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(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

(ed.). Gravitational waves (IOP, 2001)(422s).

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78 Source calculations,,3 .3, ORJ 7.Figure 7.1. The balance of viscous and gravitational radiation effects in the r-modes isillustrat<strong>ed</strong> in a diagram of rotation spe<strong>ed</strong>, showing the ratio of the maximum period P kto the rotation period P versus the temperature of the star. The solid curve indicates theboundary between viscosity-dominat<strong>ed</strong> and radiation-dominat<strong>ed</strong> behaviour: stars abovethe line are unstable. The dash<strong>ed</strong> curves illustrate possible nonlinear evolution histories asa young neutron star cools.that become important as the modes grow. This could only be done with anumerical simulation, which some groups are now working on. However, it ispossible to make simple estimates analytically.We characterize the initial configuration with just two paramters: the uniformangular velocity , and the amplitude α of the r-modes perturbation. The star isassum<strong>ed</strong> to cool at the accept<strong>ed</strong> cooling rate for neutron stars, independently ofwhether it is affect<strong>ed</strong> by the r-mode instability or not. The star is assum<strong>ed</strong> tolose angular momentum to gravitational radiation at a rate given by the linearradiation field, with its large amplitude α. This loss is taken to drive the starthrough a sequence of equilibrium states of lower and lower angular momentum.Details of this approximation are in [31], here we report only the results. The

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