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Light Cone Structure near Null Infinity of the Kerr Metric
General Relativity and Quantum Cosmology · Submitted 31 Jan 2007
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The Newman-Unti formalism is then further developed, with which the Newman-Penrose constants of the Kerr metric are computed and shown to be zero.
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The abstract, sentence by sentence
Motivated by our attempt to understand the question of angular momentum of a relativistic rotating source carried away by gravitational waves, in the asymptotic regime near future null infinity of the Kerr metric, a family of null hypersurfaces intersecting null infinity in shearfree (good) cuts are constructed by means of asymptotic expansion of the eikonal equation. The geometry of the null hypersurfaces as well asthe asymptotic structure of the Kerr metric near null infinity are studied. To the lowest order in angular momentum, the Bondi-Sachs form of the Kerr metric is worked out. The Newman-Unti formalism is then further developed, with which the Newman-Penrose constants of the Kerr metric are computed and shown to be zero. Possible physical implications of the vanishing of the Newman-Penrose constants of the Kerr metric are also briefly discussed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Motivated by our attempt to understand the question of angular momentum of a relativistic rotating source carried away by gravitational waves, in the asymptotic regime near future null infinity of the Kerr metric, a family of null hypersurfaces intersecting null infinity in shearfree (good) cuts are constructed by means of asymptotic expansion of the eikonal equation. | contribution 0.87 | 0.94 | 0.13 | asserted 1.00 |
| s1 | The geometry of the null hypersurfaces as well asthe asymptotic structure of the Kerr metric near null infinity are studied. | contribution 0.99 | 0.88 | 0.05 | asserted 0.93 |
| s2 | To the lowest order in angular momentum, the Bondi-Sachs form of the Kerr metric is worked out. | contribution 0.48 | 0.92 | 0.08 | asserted 0.99 |
| s3 | The Newman-Unti formalism is then further developed, with which the Newman-Penrose constants of the Kerr metric are computed and shown to be zero. | result 0.81 | 0.92 | 0.29 | asserted 1.00 |
| s4 | Possible physical implications of the vanishing of the Newman-Penrose constants of the Kerr metric are also briefly discussed. | interpretation 1.00 | 0.67 | 0.11 | hedged possibility 0.64 |
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Original abstract
Motivated by our attempt to understand the question of angular momentum of a relativistic rotating source carried away by gravitational waves, in the asymptotic regime near future null infinity of the Kerr metric, a family of null hypersurfaces intersecting null infinity in shearfree (good) cuts are constructed by means of asymptotic expansion of the eikonal equation. The geometry of the null hypersurfaces as well asthe asymptotic structure of the Kerr metric near null infinity are studied. To the lowest order in angular momentum, the Bondi-Sachs form of the Kerr metric is worked out. The Newman-Unti formalism is then further developed, with which the Newman-Penrose constants of the Kerr metric are computed and shown to be zero. Possible physical implications of the vanishing of the Newman-Penrose constants of the Kerr metric are also briefly discussed.
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References
How the literature uses it
4 arXiv papers cite this in 13 sentences
Papers citing it · 9 sentences without a confident label
Uses its method or tool 2 papers
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We find it most convenient to follow Bai et al. [ref] , who derive a BS form of the Kerr metric by deriving a coordinate transformation from Boyer–Lindquist coordinates $(t,r,θ,ϕ)$ to BS coordinates $(,,θ̂,ϕ̂)$, such that the BS gauge conditions [ref] are satisfied.
The Bondi--Sachs gauge, BMS frames, and memory in black hole perturbation theory · Kerr spacetime in Bondi-Sachs coordinates and its associated BMS frame · 0.98
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We will follow Ref. [ref] mainly.
Shaving off soft hairs and the black hole image memory effect · The bald Kerr black hole image · 0.99
Cites it as background 2 papers
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The null hypersurfaces of the Kerr black hole were studied early in 1998 [ref] , followed by Ref. [ref] .
Null hypersurface caustics and super-entropic black holes · Introduction · 1.00
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There were several works on the transformation of the Kerr metric to the BS coordinates [ref] .
Shaving off soft hairs and the black hole image memory effect · The bald Kerr black hole image · 0.95
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