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arXiv 2604.09545gr-qchep-th
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第五后牛顿阶的黑洞动力学

Black Hole Dynamics at Fifth Post-Newtonian Order

Deutsches Elektronen-Synchrotron DESY(德国电子同步加速器);Columbia University(哥伦比亚大学)

Rafael A. Porto, Massimiliano M. Riva

AI总结:

本文基于世界线作用推导了第五后牛顿阶的偶次速度冲击、散射角和时间延迟,结合辐射反应和记忆贡献,提出了一种各向同性描述以确定系统演化。通过Feynman的i0+预设分离保守成分,揭示了记忆贡献的非局部特性,并统一了有效一身体系数。

摘要:

使用[2409.05860]中的世界线作用,我们推导了第五后牛顿阶(5PN)的总偶次速度(相对)冲击、散射角和时间延迟,包括辐射反应和记忆贡献在${\cal O}(G^5ν^2)$和${\cal O}(G^6ν^2)$阶。我们引入了一种各向同性描述,结合能量和角动量的损失,以散射数据确定系统的演化。该框架为仅通过散射观测符来无歧义地表征双体动力学提供了途径。遵循[2409.05860],我们利用Feynman的$i0^+$预设分离保守成分。该部分包含“尾状”和“记忆状”贡献,后者在时间上非局部,由双重主值积分描述。由于相应(in-in)作用的局部时间特性,我们建立了一种与Feynman预设一致且保持完整局部动力学的系统方法。这为5PN阶的保守(各向同性)哈密顿量提供了普遍贡献,并作为副产品,一致地确定了有效一身体系数$\{{\bar d}_{5{\rm loc}}, a_{6{\rm loc}}\}$,与Tutti-Frutti框架一致。为完整性,我们分析了最近的后闵可夫斯基计算中引入的“γ-3”预设。当在我们的形式化中实施时,我们发现其在有效范围内的精确一致。相反,Feynman的预设在${\cal O}(G^5ν^2)$阶产生一个(局部)记忆状贡献,符号相反。我们还发现,一个类似的γ-3重定向在${\cal O}(G^6ν^2)$阶会与猜想矛盾,即所有$π^2$项仅来自势场区域,而Feynman的表述保持了这一预期。

英文摘要:

Using the worldline action in [2409.05860], we derive the total even-in-velocity (relative) impulse, scattering angle, and time delay at fifth post-Newtonian (5PN) order, including radiation-reaction and hereditary contributions at ${\cal O}(G^5ν^2)$ and ${\cal O}(G^6ν^2)$. We introduce an isotropic-like description which, together with the associated losses of energy and angular momentum, fixes the evolution of the system from scattering data. This framework opens the door to an unambiguous characterization of the underlying two-body dynamics solely in terms of scattering observables. Following [2409.05860], we isolate a conservative component using Feynman's $i0^+$ prescription. This sector contains both "tail-like" and "memory-like" contributions, the latter being nonlocal in time and described by a double Principal-Value integral. Owing to the local-in-time character of the corresponding (in-in) action, we establish a systematic procedure that is consistent with Feynman's prescription while preserving the complete local dynamics. This provides a universal contribution to the conservative (isotropic) Hamiltonian at 5PN order and, as a byproduct, also fixes the value of the Effective One Body coefficients $\{{\bar d}_{5{\rm loc}}, a_{6{\rm loc}}\}$ consistently with the Tutti-Frutti framework. For completeness, we analyse the "$γ\text{-}3$" prescription introduced in recent post-Minkowskian computations. When implemented in our formalism, we find exact agreement over the overlapping regime of validity. In contrast, Feynman's prescription yields a (local) memory-like contribution with the opposite sign at ${\cal O}(G^5ν^2)$. We also find that an analogous $γ\text{-}3$ rerouting at ${\cal O}(G^6ν^2)$ would be incompatible with the conjecture that all $π^2$ terms arise solely from the potential region, while Feynman's formulation preserves this expectation.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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