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

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Radiative moments - Source moments<br />

The relations connect<strong>in</strong>g the different radiative moments UL and<br />

VL to the correspond<strong>in</strong>g source moments IL and JL are given<br />

below. For the mass type moments we have (Blanchet 92.. 98)<br />

Uij(U) = I (2) 2GM<br />

ij (U) +<br />

+ G<br />

c 5<br />

<br />

− 2<br />

7<br />

+ 1<br />

c 3<br />

+∞<br />

0<br />

+∞<br />

0<br />

dτ<br />

<br />

cτ<br />

ln<br />

2r0<br />

+ 11<br />

2<br />

dτI (3)<br />

aa (U − τ)<br />

7 I(5) aa − 5<br />

7 I(4) aa<br />

<br />

+4 W (2) Iij − W (1) I (1)<br />

<br />

ij<br />

<br />

GM<br />

+2<br />

c3 2 +∞<br />

dτI<br />

0<br />

(5)<br />

ij (U − τ)<br />

<br />

ln 2<br />

<br />

cτ<br />

+<br />

2r0<br />

57<br />

70 ln<br />

<br />

cτ<br />

+<br />

2r0<br />

124627<br />

44100<br />

+O(7),<br />

<br />

− 2<br />

7 I(3)<br />

aa<br />

<br />

I (4)<br />

ij (U − τ)<br />

1 (4)<br />

+ εaba<br />

3 Jb<br />

BRI-IHP06-I – p.23/??

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