Pre-Phase A Report - Lisa - Nasa
Pre-Phase A Report - Lisa - Nasa
Pre-Phase A Report - Lisa - Nasa
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4.4 Data analysis 105<br />
• LISA observes primarily long-lived sources, while ground-based detectors are expected<br />
to observe mainly bursts that are so short that frequency modulation is<br />
unimportant. LISA is able to find directions and polarisations primarily from the<br />
phase- and amplitude-modulation produced by its motion during an observation.<br />
Ground-based detectors will, of course, look for radiation from rotating neutron<br />
stars, and for this case the detection and signal reconstruction problem are similar<br />
to that for LISA, but LISA’s lower data rate and lower frequency makes the analysis<br />
considerably easier.<br />
• If LISA sees a gravitational wave background, it cannot identify it by crosscorrelation<br />
with another independent detector. We will show in Section 4.4.5 below<br />
how LISA can discriminate one background from another and from instrumental<br />
noise.<br />
In what follows we will consider in turn the methods used for data analysis and the<br />
expected manner and accuracy of extraction of the different kinds of information present<br />
in the signal.<br />
4.4.1 Data reduction and filtering<br />
Noise. The fundamental principle guiding the analysis of LISA data is that of matched<br />
filtering. Assuming that the LISA detector noise n(t) is stationary (an assumption that<br />
is only a first approximation, but which will have to be tested), the noise power can be<br />
characterised by its spectral density, defined as<br />
Sh(f) =<br />
∞<br />
−∞<br />
〈 n(t)n(t + τ) 〉 e −2πifτ , (4.56)<br />
where the autocorrelation of the noise 〈 n(t)n(t + τ) 〉 depends only on the offset time τ<br />
because the noise is stationary. The subscript “h” onSh refers to the gravitational wave<br />
amplitude, and it means that the detector output is assumed normalised and calibrated<br />
so that it reads directly the apparent gravitational wave amplitude.<br />
So far we have not assumed anything about its statistics, the probability density function<br />
(PDF) of the noise. It is conventional to assume it is Gaussian, since it is usually composed<br />
of several influences, and the central limit theorem suggests that it will tend to a Gaussian<br />
distribution. However, it can happen that at some frequenciesthe noise is dominated by<br />
a single influence, and then it can be markedly non-Gaussian. This has been seen in<br />
ground-based interferometers. An important design goal of LISA will be to ensure that<br />
the noise is mainly Gaussian, and during the analysis the characterisation of the noise<br />
statistics will be an important early step.<br />
Maximum likelihood and the matched filter. The most common way of assessing<br />
whether a signal of some expected form is present in a data stream is to use the maximum<br />
likelihood criterion, which is that one uses as the detection statistic the ratio of the probability<br />
that the given data would be observed if the signal were present to the probability<br />
that it would be observed if the signal were absent. This ratio has a PDF that depends<br />
on the PDF of the noise.<br />
Corrected version 2.08 3-3-1999 9:33