

], something that has not been achieved yet with linear
perturbation theory. The fundamental quasi-radial mode in full
general relativity has a similar rotational dependence as in the
relativistic Cowling approximation, and an empirical relation
between the full GR computation and the Cowling approximation can
be constructed (Figure
18). For higher order modes, apparent intersections of mode
sequences near the mass-shedding limit do not allow for such
empirical relations to be constructed.
In the relativistic Cowling approximation, 2D time evolutions
have yielded frequencies for the
l
=0 to
l
=3 axisymmetric modes of rapidly rotating relativistic polytropes
with
N
=1.0 [104
]. The higher order overtones of these modes show characteristic
apparent crossings near mass-shedding (as was observed for the
quasi-radial modes in [330]).
Numerical relativity has also enabled the first study of nonlinear r -modes in rapidly rotating relativistic stars (in the Cowling approximation) by Stergioulas and Font [294]. For several dozen dynamical timescales, the study shows that nonlinear r -modes with amplitudes of order unity can exist in a star rotating near mass-shedding. However, on longer timescales, nonlinear effects may limit the r -mode amplitude to smaller values (see Section 3.5.3).


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Rotating Stars in Relativity
Nikolaos Stergioulas http://www.livingreviews.org/lrr-2003-3 © Max-Planck-Gesellschaft. ISSN 1433-8351 Problems/Comments to livrev@aei.mpg.de |