The original version of this Article contained errors in the Competing interests statement and Table 1 and incorrectly omitted the Acknowledgements section. The original Competing interests statement reported no competing interests for the authors; this has been corrected to “B.H. and F.F. are employees of ID Quantique, Geneva and ID Quantique Europe, Vienna, respectively, which have competing interests with Arqit in developing quantum communication technologies. B.T. is an employee of Thales Alenia Space, a joint Venture which invests in satellite quantum communications. B.H. is the inventor of several patents, both pending and accepted, in the field of space QKD. The authors declare that there are no other competing interests”. The original Table 1 omitted the captions. Table 1 captions read: The different steps of the protocol are described below, each item corresponding to the numbered row in the Table. 1. Alice prepares a series of quantum states, according to BB84 polarisation protocol. For each state, she chooses both the bit value and the corresponding basis. She sends the states to Bob over a quantum channel (arrow with diagonal stripes). 2. Many states are lost in the transmission. Bob tells Alice, which states have been lost (X in the table). He uses the classical discussion channel (white arrow). Alice and Bob discard all the corresponding states. The resulting series of bits is the raw key. 3. Alice tells Bob, over the classical discussion channel, which bases she used. Bob notes the cases when he and Alice used different bases (X in the table), but does not tell Alice. The remaining bits represent the sifted key for Bob. Alice cannot know, which of the states were received by Bob in the correct basis. 4. to 6. Alice and Carol follow the same protocol with a new series of states. 7. Alice performs an XOR of the two raw keys she exchanged with Bob and with Carol and sends the result to Carol, over the classical discussion channel. 8. Bob sends directly to Carol, which bits he received in the wrong basis and should not be used (X in the table). He uses a confidential classical channel, “which cannot be eavesdropped by Alice” (black arrow). 9. Carol notes the wrong bits in the XORed key. 10. Carol makes an XOR of the two sifted keys, and sends to Bob, which bits should not be used (X in the table). She also uses the same confidential classical channel, “which cannot be eavesdropped by Alice”. 11. Bob and Carol now share a common sifted key, unknown to Alice. They can process it in the standard way (error estimation, error correction, privacy amplification) to finally get a shared secret key. The main hypothesis of the protocol is that Bob and Carol share a confidential classical channel, which cannot be eavesdropped by Alice. The correct Acknowledgements read: B.H., R.A., E.D., F.F., P.G., H.H., V.M., A.P., J.A.S., A.W. and H.Z. acknowledge support from the H2020-funded research project OPENQKD, Grant agreement contract number 857156, https://openqkd.eu/. This has now been corrected in both the PDF and HTML versions of the Article.@en

Long optical storage times are an essential requirement to establish high-rate entanglement distribution over large distances using memory-based quantum repeaters. Rare earth ion-doped crystals are arguably well-suited candidates for building such quantum memories. Toward this end, we investigate the 795.32 nm 3H6 ↔ 3H4 transition of 1% thulium-doped yttrium gallium garnet crystal (Tm3+:Y3Ga5O12 : Tm3+:YGG). Most essentially, we find that the optical coherence time can reach 1.1 ms, and, using laser pulses, we demonstrate optical storage based on the atomic frequency comb (AFC) protocol up to 100 µs. In addition, we demonstrate multiplexed storage, including feed-forward selection, shifting, and filtering of spectral modes, as well as quantum state storage using members of non-classical photon pairs. Our results show that Tm:YGG can be a potential candidate for creating multiplexed quantum memories with long optical storage times.@en

We argue that long optical storage times are required to establish entanglement at high rates over large distances using memory-based quantum repeaters. Triggered by this conclusion, we investigate the 795.325 nm3 H6↔H34 transition of Tm:Y3Ga5O12 (Tm:YGG). Most importantly, we find that the optical coherence time can reach 1.1 ms, and, using laser pulses, we demonstrate optical storage based on the atomic frequency comb protocol during up to 100 μs as well as a memory decay time Tm of 13.1 μs. Possibilities of how to narrow the gap between the measured value of Tm and its maximum of 275 μs are discussed. In addition, we demonstrate multiplexed storage, including with feed-forward selection, shifting and filtering of spectral modes, as well as quantum state storage using members of nonclassical photon pairs. Our results show the potential of Tm:YGG for creating multiplexed quantum memories with long optical storage times, and open the path to repeater-based quantum networks with high entanglement distribution rates.@en

The forthcoming quantum Internet is poised to allow new applications not possible with the conventional Internet. The ability for both quantum and conventional networking equipment to coexist on the same fiber network would facilitate the deployment and adoption of coming quantum technology. Most quantum networking tasks, like quantum repeaters and the connection of quantum processors, require nodes for multi-qubit quantum measurements (often Bell-State measurements), and their real-world coexistence with the conventional Internet has yet to be shown. Here we field deploy a Measurement-Device Independent Quantum Key Distribution (MDI-QKD) system, containing a Bell-State measurement node, over the same fiber connection as multiple standard Internet Protocol (IP) data networks, between three nearby cities in the Netherlands. We demonstrate over 10 Gb/s classical data communication rates simultaneously with our next-generation QKD system, and estimate 200 GB/s of classical data transmission would be easily achievable without significantly affecting QKD performance. Moreover, as the system ran autonomously for two weeks, this shows an important step towards the coexistence and integration of quantum networking into the existing telecommunication infrastructure.@en

In this work, we fabricate a multimode quantum memory out of a thulium-doped crystal and demonstrate storage of laser pulses of up to 100 µsec. A significant step forward for creating quantum memories with long optical storage times.@en