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Phys. Rev. D 67, 122003 (2003) [17 pages]

Implementation of time-delay interferometry for LISA

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Massimo Tinto*, Daniel A. Shaddock, Julien Sylvestre, and J. W. Armstrong§
Jet Propulsion Laboratory, California Institute of Technology, Pasadena, California 91109

Received 25 February 2003; published 11 June 2003

We discuss the baseline optical configuration for the Laser Interferometer Space Antenna (LISA) mission, in which the lasers are not free-running, but rather one of them is used as the main frequency reference generator (the master) and the remaining five as slaves, these being phase-locked to the master (the master-slave configuration). Under the condition that the frequency fluctuations due to the optical transponders can be made negligible with respect to the secondary LISA noise sources (mainly proof-mass and shot noises), we show that the entire space of interferometric combinations LISA can generate when operated with six independent lasers (the one-way method) can also be constructed with the master-slave system design. The corresponding hardware trade-off analysis for these two optical designs is presented, which indicates that the two sets of systems needed for implementing the one-way method, and the master-slave configuration, are essentially identical. Either operational mode could therefore be implemented without major implications on the hardware configuration. We then derive the required accuracies of armlength knowledge, time synchronization of the onboard clocks, sampling times and time-shifts needed for effectively implementing time-delay interferometry for LISA. We find that an armlength accuracy of about 16 meters, a synchronization accuracy of about 50 ns, and the time jitter due to a presently existing space qualified clock will allow the suppression of the frequency fluctuations of the lasers below to the level identified by the secondary noise sources. A new procedure for sampling the data in such a way to avoid the problem of having time shifts that are not integer multiples of the sampling time is also introduced, addressing one of the concerns about the implementation of time-delay interferometry.

© 2003 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevD.67.122003
DOI:
10.1103/PhysRevD.67.122003
PACS:
04.80.Nn, 07.60.Ly, 95.55.Ym

*Also at Space Radiation Laboratory, California Institute of Technology, Pasadena, CA 91125. Electronic address: Massimo.Tinto@ jpl.nasa.gov

Electronic address: Daniel.A.Shaddock@jpl.nasa.gov

Also at LIGO Laboratory, California Institute of Technology, Pasadena, CA 91125. Electronic address: jsylvest@ligo.caltech.edu

§Electronic address: John.W.Armstrong@jpl.nasa.gov