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(23) The Doppler shift of the cyclotron frequency is included through a coordinate transformation to the retarded time [10]

Phase Finally, the instantaneous field phase at each antenna is given as the integral over all past instantaneous field frequencies: φj(t) = Z trj(t) 0 ωc(trj(t′)) dt′ +φc +ϕa(trj(

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Antenna Arrays for CRES-based Neutrino Mass Measurement

physics.ins-det · 2025-04-21 · accept · novelty 5.0

An antenna-array readout for cyclotron radiation emission spectroscopy can in principle reach a 40 meV neutrino mass sensitivity, supported by bench-scale array measurements.

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  • Antenna Arrays for CRES-based Neutrino Mass Measurement physics.ins-det · 2025-04-21 · accept · none · ref 3

    An antenna-array readout for cyclotron radiation emission spectroscopy can in principle reach a 40 meV neutrino mass sensitivity, supported by bench-scale array measurements.