optical phase across up to 10 km of fiber.
Each node (Alice and Bob) houses a single ion prepared in the |↓⟩ state (99.9 % fidelity). A π‑pulse on the 729 nm transition lifts the ion to |↑⟩, followed by a short 854 nm pulse that partially transfers population back to |↓⟩, emitting a photon with a controllable excitation probability α. The photon is collected (≈9 % efficiency), coupled into single‑mode fiber, frequency‑converted, and sent to an intermediate station where interference on a beam‑splitter and detection by superconducting nanowire single‑photon detectors heralds entanglement. Phase fluctuations are cancelled by sending a continuous‑wave 1548 nm reference together with the quantum signal (WDM) and a weak 393 nm reference pulse (TDM), achieving an interference contrast of 0.986 ± 0.005 over 10 km.
Error sources—simultaneous excitation, ion gate and decoherence errors, spurious detector clicks, residual phase noise, and spin‑motion entanglement—are quantified and mitigated. By choosing α = 17 % the system reaches a heralded entanglement generation rate of 2.226 cps (average generation time 450 ms). At a lower excitation probability (α = 2.5 %) the Bell‑state fidelity reaches 0.923 ± 0.012. The authors further implement a storage protocol: after generation, the entangled state is transferred from the optical qubit to a long‑lived auxiliary level |s⟩ using Raman transitions, and a sequence of Knill dynamical decoupling pulses (interval 0.5 ms) protects the state. Measured ⟨XX⟩ decays exponentially with a coherence time of 8.55 ± 0.036 s (decoherence rate 1.8 Hz), yielding a quantum‑link efficiency (generation rate / decoherence rate) of 1.2, above the threshold for deterministic delivery. The average fidelity of a stored Bell pair at the moment a subsequent pair is generated is 0.578 ± 0.006, comfortably above the 0.5 limit required for swapping.
Leveraging this high‑fidelity, high‑rate entanglement, the authors demonstrate device‑independent quantum key distribution (DI‑QKD). Over a 10 km fiber they perform 405 145 experimental rounds (≈386 h of data collection). The CHSH parameter is S = 2.5758 ± 0.0059 and the quantum bit error rate (QBER) is 3.60 ± 0.06 %. After error correction (efficiency 1.122) and privacy amplification, 1 917 secret bits are distilled, corresponding to a per‑round key rate of ~4 × 10⁻³, which asymptotically approaches 0.325 per round. Extending the link to 101 km, they obtain S = 2.504 ± 0.075 and QBER = 6.9 ± 1.1 %, yielding an asymptotic key rate of 0.0974 per round—demonstrating a positive key rate at a distance more than two orders of magnitude beyond previous DI‑QKD experiments.
In summary, the paper delivers a functional building block for scalable quantum repeaters: long‑lived trapped‑ion memories, efficient telecom conversion, and phase‑stabilised single‑photon entanglement that together enable deterministic, high‑fidelity entanglement over metropolitan distances and practical DI‑QKD. The authors outline clear pathways for further scaling—using clock‑transition ion species or decoherence‑free subspaces to extend memory coherence, cavity‑enhanced photon collection to boost rates, and multi‑node network architectures—to ultimately achieve deterministic entanglement distribution across thousands of kilometres.
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