2005
DOI: 10.1103/physrevd.72.122003
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Relativistic analysis of the LISA long range optical links

Abstract: The joint ESA/NASA LISA mission consists in three spacecraft on heliocentric orbits, flying in a triangular formation of 5 Mkm each side, linked by infrared optical beams. The aim of the mission is to detect gravitational waves in a low frequency band. For properly processing the science data, the propagation delays between spacecraft must be accurately known. We thus analyse the propagation of light between spacecraft in order to systematically derive the relativistic effects due to the static curvature of th… Show more

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Cited by 19 publications
(31 citation statements)
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“…Thus physically the link measures an inaccurate combination of x SC , the relative displacement between SC and TM1, and the relative displacement x SC2 between SC and TM2. The differential interferometer signal is then o = (1 + δ SC )x SC − x SC2 and the effect of this cross-talk is the addition of an acceleration-like term δ SC (o SC − o nSC ) s 2 + ω 2 2 on the right-hand side of the second line of (5). If the coefficient δ SC has been measured then the following combination of signals [20]:…”
Section: Measurement Of Acceleration Noise and The Separation Of Sc Jmentioning
confidence: 99%
See 1 more Smart Citation
“…Thus physically the link measures an inaccurate combination of x SC , the relative displacement between SC and TM1, and the relative displacement x SC2 between SC and TM2. The differential interferometer signal is then o = (1 + δ SC )x SC − x SC2 and the effect of this cross-talk is the addition of an acceleration-like term δ SC (o SC − o nSC ) s 2 + ω 2 2 on the right-hand side of the second line of (5). If the coefficient δ SC has been measured then the following combination of signals [20]:…”
Section: Measurement Of Acceleration Noise and The Separation Of Sc Jmentioning
confidence: 99%
“…The relative frequency shift between emitter and receiver is [4,5] (1) is time varying. In LISA, for instance, the laser frequency shift oscillates at the frequency of the gravitational wave.…”
Section: Introductionmentioning
confidence: 99%
“…Indeed, at zeroth order in 1/c 2 , the nominal 5 million km armlength means 16.7 s of travel time; the flexing amplitude of 48000 km means 0.16 s fluctuation. At half order, the Sagnac and parallax effects amount to 960 km, that is 3 · 10 −3 s. While at first order, the Shapiro contribution, thanks to the supressing effect of LISA configuration, is less than 30 m, that is 10 −7 s, as we computed in [Chauvineau et al (2005)], with the classical orbit model. Now, we have shown that purely relativistic effects in orbits cause a correction up to 3 km in a period, meaning an effect of several milliseconds in the photon flight time at zeroth order in 1/c 2 .…”
Section: Orbit Model Comparisonmentioning
confidence: 68%
“…Hence, the need for LISA TDI simulators. We stress that coherence is needed, in those, between the photon time transfer model [Chauvineau et al (2005)], the orbit model, coordinates and timescales transformations [Pireaux (2007)]. We studied here the second point.…”
Section: Discussionmentioning
confidence: 99%
“…Both at the emitter and at the receiver, the frequency 1 of the light is measured in their relative rest frame. The difference of these two measurements is given by (Synge 1964;Chauvineau et al 2005):…”
Section: The Basic Element: the Doppler Linkmentioning
confidence: 99%