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Journal ArticleDOI

Unified geometric theory of gravity and supergravity

S. W. MacDowell, +1 more
- 04 Apr 1977 - 
- Vol. 38, Iss: 14, pp 739-742
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TLDR
In this article, a unified geometric formulation of gravitation and supergravity is presented, which is constructed out of the components of the curvature tensor for bundle spaces with four-dimensional Lorentz base manifold and structure groups Sp(4) for gravity and OSp(1, 4) for supergravity.
Abstract
A unified geometric formulation of gravitation and supergravity is presented. The action for these theories is constructed out of the components of the curvature tensor for bundle spaces with four-dimensional Lorentz base manifold and structure groups Sp(4) for gravity and OSp(1,4) for supergravity. The requirement of invariance under reflections, local Lorentz transformations, and general coordinate transformations uniquely determines the action and ensures the existence of local supersymmetry in supergravity.

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Resonant superalgebras and N = 1 supergravity theories in three spacetime dimensions

TL;DR: In this paper, the authors explore N = 1 supersymmetric extensions of algebras going beyond the Poincare and AdS ones in three spacetime dimensions, and present new superalga-bras which all correspond to super-symmetric extensions with one fermionic charge Q α concerning the so-called resonant alga.
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Surface Charges for Gravity and Electromagnetism in the First Order Formalism

TL;DR: In this paper, a new derivation of surface charges for 3+1 gravity coupled to Electromagnetism is obtained, and the surface charges are quasilocal, explicitly coordinate independent, gauge invariant and background independent.
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Vector stability in quadratic metric-affine theories

TL;DR: In this article , the stability of the four vector irreducible pieces of the torsion and the nonmetricity tensors in the general quadratic metric-affine Lagrangian in 4 dimensions was investigated.
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Gauge theory of gravitation: (4+N)-dimensional theory

TL;DR: In this article, the invariant line element is uniquely determined by the connection one-form which is invariant under the local gauge transformations, and the generalized Lorentz equations are derived as the geodesic equations.
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