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Center-of-mass angular momentum and memory effect in asymptotically flat spacetimes

机译:浅谈渐近扁平空间中的群质量角动量和记忆效应

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摘要

Gravitational-wave (GW) memory effects are constant changes in the GW strain and its time integrals, which are closely connected to changes in the charges that characterize asymptotically flat spacetimes. The firstGWmemory effect discovered was a lasting change in theGWstrain. It can occur whenGWsor massless fields carry away 4-momentum from an isolated source. Subsequently, it was shown that fluxes of intrinsic angular momentum can generate a new type of memory effect called the spin memory, which is an enduring change in a portion of the time integral of theGWstrain. In this paper,we note that there is another newtype of memory effect. We call it the "center-of-mass (CM) memory effect," because it is related to changes in the CM part of the angular momentum of a spacetime. We first examine a few properties of the CM angular momentum. Specifically, we describe how it transforms under the supertranslation symmetry transformations of the Bondi-Metzner-Sachs group, and we compute a new expression for the flux of CM angular momentum carried by GWs in terms of a set of radiative multipole moments of the GW strain. We then turn to the CM memory effect. The CM memory effect appears in a quantity which has the units of the time integral of theGWstrain.We define the effect in asymptotically flat spacetimes that start in a stationary state, radiate, and settle to a different stationary state. We show that it is invariant under infinitesimal supertranslation symmetries in this context. To determine the magnitude of the flux of CM angular momentum and theCMmemory effect, we compute these quantities for nonspinning, quasicircular compact binaries in the post-Newtonian approximation. The CM memory effect arises from terms in the gravitational waveform for such binaries beginning at third and fourth post-Newtonian order for unequal- and equal-mass binaries, respectively. Finally, we estimate the amplitude of the CM memory effect for these binaries. We anticipate that it will be u
机译:引力波(GW)存储器效果是GW应变的恒定变化及其时间积分,其紧密地连接到表征渐近平坦的倒数的电荷的变化。发现的FirstGWMemory效果是TheGWstrain的持久变化。当GWSOR无压磁场从隔离源携带4次动力时可能发生。随后,显示内在角动量的助熔剂可以产生称为自旋记忆的新型记忆效应,这是Gwstrain的一部分时间内的持久变化。在本文中,我们注意到还有另一个内存效果的新型。我们称之为“质量中心(CM)记忆效应”,因为它与时空角动量的CM部分的变化有关。我们首先检查CM角动量的几个属性。具体而言,我们描述它是如何将根据邦迪METZNER - 萨克斯组的supertranslation对称变换,并且我们计算在一组GW应变的辐射多极矩的方面为通过GW的进行CM的角动量通量一个新的表达式。然后我们转到CM内存效果。 CM内存效果出现在具有TheGwstrain的时间整体的单位的数量中。我们在朝向静止状态下开始的渐近扁平时空中的效果,辐射,并沉降到不同的静止状态。我们表明它在此上下文中的无限超周期对称下是不变的。为了确定CM角动量和THEMMEMORY效果的磁通量的大小,我们将这些数量计算在牛顿后近似的非纯净,QuasiClular Compact二进制文件。对于从第三和第四届牛顿术语顺序的比例和相等的大众二进制文件开始的这种二进制文件的引力波形中的术语术语产生。最后,我们估计这些二进制文件的CM内存效果的幅度。我们预计它将是你

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  • 来源
    《Physical review, D》 |2018年第2期|共26页
  • 作者

    David A. Nichols;

  • 作者单位

    Gravitation Astroparticle Physics Amsterdam (GRAPPA) University of Amsterdam Science Park P.O. Box 94485 1090 GL Amsterdam Netherlands and Department of Astrophysics/IMAPP Faculty of Science Radboud University P.O. Box 9010 6500 GL Nijmegen Neth;

  • 收录信息
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 粒子物理学;场论;
  • 关键词

    characterize; transforms; nonspinning;

    机译:表征;变换;非宁静;

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