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

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Energy Flux - Modified Harmonic Coords<br />

Logs can be removed by the follow<strong>in</strong>g shift on the particle world-l<strong>in</strong>es:<br />

ξ i 1 =<br />

22 m<br />

3<br />

2 1m2 c6 r2 ni <br />

r<br />

ln ,<br />

ξ i 2<br />

= − 22<br />

3<br />

Under shift ξ, Accn of First particle shifts by<br />

Rel Accn shifts by<br />

δξa i = − m3 ν<br />

+<br />

r 4<br />

δξa i 1 = ¨ ξ i 1 − ξ j<br />

1<br />

m1m 2 2<br />

c 6 r 2 ni ln<br />

r ′ 1<br />

r<br />

r ′ 2<br />

<br />

− ξj<br />

2 ∂ja i 1 .<br />

<br />

110 ˙r 2 − 22v 2 n i − 44 ˙rv i ln<br />

<br />

− 176<br />

3 ˙r2 + 22<br />

3 v2 − 22<br />

3<br />

m<br />

r<br />

<br />

.<br />

n i + 44<br />

3 ˙rvi<br />

Log dependence <strong>in</strong> the above transformation exactly cancels the log dependence<br />

of the acceleration <strong>in</strong> standard harmonic coord<strong>in</strong>ates. Some 3PN coefficients<br />

<strong>in</strong> the EOM are also modified and the f<strong>in</strong>al result for Accn <strong>in</strong> Modified Harm<br />

Coords. agrees with that displayed <strong>in</strong> e.g. Mora Will<br />

BRI-IHP06-I – p.33/??<br />

r<br />

<br />

r ′ 0

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