\begin{document}$ \left| 0 \right\rangle $\end{document} or \begin{document}$ \left| 1 \right\rangle $\end{document} or Bell states by the sender Alice. A sequence of single-photon states \begin{document}$ \left| 0 \right\rangle $\end{document} and \begin{document}$ \left| 1 \right\rangle $\end{document} and one photon from the Bell state mixed with decoy qubits is sent to the receiver Bob via a quantum channel. Bob obtains the final sifted compressed states \begin{document}$ \left| 0 \right\rangle $\end{document} and \begin{document}$ \left| 1 \right\rangle $\end{document} and conjugate transpose of the isometric tensors. Using our protocols, Bob can decompress the received states \begin{document}$ \left| 0 \right\rangle $\end{document} and \begin{document}$ \left| 1 \right\rangle $\end{document} into original entangled states. Since quantum processors that are used to send quantum information between nodes are relatively primitive and low in power and the preparation of many-photon entanglement is relatively difficult at present, finding suitable protocols for the compression of transmitted quantum data brings important practical benefits. More generally, the quantum information theory primarily investigates quantum data manipulation under locality constraints, so our protocols connect naturally to these investigations. Our protocols increase the encoding capacity of QKD protocols. Not only our proposed processes of compression and decompression are very simple, but also entanglement compression using isometric tensors can be implemented by using quantum circuits and current technology. Because many ideas for designing of quantum information processing equipment envision that a network composed of relatively small quantum processors sending quantum information between nodes, it is greatly significant to find appropriate protocols for compressing the transmitted quantum data ."> - 必威体育下载

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Citation:

    Lai Hong
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    • Abstract views:1895
    • PDF Downloads:58
    • Cited By:0
    Publishing process
    • Received Date:13 April 2023
    • Accepted Date:02 June 2023
    • Available Online:18 July 2023
    • Published Online:05 September 2023

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