Gravitational self-force and the effective-one-body formalism between the innermost stable circular orbit and the light ring

Gravitational self-force and the effective-one-body formalism between the innermost stable circular orbit and the light ring
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DOI:
10.1103/physrevd.86.104041
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发表时间:
2012-09
期刊:
影响因子:
5
通讯作者:
S. Akçay;L. Barack;T. Damour;N. Sago
S. Akçay;L. Barack;T. Damour;N. Sago
中科院分区:
物理与天体物理2区
文献类型:
--
作者:
S. Akçay;L. Barack;T. Damour;N. Sago

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我们计算保守片的引力自作用力(GSF)作用于一个粒子的质量M1,因为它移动沿着(不稳定)圆形测地轨道之间的最内层的稳定轨道和光环的史瓦西黑洞的质量M2?M1.更确切地说,我们构造函数huuR,L(x)?h??R,Lu?u?(与德特韦勒的规范不变的“红移”变量),其中h??R,L(?m1)是Lorenz规范中的正则化度量微扰,u?是m1在m2的背景史瓦西度规中的四速度,而x?【GC-3(m1+m2)?】2/3是从轨道频率?构造的不变坐标。特别地,我们探索了huuR,L在x=1/3的“光环”之外的行为(即,r= 3Gm 2/c2),其中圆形轨道变为零。利用最近发现的huuR,L和a(u)之间的联系,对称质量比??m1 m2/(m1+m2)2,主径向势A(u,?)= 1-2u+?a(u)+O(?2)的有效单体(EOB)的形式主义,我们计算从我们的GSF数据EOB函数a(u)在整个区域0<u<1/3(从而扩展以前的结果限于u?1/5)。我们发现a(u)像a(u)一样发散?0.25(1-3u)-1/2在光环极限,u?(1/3)-,解释这种发散行为的物理起源,并讨论其后果的EOB形式主义。我们构造了a(u)的精确的全局解析拟合,在整个区域0<u<1/3(甚至更远)上都是有效的,并给出了a(u)及其前三阶导数在最内层稳定圆轨道u=1/6处的精确数值估计,以及相关的O(?)轨道频率的变化。在以前的工作中,我们使用GSF的数据,稍微偏心的轨道上计算一定的线性组合的a(u)和它的前两个衍生物,也涉及O(?)第二EOB径向电位D的一部分?(u)=1+?你是谁?(u)+O(?2)。结合这些结果与我们目前的全球解析表示(u),我们数值计算d?(u)在间隔0<u上?1/6
We compute the conservative piece of the gravitational self-force (GSF) acting on a particle of mass m1 as it moves along an (unstable) circular geodesic orbit between the innermost stable orbit and the light ring of a Schwarzschild black hole of mass m2?m1. More precisely, we construct the function huuR,L(x)?h??R,Lu?u? (related to Detweiler’s gauge-invariant “redshift” variable), where h??R,L(?m1) is the regularized metric perturbation in the Lorenz gauge, u? is the four-velocity of m1 in the background Schwarzschild metric of m2, and x?[Gc-3(m1+m2)?]2/3 is an invariant coordinate constructed from the orbital frequency ?. In particular, we explore the behavior of huuR,L just outside the “light ring” at x=1/3 (i.e., r=3Gm2/c2), where the circular orbit becomes null. Using the recently discovered link between huuR,L and the piece a(u), linear in the symmetric mass ratio ??m1m2/(m1+m2)2, of the main radial potential A(u,?)=1-2u+?a(u)+O(?2) of the effective-one-body (EOB) formalism, we compute from our GSF data the EOB function a(u) over the entire domain 0<u<1/3 (thereby extending previous results limited to u?1/5). We find that a(u) diverges like a(u)?0.25(1-3u)-1/2 at the light-ring limit, u?(1/3)-, explain the physical origin of this divergent behavior, and discuss its consequences for the EOB formalism. We construct accurate global analytic fits for a(u), valid on the entire domain 0<u<1/3 (and possibly beyond), and give accurate numerical estimates of the values of a(u) and its first three derivatives at the innermost stable circular orbit u=1/6, as well as the associated O(?) shift in the frequency of that orbit. In previous work we used GSF data on slightly eccentric orbits to compute a certain linear combination of a(u) and its first two derivatives, involving also the O(?) piece of a second EOB radial potential D? (u)=1+?d? (u)+O(?2). Combining these results with our present global analytic representation of a(u), we numerically compute d? (u) on the interval 0<u?1/6