Astron. Astrophys. 321, 1024-1026 (1997)
6. The overlap integrals
Using the and
decomposition of Eq. (8) for gives
![[EQUATION]](img83.gif)
By Eq. (12), V is a spherical harmonic of order 2. Therefore, only
the normal modes belonging to will contribute
to the overlap integral, that is, Substituting
for and V and carrying out integrations over
, gives
![[EQUATION]](img89.gif)
For numerical calculations the following steps were taken.
1) A Rayleigh-Ritz variational method was employed to obtain the
eigenfrequencies and eigenfunctions for various
and modes(Sobouti & Silverman 1978). The
method consisted of expanding the and
potentials of Eqs. (8) in power series of
r, substituting the resulting 's in Eq.
(6) and finding the expansion coefficients by variational
calculations.
2) The information thus obtained was used to extract the
potential for each of the
and modes and to calculate the overlap integrals
of Eq. (19a), and eventually the cross sections and the energy
absorption rates. Numerical values for polytropic structures are
summarized in Table 1.
![[TABLE]](img91.gif)
Table 1. Cross sections for different modes of polytropic indeces 1.5, 2, 2.5
© European Southern Observatory (ESO) 1997
Online publication: June 30, 1998
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