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Anonymous transmission in a noisy quantum network using the W state: Difference between revisions
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Anonymous transmission in a noisy quantum network using the W state (edit)
Revision as of 07:24, 12 November 2021
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==Assumptions== | ==Assumptions== | ||
<!-- It describes the setting in which the protocol will be successful. --> | <!-- It describes the setting in which the protocol will be successful. --> | ||
The protocol relies on a set of classical subroutines (collision detection, receiver notification, veto and logical OR). Their proposed implementation [[Anonymous transmission in a noisy quantum network using the W state#References|[1] ]] has been shown to be information-theoretically secure in the classical regime, even with an arbitrary number of corrupted participants, assuming the parties share pairwise authenticated private channels and a broadcast channel. | The protocol relies on a set of classical subroutines (collision detection, receiver notification, veto and logical OR). Their proposed implementation [[Anonymous transmission in a noisy quantum network using the W state#References|[1]]] has been shown to be information-theoretically secure in the classical regime, even with an arbitrary number of corrupted participants, assuming the parties share pairwise authenticated private channels and a broadcast channel. | ||
The protocol assumes that the implementations listed above remain secure even in the presence of a quantum adversary. | The protocol assumes that the implementations listed above remain secure even in the presence of a quantum adversary. | ||
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==References== | ==References== | ||
# A. Broadbent and A. Tapp, inAdvances in Cryptology– ASIACRYPT 2007, edited by K. Kurosawa (Springer Berlin Heidelberg, Berlin, Heidelberg, 2007) pp. 410–426. | #A. Broadbent and A. Tapp, inAdvances in Cryptology– ASIACRYPT 2007, edited by K. Kurosawa (Springer Berlin Heidelberg, Berlin, Heidelberg, 2007) pp. 410–426. | ||