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

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Far Zone Angular Momentum Flux<br />

From the expressions for ULs and VLs, one can schematically split<br />

the total contribution to the angular momentum flux as the sum of<br />

the <strong>in</strong>stantaneous and hereditary terms.<br />

Start<strong>in</strong>g <strong>from</strong> the expression for the angular momentum flux <strong>in</strong> terms<br />

of the radiative multipole moments and the expressions for the<br />

radiative moments <strong>in</strong> terms of the source multipoles the AMF can be<br />

re-written as<br />

dJi<br />

dt<br />

<br />

<strong>in</strong>st(s)<br />

dJi<br />

dt<br />

<br />

=<br />

= G<br />

<br />

2<br />

εipq<br />

c5 + 1<br />

c 2<br />

+ 1<br />

c 6<br />

1<br />

dJi<br />

dt<br />

5 I(2)<br />

pj I(3)<br />

qj<br />

63 I(3)<br />

pjk I(4)<br />

qjk<br />

<br />

<br />

<strong>in</strong>st<br />

+ 32<br />

45<br />

+<br />

J (2)<br />

pj<br />

1<br />

118800 I(5)<br />

pjklm I(6)<br />

qjklm<br />

dJi<br />

dt<br />

<br />

hered<br />

<br />

(3)<br />

J qj + 1<br />

c4 .<br />

1<br />

2268 I(4)<br />

pjkl I(5)<br />

qjkl<br />

16 (4) (5)<br />

+ J pjklJ qjkl<br />

14175<br />

<br />

,<br />

1 (3)<br />

+ J pjk 28<br />

BRI-IHP06-I – p.71/??

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