A Large Low-Pressure AHTR [sm article]

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5PN term has been added in [56] and shown to be due exclusively to the mass octupole and current quadrupole tail integrals in (40), and to the post-Newtonian corrections in the dominant mass quadrupole tail integral in (38) or (39). 5PN order is special to the case of a circular orbit [56]. In the non-circular case the instantaneous terms would also contribute. Incidentally notice that the nonlinear memory integral is instantaneous in the energy loss, and therefore gives no contribution in (65).

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Taylor J. , Astrophys. J. (Letters) 195 (1975) L51. [12] Taylor J. , Fowler L. , Mc Culloch P. , Nature 277 (1979) 437. [13] Peters P. , Phys. Rev. 131 (1963) 435. [14] Esposito L. , Harrison E. , Astrophys. J. 196 (1975) L1. [15] Wagoner R. , Astrophys. J. 196 (1975) L63. , Esposito F. , Astrophys. J. 160 (1970) 153. , Astrophys J. 142 (1965) 1488. , Astrophys J. 158 (1969) 45. , Astrophys J. 158 (1969) 55. [20] Burke W. , unpublished Ph. D. Thesis, California Institute of Technology (1969).

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