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Multicopy quantum state teleportation with application to storage and retrieval of quantum programs

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⚡ Quantum Brief
Researchers developed a correction-free quantum teleportation protocol where Alice uses multiple identical copies of an unknown quantum state to transmit a single perfect copy to Bob without requiring Bob to perform corrections. The protocol achieves a success probability of p(d,k) = k/(d(k-1+d)), where k is the number of copies and d is the quantum system’s dimension, proving that more copies increase success rates. Alice performs a joint measurement on k copies of the state and her half of a maximally entangled qudit pair, sending Bob only a binary success/failure message. This method enhances quantum program storage and retrieval, improving the probability of recovering and applying stored quantum operations to target states. The team’s use of group representation theory suggests broader applications for quantum information tasks involving multiple state copies.
Multicopy quantum state teleportation with application to storage and retrieval of quantum programs

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AbstractThis work considers a teleportation task for Alice and Bob in a scenario where Bob cannot perform corrections. In particular, we analyse the task of $\textit{multicopy state teleportation}$, where Alice has $k$ identical copies of an arbitrary unknown $d$-dimensional qudit state $\vert\psi\rangle$ to teleport a single copy of $\vert\psi\rangle$ to Bob using a maximally entangled two-qudit state shared between Alice and Bob without Bob's correction. Alice may perform a joint measurement on her half of the entangled state and the $k$ copies of $\vert\psi\rangle$. We prove that the maximal probability of success for teleporting the exact state $\vert\psi\rangle$ to Bob is $p(d,k)=\frac{k}{d(k-1+d)}$ and present an explicit protocol to attain this performance. Then, by utilising $k$ copies of an arbitrary target state $\vert\psi\rangle$, we show how the multicopy state teleportation protocol can be employed to enhance the success probability of storage and retrieval of quantum programs, which aims to universally retrieve the action of an arbitrary quantum channel that is stored in a state. Our proofs make use of group representation theory methods, which may find applications beyond the problems addressed in this work.Featured image: Pictorial illustration of the teleportation scenario considered in this work. Alice and Bob share one pair of a maximally entangled qudit state $|\phi_d^+\rangle$ and Alice has $k$ copies of an arbitrary qudit $|{\psi}\rangle$. In order to teleport the state $|{\psi}\rangle$ to Bob, Alice performs a joint measurement $M$ on all quantum states on her side. We consider the case where Bob probabilistically receives a single copy of $|{\psi}\rangle$ without any corrections, hence Alice's measurement outcome may be assumed to be dichotomic, where one measurement outcome corresponds to success, where Bob receives the exact state $|\psi\rangle$ with probability $p(d,k)$, and a failure case where Bob receives a quantum state which is not $|\psi\rangle$.Popular summaryTeleporting Quantum States Without Corrections: The Power of Multiple Copies Quantum teleportation allows two parties, referred to as Alice and Bob, to transmit a quantum state without having access to a quantum channel, but by consuming quantum entanglement. In standard quantum teleportation, Bob must perform a "correction step" based on classical information sent by Alice to recover the exact quantum state. For some applications, this correction step does not pose any issue, Bob may just perform a local correction that will depend on Alice’s classical message. However, this correction step causes problems for certain advanced tasks. In particular, it prevents us from using standard teleportation to store a "quantum program" (a quantum operation) and later retrieve it to apply to a new state. While alternative methods like "Port-Based Teleportation" can work without corrections, they require access to a large entangled resource. In our paper, we explore a new scenario: what happens if Alice and Bob still only share a single pair of entangled particles, but Alice has access to multiple identical copies (let's call the number of copies k) of the unknown quantum state she wants to send? We discovered that Alice can process all k copies together by performing a joint measurement. By doing this, she can improve the success probability of successfully teleport a single, perfect copy of the state to Bob without him needing to perform any correction at all. In a nutshell, Alice performs a joint measurement on her side and sends a single bit of information to Bob—essentially a simple "success" or "failure" message. When the protocol succeeds, Bob holds the exact intended quantum state. We mathematically proved that the highest possible probability of success is exactly $p(d,k)=k/(d(k−1+d))$, where d is the dimension of the quantum system to be teleported. This formula shows a clear advantage: the more copies Alice starts with, the higher the chance of a perfect, correction-free teleportation. This multicopy teleportation protocol can be directly applied to improve the storage and retrieval of quantum programs. When a user wants to retrieve a stored quantum operation and apply it to a target state, having multiple copies of that target state enhances the probability of successfully retrieving the program. From a broader perspective, the methods and approach of this work may find applications in other tasks where one may have access to multiple copies of a target state.► BibTeX data@article{Grosshans2026multicopyquantum, doi = {10.22331/q-2026-05-13-2105}, url = {https://doi.org/10.22331/q-2026-05-13-2105}, title = {Multicopy quantum state teleportation with application to storage and retrieval of quantum programs}, author = {Grosshans, Fr{\'{e}}d{\'{e}}ric and Horodecki, Micha{\l{}} and Murao, Mio and M{\l{}}ynik, Tomasz and Quintino, Marco T{\'{u}}lio and Studzi{\'{n}}ski, Micha{\l{}} and Yoshida, Satoshi}, journal = {{Quantum}}, issn = {2521-327X}, publisher = {{Verein zur F{\"{o}}rderung des Open Access Publizierens in den Quantenwissenschaften}}, volume = {10}, pages = {2105}, month = may, year = {2026} }► References [1] C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres, and W. K. 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AbstractThis work considers a teleportation task for Alice and Bob in a scenario where Bob cannot perform corrections. In particular, we analyse the task of $\textit{multicopy state teleportation}$, where Alice has $k$ identical copies of an arbitrary unknown $d$-dimensional qudit state $\vert\psi\rangle$ to teleport a single copy of $\vert\psi\rangle$ to Bob using a maximally entangled two-qudit state shared between Alice and Bob without Bob's correction. Alice may perform a joint measurement on her half of the entangled state and the $k$ copies of $\vert\psi\rangle$. We prove that the maximal probability of success for teleporting the exact state $\vert\psi\rangle$ to Bob is $p(d,k)=\frac{k}{d(k-1+d)}$ and present an explicit protocol to attain this performance. Then, by utilising $k$ copies of an arbitrary target state $\vert\psi\rangle$, we show how the multicopy state teleportation protocol can be employed to enhance the success probability of storage and retrieval of quantum programs, which aims to universally retrieve the action of an arbitrary quantum channel that is stored in a state. Our proofs make use of group representation theory methods, which may find applications beyond the problems addressed in this work.Featured image: Pictorial illustration of the teleportation scenario considered in this work. Alice and Bob share one pair of a maximally entangled qudit state $|\phi_d^+\rangle$ and Alice has $k$ copies of an arbitrary qudit $|{\psi}\rangle$. In order to teleport the state $|{\psi}\rangle$ to Bob, Alice performs a joint measurement $M$ on all quantum states on her side. We consider the case where Bob probabilistically receives a single copy of $|{\psi}\rangle$ without any corrections, hence Alice's measurement outcome may be assumed to be dichotomic, where one measurement outcome corresponds to success, where Bob receives the exact state $|\psi\rangle$ with probability $p(d,k)$, and a failure case where Bob receives a quantum state which is not $|\psi\rangle$.Popular summaryTeleporting Quantum States Without Corrections: The Power of Multiple Copies Quantum teleportation allows two parties, referred to as Alice and Bob, to transmit a quantum state without having access to a quantum channel, but by consuming quantum entanglement. In standard quantum teleportation, Bob must perform a "correction step" based on classical information sent by Alice to recover the exact quantum state. For some applications, this correction step does not pose any issue, Bob may just perform a local correction that will depend on Alice’s classical message. However, this correction step causes problems for certain advanced tasks. In particular, it prevents us from using standard teleportation to store a "quantum program" (a quantum operation) and later retrieve it to apply to a new state. While alternative methods like "Port-Based Teleportation" can work without corrections, they require access to a large entangled resource. In our paper, we explore a new scenario: what happens if Alice and Bob still only share a single pair of entangled particles, but Alice has access to multiple identical copies (let's call the number of copies k) of the unknown quantum state she wants to send? We discovered that Alice can process all k copies together by performing a joint measurement. By doing this, she can improve the success probability of successfully teleport a single, perfect copy of the state to Bob without him needing to perform any correction at all. In a nutshell, Alice performs a joint measurement on her side and sends a single bit of information to Bob—essentially a simple "success" or "failure" message. When the protocol succeeds, Bob holds the exact intended quantum state. We mathematically proved that the highest possible probability of success is exactly $p(d,k)=k/(d(k−1+d))$, where d is the dimension of the quantum system to be teleported. This formula shows a clear advantage: the more copies Alice starts with, the higher the chance of a perfect, correction-free teleportation. This multicopy teleportation protocol can be directly applied to improve the storage and retrieval of quantum programs. When a user wants to retrieve a stored quantum operation and apply it to a target state, having multiple copies of that target state enhances the probability of successfully retrieving the program. From a broader perspective, the methods and approach of this work may find applications in other tasks where one may have access to multiple copies of a target state.► BibTeX data@article{Grosshans2026multicopyquantum, doi = {10.22331/q-2026-05-13-2105}, url = {https://doi.org/10.22331/q-2026-05-13-2105}, title = {Multicopy quantum state teleportation with application to storage and retrieval of quantum programs}, author = {Grosshans, Fr{\'{e}}d{\'{e}}ric and Horodecki, Micha{\l{}} and Murao, Mio and M{\l{}}ynik, Tomasz and Quintino, Marco T{\'{u}}lio and Studzi{\'{n}}ski, Micha{\l{}} and Yoshida, Satoshi}, journal = {{Quantum}}, issn = {2521-327X}, publisher = {{Verein zur F{\"{o}}rderung des Open Access Publizierens in den Quantenwissenschaften}}, volume = {10}, pages = {2105}, month = may, year = {2026} }► References [1] C. H. Bennett, G. Brassard, C. Crépeau, R. Jozsa, A. Peres, and W. K. Wootters, Teleporting an unknown quantum state via dual classical and einstein-podolsky-rosen channels, Phys. Rev. Lett. 70, 1895–1899 (1993). https:/​/​doi.org/​10.1103/​PhysRevLett.70.1895 [2] H.-J. Briegel, W. Dür, J. I. Cirac, and P. Zoller, Quantum repeaters: The role of imperfect local operations in quantum communication, Phys. Rev. Lett. 81, 5932–5935 (1998), arXiv:quant-ph/​9803056 [quant-ph]. https:/​/​doi.org/​10.1103/​PhysRevLett.81.5932 arXiv:quant-ph/9803056 [3] D. Gottesman and I. L. Chuang, Demonstrating the viability of universal quantum computation using teleportation and single-qubit operations, Nature 402, 390–393 (1999a), arXiv:quant-ph/​9908010 [quant-ph]. https:/​/​doi.org/​10.1038/​46503 arXiv:quant-ph/9908010 [4] C. H. Bennett, D. P. Divincenzo, J. A. Smolin, and W. K. Wootters, Mixed-state entanglement and quantum error correction, Phys. Rev. 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