Covert Capacity of Bosonic Channels
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We investigate the quantum-secure covert-communication capabilities of lossy thermal-noise bosonic channels, the quantum-mechanical model for many practical channels. We determine the expressions for the covert capacity of these channels: $L_{\text{no-EA}}$, when Alice and Bob share only a classical secret, and $L_{\text{EA}}$, when they benefit from entanglement assistance. We find that entanglement assistance alters the fundamental scaling law for covert communication. Instead of $L_{\text{no-EA}}\sqrt{n}-r_{\text{no-EA}}(n)$, $r_{\text{no-EA}}(n)=o(\sqrt{n})$, entanglement assistance allows $L_{\text{EA}}\sqrt{n}\log n-r_{\text{EA}}(n)$, $r_{\text{EA}}(n)=o(\sqrt{n}\log n)$, covert bits to be transmitted reliably over $n$ channel uses.
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Cited by 2 Pith papers
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Covert Signaling for Communication and Sensing over the Bosonic Channels
Sparse signaling over bosonic channels minimizes detectability with a two-consecutive-photon-number mixture (vacuum plus single photon at low brightness), revealing power thresholds that trade covertness against commu...
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Covert Signaling for Communication and Sensing over the Bosonic Channels
The optimal input signal state for minimizing detectability in sparse covert signaling over bosonic channels is a mixture of two consecutive photon-number states, specifically vacuum and single photon in low-brightnes...
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