Abstract
There are four definitions of a symmetric space M:
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1
The global one: M = GIH is a homogeneous space, where H is essentially the group of fixed points of an involution σ of a Lie group G.
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2
The infinitesimal one: M is a real manifold with a torsionfree affine connection \( \nabla \) whose curvature is covariantly constant: \( \nabla R{\text{ = 0}} \) .
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3
The mixed one: M is a real manifold with an affine connection \( \nabla \) such that the geodesic symmetry s P with respect to any point p ε M is an automorphism of \( \nabla \) .
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4
The algebraic one, which reflects axiomatically the properties of the map \( \mu :M \times M \to M{\mathbf{ }}{\text{given by}}{\mathbf{ }}\mu \left( {x,y} \right): = s_x \left( y \right){\mathbf{ }}{\text{with}}{\mathbf{ }}s_x {\mathbf{ }}{\text{as in}}{\mathbf{ }}\left( {\text{3}} \right) \).
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© 2000 Springer-Verlag Berlin Heidelberg
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(2000). Chapter I: Symmetric spaces and the Lie-functor. In: Bertram, W. (eds) The Geometry of Jordan and Lie Structures. Lecture Notes in Mathematics, vol 1754. Springer, Berlin, Heidelberg. https://doi.org/10.1007/3-540-44458-0_1
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DOI: https://doi.org/10.1007/3-540-44458-0_1
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