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(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

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Description of the LISA mission 127Figure 10.6. Early ONERA design of LISA free mass sensor call<strong>ed</strong> CAESAR. Up to fourcapacitor plates on each face of the housing around the test mass allow the relative positionand angular orientation to be measur<strong>ed</strong> accurately. Electrical forces also can be appli<strong>ed</strong>, ifdesir<strong>ed</strong>.After completion of the initial CAESAR design, additional studies of freemass sensor designs and of the LISA requirements have been carri<strong>ed</strong> out,influenc<strong>ed</strong> strongly by the CAESAR design. A number of the factors influencingthe design were discuss<strong>ed</strong> by Speake [19] and by Vitale and Speake [20]. A designwith a considerably different geometry for the capacitor plates was investigat<strong>ed</strong> byJosselin, Rodrigues and Touboul [21], and has since been construct<strong>ed</strong> and test<strong>ed</strong>in the laboratory and the LISA free mass sensor requirements were simplifi<strong>ed</strong> andsomewhat relax<strong>ed</strong> [6].One current version of the error allocation budget for the free mass sensoris describ<strong>ed</strong> in section 4.2.3 of [6]. The total acceleration error allow<strong>ed</strong> forone sensor is 3 × 10 −15 ms −2 /rtHz over the frequency range 0.1–30 mHz.The six largest allocations to individual error sources are as follows: thermaldistortion of the main spacecraft; temperature difference variations across the

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