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4. Evenly sampled data and limits for continuous functions

The mentioned above equations are valid without restrictions on the distribution of the times of observations. However, evenly spaced signals are also often used in astronomy, and they allow to use the same matrices inside the interval, except the edges. For large number of evenly sampled observations, one may replace sums by integrals:
equation733
Corresponding parameters may be computed as integrals
equation741
Particularly, an expectation of the rms deviation tex2html_wrap_inline2452 of the parameter X is
equation745
where V[X] is a value of the integral characterizing variance of X, and tex2html_wrap_inline2008 is an "unit weight" error (cf. Whittaker & Robinson 1928). Hereafter one may omit a constant n/(z2-z1), when replacing sums by integrals, while not specially mentioned. For example, Eq. (9) may be rewritten as
equation752

For an interval (-1, 1) covered by the observations, Ss=2/(s+1) for even s and 0 else. For constant weights p(z)=1 (case "up") the matrices are the following:
equation759
For the coefficients tex2html_wrap_inline1998 one may obtain
eqnarray788
For simple running mean ("um") h[C0,z]=1/2, V=1/2, and other coefficients tex2html_wrap_inline2478 by definition. One may note that coefficients C1 and C2 for "unweighted" polynomial fits are equal to tex2html_wrap_inline2484 and tex2html_wrap_inline2486 (in dimensionless argument units z). However, with changing interval, the observational points are added to and removed from the set, thus such an approximation is valid only for a fixed set of data (tk,xk). For continuous functions, one may not choose an interval of t0 with a fixed set, and derivatives are computed using Eq. (31).

For the weights p(z)=(1-z2)2,
equation805
For "weighted mean" ("wm"):
equation838
For "weighted parabolae" ("wp"):
eqnarray844
To determine h[C01,z] and h[C02,z], one would use Eqs. (38, 39). However, for continuous polynomial fits and all weight functions satisfying the condition tex2html_wrap_inline2500 the matrices tex2html_wrap_inline2414 tex2html_wrap_inline2416 are equal to zero, as well as tex2html_wrap_inline2506 For "wp",
eqnarray864
One may note that more complicated character of the evaluation of the derivatives as compared with coefficients C1 and C2 leads to much larger values of corresponding parameter V, e.g. V[C01]/V[C10]=525/140.

  figure878
Figure 3: Projective functions h[C0,z] for 4 model "symmetric" polynomial fits

First derivative of the smoothing function in the case of continuous signal x(t) is equal to
eqnarray883
For "symmetric" fits tex2html_wrap_inline2520 one may obtain
eqnarray900
One may note that derivatives for the "unweighted" fits are strongly dependent on particular values of the signal at the borders, making impossible the form (50) without using the Dirac's tex2html_wrap_inline2522 functions. In a case tex2html_wrap_inline2524 one may introduce corresponding functions tex2html_wrap_inline2526 and to obtain V=15/7 for "wm" and V=525/22 for "wp".

Expressions for "asymmetric" fits are much more complicated. For an extreme case tex2html_wrap_inline2532 tex2html_wrap_inline2534 for "unweighted" fits, and tex2html_wrap_inline2536. Corresponding functions h are equal to 0, if z<0 and z>1. From 0 to 1 they are the following:
eqnarray937


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