Gravitational wave tails are produced by back-scattering of the outgoi
ng gravitational radiation (emitted by an isolated system) off the cur
ved spacetime associated with the total mass of the system. This paper
investigates the spectral (or Fourier) decomposition of gravitational
wave tails at large distances from the system, at the 1.5 post-Newton
ian order in the wave field. It is shown that the effects of wave tail
s are (i) to increase the amplitude of the Fourier components of the (
linear) waves by a factor linearly depending on the frequency, and (ii
) to add to the phase of the waves a supplementary phase depending on
the frequency as omega ln omega. The latter frequency-dependent phase
introduces a new effect which should be observable in any radiation co
ntaining more than one frequency, for instance in the radiation emitte
d by a binary star system orbiting a Keplerian ellipse with non-zero e
ccentricity, or in the radiation emitted by an inspiralling (compact)
binary star system. We propose in this paper to include the tail-induc
ed effects (i) and (ii) in the matched filters of the future data anal
ysis of inspiralling compact binary signals in laser interferometer gr
avity-wave detectors (at least in future, very sensitive, such detecto
rs). In this way, the filters will be highly correlated with the actua
l signal, and in particular will remain, as the frequency of the signa
l increases, in accurate phase with it. The contribution of the wave t
ail in the total gravitational energy emitted by a binary system is al
so calculated, and a numerical application to the binary pulsar PSR 19
13+16 is presented. We find that the tail-induced relative correction
in the orbital P(Th) of the pulsar is equal to -1.65 x 10(-7) (too sma
ll to be observed).