Astron. Astrophys. 321, 1024-1026 (1997)
3. The Hilbert space of the displacement field
Let be a function space whose elements are
and in which the inner product is defined
as
![[EQUATION]](img16.gif)
where the integration is over the volume of the star.
on is self adjoint,
. There follows the eigenvalue problem
![[EQUATION]](img18.gif)
where is the eigenfrequency of an
oscillation mode, is its eigendisplacement
vector, and n is a collection of three indices, indicating the
three wave numbers in, say, directions of a
spherical polar coordinates. Furthermore, is an
orthogonal set and can be normalized to unity,
![[EQUATION]](img23.gif)
The set is also complete and may serve as a
basis for . See Dixit et al. (1980). Thus, any
may be expanded in a unique way in terms of
. Numerical values of for
hypothetical or actual star models are abundant in the astronomical
literature of seventies and eighties.
© European Southern Observatory (ESO) 1997
Online publication: June 30, 1998
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