Abstract
For the next lecture, we consider four-dimensional asymptotically flat spacetimes, which are the solutions of General Relativity with localised energy-momentum sources. We will start with a review of the work of Penrose on the conformal compactification of asymptotically flat spacetimes in order to get a global view on the asymptotic structure. We will then concentrate on the properties of radiative fields by reviewing the work of van der Burg, Bondi, Metzner and Sachs of 1962. One may think at first that the group of asymptotic symmetries of radiative spacetimes is the Poincaré group, but a larger group appears, the BMS group which contains so-called supertranslations. Additional symmetries, known as superrotations, also play a role and we shall briefly discuss them too. Finally, we will give some comments on the scattering problem in General Relativity. We will show that the extended asymptotic group gives conserved quantities once junction conditions are fixed at spatial infinity
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Notes
- 1.
Strictly speaking it implies that Ψ = 0 up to the lowest l = 0, 1 spherical harmonics. However, these harmonics are exactly zero modes of the differential operator ε C(A D B) D C Ψ defined in C AB. Therefore we can set them to zero.
- 2.
Similarly to the construction of the AdS 3 phase space of stationary field configurations with boundary fields turned on that was described in (2.57) or for the asymptotically flat analogue (2.73), one can construct gravitational vacua and Schwarzschild black holes that carry a supertranslation field, see [15, 16].
- 3.
- 4.
The attentive reader might already notice that such an observable is not clearly the difference between a quantity in the initial and final state. Instead \(\int _{u_i}^{u_f} du \: \Psi \) is non-local in retarded time! Therefore, though it bears analogy with the displacement memory effect, the spin memory effect is not (yet?) proven to be a memory effect at the first place! For a discussion of memory effects associated with Diff(S 2) symmetries, see [17].
- 5.
Shortcut: just formally replace u →−v everywhere while leaving r unchanged.
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Compère, G. (2019). Asymptotically Flat Spacetimes. In: Advanced Lectures on General Relativity. Lecture Notes in Physics, vol 952. Springer, Cham. https://doi.org/10.1007/978-3-030-04260-8_3
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