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PENT
Return the information entropy of a time series
This function will return S, the information entropy of a time series for a set of trial periods
Time series analysis, period finding, astronomical utilities.
Result = PENT(P, T, X, [N, M ] )
P - array of trial period values. T - array of observation times (same units as P). X - array of observations.
N - If four parameters are given then the 4th parameter is assumed to be N. Then NxN boxes are used to calculate S. M,N - If five parameters are given then parameter 4 is M and parameter 5 is N. S is then calculated using MxN boxes - M partitions for the phase and N partitions for the data.
This function returns S, the information entropy of the time series for the periods given in P as defined by Cincotta, Me'ndez & Nu'n~ez (Astrophysical Journal 449, 231-235, 1995). The minima of S occur at values of P where X shows periodicity.
The procedure involves dividing the phase space into N^2 partitions (NxN boxes) and then calculating: __ N^2 S = - \ mu_i . ln(mu_i) for all mu_i <> 0 /_ i = 1 where mu_i is the number of data points in partition i normalised by the number of partitions. The option of using MxN boxes is an additional feature of this routine.
To generate a similar sythetic data set to Cincotta et al. we do the following: IDL> P0 = 173.015 ; Fundamental period IDL> T = randomu(seed,400)*15000 ; 400 random observation times IDL> A0 = 14.0 ; Mean magnitude IDL> M0 = -0.5 * sin(2*!pi*T/P0) ; Fundamental mode IDL> M1 = -0.15 * sin(4*!pi*T/P0) ; 1st harmonic IDL> M2 = -0.05 * sin(6*!pi*T/P0) ; 2nd harmonic IDL> sig = randomu(seed,400)*0.03 ; noise IDL> U = A0 + M0 + M1 + M2 + sig ; Synthetic data IDL> Ptest = 100. + findgen(2000)/2. ; Trial periods IDL> S = pent(Ptest,T,U) ; Calculate S ... this takes a few seconds ... IDL> plot,Ptest,S,xtitle="P",ytitle="S" ; plot S v. P IDL> print,Ptest(where(S eq min(S))) ; Print best period (+/- 0.5) The plot produced should be similar to Fig. 2 of Cincotta et al.
My own (limited) experience with this routine suggests that it is not as good as other techniques for finding weak, multi-periodic signals in poorly sampled data, but is good for establishing periods of eclipsing binary stars when M is quite large (try MxN = 64x16, 128x16 or even 256x16). This suggests it may be good for other periodic light curves (Cepheids, RR Lyrae etc.). I would be glad to receive reports of other peoples experience with this technique (e-mail pflm@bro730.astro.ku.dk).
Written by: Pierre Maxted, 14Sep95 Modifications: Normalisation of S corrected, T-min(T) taken out of loop. - Pierre Maxted, 15Sep95 Converted to IDL V5.0 W. Landsman September 1997
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