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Pre-Phase A Report - Lisa - Nasa

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44 Chapter 2 Different Ways of Detecting Gravitational Waves<br />

Figure 2.3 Conceptual design of the Gravitational Wave Interferometer<br />

(GWI). Left: GWI structure after deployment in low-Earth orbit. Right:<br />

Schematic of the interferometer system.<br />

shielded proof masses in three widely separated drag-free spacecraft, using laser transponders<br />

rather than mirrors at the ends of the interferometer arms to greatly reduce the shot<br />

noise. Both, the separated spacecraft and monolithic approaches were mentioned in a 1976<br />

committee report by Weiss et al. [73] and described by Weiss in a 1979 paper [74]. A more<br />

complete discussion of a possible separated spacecraft interferometer with 1×106 km arm<br />

lengths was given by Decher et al. [75] in 1980, but it required frequent major adjustments<br />

to the orbit of one spacecraft and had other disadvantages.<br />

The first suggestion of a mission using spacecraft orbits similar to those planned for LISA<br />

was made in 1981 by Faller and Bender [76, 77]. It included the appraoch suggested by<br />

Faller of using the apparent changes in length of one arm to determine the laser phase<br />

noise, and then correcting the arm length difference based on the measured laser phase<br />

noise. A full description of this concept, then tentatively named the Laser Antenna for<br />

Gravitational-radiation Observation in Space (LAGOS), was given by Faller [78].<br />

LAGOS had already many elements of the present-day LISA mission. It consisted of three<br />

drag-free satellites, one master spacecraft in the center and two auxilliary spacecraft at<br />

adistanceof106km from the central spacecraft, forming a triangle with an angle of<br />

120◦ at the central spacecraft (see Figure 2.4). This configuration would be placed in<br />

a circular heliocentric orbit at 1 AU from the Sun, about 4×107 km (15◦ ) ahead of the<br />

Earth. With 100 mW laser power and 50 cm diameter telescopes for transmitting and<br />

receiving the laser beams a strain sensitivity of δl/l =10−19 over the frequency range<br />

from 10−4 to 10−1 Hz appeared feasible. The proof masses in the spacecraft were thought<br />

to be cylinders of about 15 cm in length and diameter, freely floating inside a housing<br />

of 25 cm. Displacements of the housing by 10 µm with respect to the proof masses would<br />

3-3-1999 9:33 Corrected version 2.08

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