Pre-Phase A Report - Lisa - Nasa
Pre-Phase A Report - Lisa - Nasa
Pre-Phase A Report - Lisa - Nasa
You also want an ePaper? Increase the reach of your titles
YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.
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