1996
DOI: 10.1088/0264-9381/13/6/025
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Vacuum Einstein equations in terms of curvature forms

Abstract: A closed explicit representation of the vacuum Einstein equations in terms of components of curvature 2-forms is given. The discussion is restricted to the case of non-vanishing cubic invariant of conformal curvature spinor.The complete set of algebraic and differential identities connecting particular equations is presented and their consistency conditions are analyzed.

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Cited by 17 publications
(19 citation statements)
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“…They seem to be the first who were able to show that a conformal metric structure is actually implied as a consequence of symmetry and closure. These structures were subsequently discussed by numerous people, by 't Hooft [70], Harnett [18], and Obukhov & Tertychniy [50], amongst others, see also the references given there. These structures were subsequently discussed by numerous people, by 't Hooft [70], Harnett [18], and Obukhov & Tertychniy [50], amongst others, see also the references given there.…”
Section: Dual Operators and Metricsmentioning
confidence: 99%
“…They seem to be the first who were able to show that a conformal metric structure is actually implied as a consequence of symmetry and closure. These structures were subsequently discussed by numerous people, by 't Hooft [70], Harnett [18], and Obukhov & Tertychniy [50], amongst others, see also the references given there. These structures were subsequently discussed by numerous people, by 't Hooft [70], Harnett [18], and Obukhov & Tertychniy [50], amongst others, see also the references given there.…”
Section: Dual Operators and Metricsmentioning
confidence: 99%
“…(5) Extracting the metric: Urbantke [7] (see also the discussions in [9,10]) was able to derive, within SU (2) Yang-Mills theory, a 4-dimensional metric g ij (with i, j, . .…”
mentioning
confidence: 99%
“…At the root of the methods of complex relativity [1][2][3][4][5] is the fact that the Lorentz group O(3, 1) -or rather, its Lie algebra so(3, 1) -admits various isomorphic representations. Perhaps the most studied representation is the (1-to-2) representation of the proper orthochronous Lorentz group SO 0 (3, 1) by the elements of the group SL(2; C), which leads one into the realm of Dirac spinors and relativistic wave mechanics.…”
Section: Introductionmentioning
confidence: 99%
“…Perhaps the most studied representation is the (1-to-2) representation of the proper orthochronous Lorentz group SO 0 (3, 1) by the elements of the group SL(2; C), which leads one into the realm of Dirac spinors and relativistic wave mechanics. One approach to complex relativity then involves the representation of 2-forms on spacetime by SL(2; C) spinors (see Obukhov and Tertychniy [5]). Another approach to complex relativity is based in the fact that there is also an isomorphism of SO 0 (3, 1) with the complex orthogonal group in three dimensions SO(3; C), which acts naturally on C 3 .…”
Section: Introductionmentioning
confidence: 99%