Covert Signaling for Communication and Sensing over the Bosonic Channels
2026-05-08 • Information Theory
Information Theory
AI summaryⓘ
The authors study how to send signals secretly over quantum channels without being detected, focusing on two main strategies: spreading out very weak signals or sending stronger signals but very rarely. They analyze the best way to prepare the signal in quantum states to minimize detection, finding that a simple mix of just two photon levels works best, especially mixing no photon and one photon states when the signal is very faint. Their work also explores how to balance staying hidden with maintaining good communication or sensing performance, identifying points where one goal becomes more important than the other. This helps in designing practical, low-power quantum communication systems.
covert communicationsquare-root lawsparse signalingbosonic channelsquantum statesphoton-number statesthermal noisequantum sensingsignal detectabilitylow-brightness regime
Authors
Tianrui Tan, Evan J. D. Anderson, Michael S. Bullock, Boulat A. Bash
Abstract
Preventing signal detection in communication and active sensing requires careful control of transmission power. In fact, the square-root laws (SRL) for covert classical and quantum communication and sensing prescribe that the average output power per channel use scales as $1/\sqrt{n}$ for $n$ channel uses. Two strategies for achieving this are diffuse and sparse signaling. The former transmits signals with power decaying as $1/\sqrt{n}$ on all $n$ channel uses, which is convenient for mathematical analysis. The latter transmits constant-power signals rarely, on approximately $\sqrt{n}$ out of $n$ channel uses, while remaining silent on the others. This offers significant practical advantages in compatibility with modern digital transmitters. Here, we study sparse signaling over lossy thermal-noise bosonic channels, which describe quantumly many practical channels (including optical, microwave, and radio-frequency). We characterize the input signal state that minimizes detectability. We find an unintuitive optimal quantum state structure: a mixture of just two consecutive photon-number states. In particular, in the low-brightness regime, the optimal signal state is a mixture of vacuum and a single photon. Since these states are generally suboptimal for both communication and active sensing, we explore the resulting trade-off and identify input-power thresholds for transitions between optimizing for covertness vs. performance in communication and sensing tasks.