2021
DOI: 10.1103/physrevd.103.024057
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New spinorial approach to mass inequalities for black holes in general relativity

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Cited by 4 publications
(4 citation statements)
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“…However, the use of the skew symmetric tensor J i j in the form of the perturbation does not seem strictly necessary and could likely be removed. Another possibility would be to investigate further a spin geometry approach to proving the Penrose inequality, although this would also involve sophisticated estimates from PDE theory [19][20][21].…”
Section: Discussionmentioning
confidence: 99%
“…However, the use of the skew symmetric tensor J i j in the form of the perturbation does not seem strictly necessary and could likely be removed. Another possibility would be to investigate further a spin geometry approach to proving the Penrose inequality, although this would also involve sophisticated estimates from PDE theory [19][20][21].…”
Section: Discussionmentioning
confidence: 99%
“…The subsequent analysis will further refinement of a 1 + 1 + 2 spinorial split. This is analogous to the 1 + 3 split when an additional direction ρ a is singled out-see [15,21,23,24,30] for further discussion on the space-spinor formalism, the 1 + 3 split, the 1 + 1 + 2 split and applications. The basic elements of this formalism will be discussed on a general manifold with metric (M, g) and towards the end of this section, some results specific for Friedrich's representation of the spatial infinity of the Minkowski spacetime (M, η) will be given.…”
Section: The Space-spinor Formalismmentioning
confidence: 91%
“…Further discussion on the spinorial 1 + 1 + 2 split can be found in [15,23,24]. Particularising the previous general discussion to Friedrich's representation of the spatial infinity of the Minkowski spacetime and using the lift to the fibre space of the null frame (9a)-(9d) and exploiting (23) one can directly read…”
Section: The Space-spinor Decomposition Of the Connectionmentioning
confidence: 96%
“…The subsequent analysis will further refinement of a 1 + 1 + 2 spinorial split. This is analogous to the 1 + 3 split when an additional direction ρ a is singled out -see [32,21,24,23,16] for further discussion on the space-spinor formalism, the 1 + 3 split, the 1 + 1 + 2 split and applications. The basic elements of this formalism will be discussed on a general manifold with metric (M, g) and towards the end of this section, some results specific for Friedrich's representation of the spatial infinity of the Minkowski spacetime (M, η) will be given.…”
Section: The Space-spinor Formalismmentioning
confidence: 98%