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Gravitational Waves from Inspiralling Compact Binaries in ... - LUTH

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Log terms <strong>in</strong> total energy flux<br />

FZ total energy flux is <strong>in</strong> terms of the radiative moments,and is true<br />

for any PN source, and <strong>in</strong> particular for a b<strong>in</strong>ary system mov<strong>in</strong>g on<br />

eccentric orbit.<br />

Thus dependence on eccentricity et of the coefficient of ln r0 must<br />

necessarily be given by the function<br />

F (et) = ω8<br />

128 〈Î(4)<br />

ij Î(4)<br />

ij<br />

us<strong>in</strong>g reduced quadrupole moment<br />

〉 = 1<br />

64<br />

+∞<br />

p=1<br />

p 8 | Î<br />

(p) ij| 2 ,<br />

The result is thus perfectly <strong>in</strong> agreement with our f<strong>in</strong>d<strong>in</strong>g of the<br />

function F (e). The dependence of the tail part of the averaged<br />

energy flux on the constant r0 is such that it cancels out, for any<br />

value of the eccentricity, with a similar term com<strong>in</strong>g <strong>from</strong> the<br />

<strong>in</strong>stantaneous part of the flux. Of course such cancellation must be<br />

true for any source, and can be shown based on general arguments<br />

<strong>in</strong> Blanchet, but gives an <strong>in</strong>terest<strong>in</strong>g check of our calculations.<br />

BRI-IHP06-I – p.60/??

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