PHYSICS
OFTHE EARTH
AND P LAN ETA RY
_________ INTERIORS
ELSEVIER Physics of the Earth and Planetary Interiors 84 (1994) 139—160
A new technique in demodulation of normal modes
Ramin Nawab Philippe Lognonné
Laboratoire de Sismologie, Institut de Physique du Globe de Paris, 4 place Jussieu, 75252 Paris Cedex 05, France
(Received 6 May 1993; revision accepted 8 December 1993)
Abstract
Lateral heterogeneities of the Earth produce amplitude modulations of the so-called unresolved multiplets. A
spectral fitting technique based on the polynomial interpolation of Hermite allows the retrieval of these slowly
varying modulation functions. No restrictive hypothesis on coupling among multiplets is necessary. Modulation
functions are constrained in time within a Q-cycle for data with typical signal-to-noise ratios. Sensitivity to noise is
reduced by the introduction of cosine tapers and by a priori information on the modulation functions. The method
then damps rapid oscillations caused by noise and becomes stable. These amplitude modulations can be used in a
first stage for inversions where both phase and amplitude are necessary, and generalize basic mode observables such
as the local frequency.
1. Introduction signals and then invert these observables to re-
trieve the aspherical structure. The simplest ob-
Lateral variations of the deep structure of the servable is the frequency of the maximum of an
Earth can be retrieved by non-linear and simulta- unresolvably split normal mode resonance peak
neous inversions of a large set of spectra of and its deviation from the spherical frequency of
normal modes (see, e.g. Ritzwoller et al., 1986, the multiplet. As shown by Jordan (1978), this
1988; Giardini et al., 1987, 1988). Such methods deviation, known as the location parameter (A),
imply, however, theoretical approximations on the is, up to the first order of the perturbation theory
normal modes, for instance by neglecting cou- of the Earth’s normal modes (see, e.g. Dahien,
pling effects. This is also the case for stripping or 1979) and for times shorter than the inverse of
stacking methods (see, e.g. Dziewonski and the frequency shift (short time approximation),
Gilbert, 1973a, b; Gilbert and Dziewonski, 1975; related to the depth-averaged structure between
Buland et al., 1979), which extract from a global the source and the receiver. Inversions of these
set of normal modes the eigenfrequencies under observables have been performed by Silver and
the isolated multiplet hypothesis. Jordan (1981), Masters et a!. (1982), Roult and
Other inversion methods, in contrast, extract Romanowicz (1984), and others. More exact ex-
in a first step some observables from the seismic pressions have been developed by Dahlen (1974),
Woodhouse and Girnius (1982), Davis and Hen-
_______ son (1986) and Romanowicz and Roult (1986),
* Corresponding author, including either coupling effects or higher-order
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