This paper discussed the principles of operation and status of spacecraft Doppler tracking, the
current-generation GW detector technology in the
10–6 to 10–1 Hz band. Doppler tracking differs
from all other currently-operating detectors in that the size of the apparatus (earth-spacecraft
distance) is large compared with the GW wavelength. As a consequence times-of-flight of GWs and
radio waves through the apparatus are important, resulting in a three-pulse signal response and
various two-pulse noise responses. The different signal and noise transfer functions suggest data
analysis approaches for various waveforms; some of these approaches were outlined here. The
sensitivity of current-generation Doppler observations was discussed as well as what would be
required to improve this sensitivity by another order of magnitude (to
10–17 for sinusoidal
waves). Further large sensitivity improvements in the low-frequency band will require dedicated
multi-spacecraft arrays in space; ideas with their genesis in Doppler tracking will be used for
laser noise cancellation in these unequal-armlength arrays. Until such a dedicated mission flys,
spacecraft tracking will provide the best observational capability in the low-frequency GW
band.
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