准圆形紧二进制系统的重力波分阶段化到四分之一半的后牛顿秩序
Luc Blanchet1, Guillaume Faye1,2, Quentin Henry3
1𝒢ℝϵℂ𝒪, Institut d'Astrophysique de Paris, UMR 7095, CNRS, Sorbonne Université, 98bis boulevard Arago, 75014 Paris, France.
Physical review letters
|October 6, 2023
概括
无自旋二进制星的引力波启发阶段是以4.5的后牛顿 (PN) 顺序计算的. 这项研究推进了引力波物理学,并有助于分析来自紧的二进制系统的信号.
科学领域:
- 引力波物理 引力波物理
- 一般相对论一般相对论.
- 天体物理学 天体物理学
背景情况:
- 紧的二进制星系是引力波的主要来源.
- 准确的波形建模对于检测和解释引力波信号至关重要.
- 后牛顿式 (PN) 扩张提供了一种方法,可以在启发阶段大致估计引力波的产生.
研究的目的:
- 为无旋转的紧双星推导引力波阶段到4.5后牛顿 (PN) 顺序.
- 为了计算领先的振幅模式 (l,m) = ((2,2) 到 4PN 的顺序.
- 提供与当前和未来引力波探测器相关的PN贡献的数值估计.
主要方法:
- 使用后牛顿式 (PN) 膨胀技术计算启发阶段.
- 领先振幅模式的导数 (l,m) = ((2,2)).
- 应用静止相近似来确定辐射的流量和相位.
主要成果:
- 对于无旋转的紧二进制星,引力波阶段的推导值高达4.5PN.
- 领先的振幅模式 (l,m) = ((2,2) 在4PN顺序下确定.
- 提供了静止相近似的辐射流量和相位.
结论:
- 导出的4.5PN顺序为引力波的启发阶段提供了更准确的描述.
- 这些结果增强了引力波数据分析的分析工具.
- 数字估计提供了关于像LIGO和Virgo这样的天文台对不同PN贡献的检测能力的见解.
相关概念视频
Kepler's Third Law of Planetary Motion
3.3K
In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. In 1909, he formulated his first two laws based on the observations of his forebears, Nikolaus Copernicus and Tycho Brahe. However, in 1918, he published his third law of planetary motion, which gives a precise mathematical relationship between a planet's average distance from the Sun and the amount of time it takes to revolve around the Sun. It...
3.3K
Second Order systems II
117
In an underdamped second-order system, where the damping ratio ζ is between 0 and 1, a unit-step input results in a transfer function that, when transformed using the inverse Laplace method, reveals the output response. The output exhibits a damped sinusoidal oscillation, and the difference between the input and output is termed the error signal. This error signal also demonstrates damped oscillatory behavior. Eventually, as the system reaches a steady state, the error diminishes to zero.
117
Kepler's Second Law of Planetary Motion
4.2K
In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. His first law states that all planets orbit the Sun in an elliptical orbit, with the Sun at one of the ellipse's foci. Therefore, the distance of a planet from the Sun varies throughout its revolution around the Sun.
While in an elliptical orbit, the total energy of the planet is conserved. Therefore, the planet slows down when it is at apogee and...
While in an elliptical orbit, the total energy of the planet is conserved. Therefore, the planet slows down when it is at apogee and...
4.2K
Second Order systems I
169
A servo system exemplifies a second-order system, featuring a proportional controller and load elements that ensure the output position aligns with the input position. The relationship between these components is described by a second-order differential equation. Applying the Laplace transform under zero initial conditions yields the transfer function, showing how inputs are converted to outputs in the system.
By reinterpreting the system, one can derive the closed-loop transfer function, which...
By reinterpreting the system, one can derive the closed-loop transfer function, which...
169
Kepler's First Law of Planetary Motion
4.1K
In the early 17th century, German astronomer and mathematician Johannes Kepler postulated three laws for the motion of planets in the solar system. He formulated his first two laws based on the observations of his forebears, Nikolaus Copernicus and Tycho Brahe.
Polish astronomer Nikolaus Copernicus put forth a theory that stated a heliocentric model for the solar system. According to this heliocentric theory, all the planets, including Earth, orbit the Sun in circular orbits.
On the other hand,...
Polish astronomer Nikolaus Copernicus put forth a theory that stated a heliocentric model for the solar system. According to this heliocentric theory, all the planets, including Earth, orbit the Sun in circular orbits.
On the other hand,...
4.1K
Gravitation Between Spherically Symmetric Masses
918
The gravitational potential energy between two spherically symmetric bodies can be calculated from the masses and the distance between the bodies, assuming that the center of mass is concentrated at the respective centers of the bodies.
918


