Answers are grounded in this paper and cite their sources.
A beacon organised by the transit law's phase steps is only as useful as the receiver that can find it: a narrowband, structured signal that must be acquired against Doppler uncertainty and noise. This paper specifies the companion receiver to such a beacon and computes its link performance end to end. With a 0.60-metre dish of gain 21.0 decibels and a system temperature of sixty kelvin, a forty-decibel-watt beacon gives a received power of -99.1 decibel-watts at one thousand kilometres, a signal-to-noise ratio of 111.7 decibels in one hertz; at one astronomical unit the received power is -202.6 decibel-watts and the ratio 8.2 decibels, above the ten-decibel detection requirement. A full Doppler search of plus or minus fifty kilohertz completes in 10 seconds. SIMULATED, NOT MEASURED: the receiver is specified and computed, and no beacon signal has been received.
No takes yet. Share an insight, caveat, or question.
William Alexander Aldred (2026) studied this question.
Synapse has enriched 8 closely related papers on similar clinical questions. Consider them for comparative context: