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首页> 外文期刊>General Relativity and Gravitation >Review: Hamiltonian Linearization of the Rest-Frame Instant Form of Tetrad Gravity in a Completely Fixed 3-Orthogonal Gauge: A Radiation Gauge for Background-Independent Gravitational Waves in a Post-Minkowskian Einstein Spacetime
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Review: Hamiltonian Linearization of the Rest-Frame Instant Form of Tetrad Gravity in a Completely Fixed 3-Orthogonal Gauge: A Radiation Gauge for Background-Independent Gravitational Waves in a Post-Minkowskian Einstein Spacetime

机译:评论:完全固定的3正交量规中四重心的静止帧即时形式的汉密尔顿线性化:辐射量规,用于后Minkowskian爱因斯坦时空中与背景无关的引力波

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摘要

In the framework of the rest-frame instant form of tetrad gravity, where the Hamiltonian is the weak ADM energy $hat E_{ADM}$ , we define a special completely fixed 3-orthogonal Hamiltonian gauge, corresponding to a choice of non-harmonic 4-coordinates, in which the independent degrees of freedom of the gravitational field are described by two pairs of canonically conjugate Dirac observables (DO) $r_{overline a } (tau ,overrightarrow sigma ),pi overline a (tau ,overrightarrow sigma ),overline a = 1,2$ . We define a Hamiltonian linearization of the theory, i.e. gravitational waves, without introducing any background 4-metric, by retaining only the linear terms in the DO's in the super-hamiltonian constraint (the Lichnerowicz equation for the conformal factor of the 3-metric) and the quadratic terms in the DO's in $hat E_{ADM}$ . We solve all the constraints of the linearized theory: this amounts to work in a well defined post-Minkowskian Christodoulou-Klainermann space-time. The Hamilton equations imply the wave equation for the DO's $r_{overline a } (tau ,overrightarrow sigma ),$ , which replace the two polarizations of the TT harmonic gauge, and that linearized Einstein's equations are satisfied. Finally we study the geodesic equation, both for time-like and null geodesics, and the geodesic deviation equation.
机译:在四重引力的其余帧瞬时形式的框架中,哈密顿量为弱ADM能量$ hat E_ {ADM} $,我们定义了一个特殊的完全固定的3正交哈密顿量表,对应于非调和的选择4坐标,其中重力场的独立自由度由两对正则共轭狄拉克可观测量(DO)$ r_ {overline a}(tau,overrightarrow sigma)描述,pi上标a(tau,overrightarrow sigma)。 ,overline a = 1,2 $。我们通过仅保留超哈密顿约束中DO的线性项来定义该理论的哈密顿线性化,即引力波,而不引入任何背景4度量(3度量的共形因子的Lichnerowicz方程)以及DO中$ hat E_ {ADM} $中的二次项。我们解决了线性化理论的所有限制:这相当于在定义明确的后Minkowskian Christodoulou-Klainermann时空中工作。汉密尔顿方程意味着DO的$ r_ {overline a}(tau,overarrowarrow sigma),$的波动方程,它代替了TT谐波量规的两个极化,并且满足了线性化的爱因斯坦方程。最后,我们研究了时空和零地线的测地线方程以及测地线偏差方程。

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