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Pre-Phase A Report - Lisa - Nasa

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1.1 Theory of gravitational radiation 15<br />

terns of more complicated sources and detectors. For example, a binary star system will<br />

emit circularly polarised radiation along its orbital angular momentum axis, since from<br />

this direction its mass motions are circular. By contrast, it will emit linearly polarised<br />

radiation along directions in the orbital plane, since from these directions the transverse<br />

mass motions are simple linear oscillations.<br />

By measuring the degree of circular polarization in a wave and its orientation,<br />

LISA can determine the angle of inclination of a binary orbit, and even the<br />

direction of this inclination projected on the sky (to within a 90 ◦ ambiguity).<br />

This information cannot usually be obtained by conventional observations of binary systems,<br />

and is crucial to determining stellar masses. Note also that we see that the frequency<br />

of the gravitational radiation from a binary is twice the frequency of the orbital motion,<br />

since after half an orbital period the two stars have replaced one another and the mass<br />

distribution is the same as at the beginning. (This is true even if the stars have dissimilar<br />

masses, at least for the quadrupole radiation described below.)<br />

Similarly, LISA will be most sensitive to sources located along a line perpendicular to the<br />

plane containing its spacecraft, but it will have some sensitivity to sources in its plane.<br />

As LISA orbits the Sun, its orientation in space changes (see Chapter 3 and<br />

especially Section 4.4). This produces an amplitude modulation in a signal<br />

received from a long-lived source, which gives some information about its<br />

direction. Further directional information comes from LISA’s changing orbital<br />

velocity. This results in a Doppler-induced phase modulation that can, for<br />

sufficiently high frequencies, give very accurate positions.<br />

This is similar to the way radio astronomers determine precise pulsar positions using only<br />

single radio antennas with very broad antenna patterns. These issues are discussed in<br />

detail in Section 4.4 .<br />

For frequencies above about 3 mHz, LISA’s arm length is long enough that it can measure<br />

the differences between the arrival times of the gravitational wave at the different<br />

corners. This can in principle be used to triangulate positions on the sky, provided the<br />

telemetry returns enough information to extract these timing signals. Further study is required<br />

to determine whether the added information justifies providing the extra telemetry<br />

bandwidth.<br />

1.1.3 Generation of gravitational waves<br />

We mentioned above the different approximation methods that are used to decide how<br />

much radiation to expect from a given source. The simplest approximation, and the one<br />

that is used for most estimates, is the lowest-order post-Newtonian formula, called the<br />

“quadrupole formula”. Recall that the quadrupole radiation is the dominant radiation,<br />

because conservation of energy and momentum kill off monopole and dipole gravitational<br />

radiation. The interested reader can find a derivation of the quadrupole formula, using<br />

only the assumptions and mathematical level we have adopted here, in Reference [7].<br />

Corrected version 2.08 3-3-1999 9:33

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