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Time series analysis in the frequency domain

  For the detection of smooth signals, e.g. sinusoids, use either SCARGLE/TSA or AOV/TSA with bins. The sensitivity of these statistics to sharp signals (such as strongly pulsed variations or light curves of very wide eclipsing binaries) is poor. For the detection of such signals better use AOV/TSA with a bin width matching the width of these features.

The command SINEFIT/TSA serves two purposes: a) least squares estimation of the parameters of a detected signal and b) filtering the data for a given frequency (so-called prewhitening). The trend removal (zero frequency) constitutes a special case of this filtering. For a pure sinusoid model, the statistic used in SINEFIT/TSA is related to that used in SCARGLE/TSA (Lomb, 1976, Scargle, 1982).

SCARGLE/TSA --
Scargle sine model: This command computes Scargle's (1982) periodogram for unevenly spaced observations x. The Scargle statistic uses a pure sine model and is a special case of the power spectrum statistic normalized to the variance of the raw data,
. The phase origins of the sinusoids are for each frequency chosen in such a way that the sine and cosine components of become independent. Hence for white noise ( hypothesis) S is the ratio of and . For large numbers of observations , numerator and denominator become uncorrelated so that S has a Fisher-Snedecor distribution approaching an exponential distribution in the asymptotic limit: for .

We recommend this statistic for larger data sets and for the detection of smooth, nearly sinusoidal signals, since then its test power is large and the statistical properties are known. In particular the expected value is 1. For observations correlated in groups of size , divide the value of the Scargle statistics by (Sect. gif). The slow algorithm implemented here is suitable for modest numbers of observations. For a faster, FFT based version see Press and Rybicki (1991).

SINEFIT/TSA --
Least-squares sinewave fitting: This command fits sine (Fourier) series by nonlinear least squares iterations with simultaneous correction of the frequency. Its main applications are the evaluation of the significance of a detection, parameter estimation, and massaging of data. The values fitted for frequency and Fourier coefficients are displayed on the terminal. For observations correlated in groups of size multiply the errors by (Sect. gif). With the latter correction and for purely sinusoidal variations SINEFIT/TSA computes the frequency with an accuracy comparable to the one of the power spectrum (Lomb, 1976, Schwarzenberg-Czerny, 1991). Additionally, the command displays the parameters of the fitted base sinusoid, i.e. of the first Fourier term.

SINEFIT/TSA returns also the table of the residuals (i.e. of the observations with the fitted oscillation subtracted) in a format suitable for further analysis by any method supported by the TSA package. In this way, the command can be used to perform a CLEAN-like analysis manually by removing individual oscillations one by one in the time domain (see Roberts et al., 1987, Gray & Desikhary, 1973). Since in most astronomical time series the number of different sinusoids present is quite small, we recommend this manual procedure rather than its automated implementation in frequency space by the CLEAN algorithm.

Alternatively, the command can be used to remove a trend from data. In order to use SINEFIT/TSA for a fixed frequency, specify one iteration only. The corresponding value of may in principle be recovered from the standard deviation , where and and are the number of observations and the number of Fourier coefficients (including the mean value), respectively. However, the computation of the periodogram with SINEFIT/TSA is very cumbersome while the results should correspond exactly to the Scargle periodogram (Scargle, 1982, Lomb, 1976).

AOV/TSA --
Analysis of variance: The command computes the analysis of variance (AOV) periodogram. The AOV statistics is a new and powerful method especially for the detection of nonsinusoidal signals (Schwarzenberg-Czerny, 1989). It uses the step function model, i.e. phase binning. Its statistic is . The distribution of S for white noise ( hypothesis) and order bins is the Fisher-Snedecor distribution . The expected value of the AOV statistics for pure noise is 1 for uncorrelated observations and for observations correlated in groups of size .

Among all statistics named in this chapter, AOV is the only one with exactly known statistical properties even for small samples. On large samples, AOV is not less sensitive than other statistics using phase binning, i.e. the step function model: , Whittaker & Roberts and PDM. Therefore we recommend the AOV statistics for samples of all sizes and particularly for signals with narrow sharp features (pulses, eclipses). If on the average consecutive observations are correlated, divide the value of the periodogram by and use the distribution (Sect. gif). For smooth light curves use low order, e.g. 4 or 3, for optimal sensitivity. For numerous observations and sharp light curves use phase bins of width comparable to that of the narrow features (e.g. pulses, eclipses). Note that phase coverage and consequently quality of the statistics near 0 frequency are notoriously poor for most observations.



next up previous contents
Next: Analysis in the Up: MIDAS utilities for Previous: Fourier analysis



Pascal Ballester
Tue Mar 28 16:52:29 MET DST 1995