Citation: Krupka, D.; Brajerˇ cík, J.
Schwarzschild Spacetimes: Topology.
Axioms 2022, 11, 693. https://
doi.org/10.3390/axioms11120693
Academic Editor: Sidney A. Morris
Received: 14 November 2022
Accepted: 2 December 2022
Published: 4 December 2022
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axioms
Article
Schwarzschild Spacetimes: Topology
Demeter Krupka
1,2,†,‡
and Ján Brajerˇ cík
3,
*
,‡
1
Lepage Research Institute, 081 16 Presov, Slovakia
2
Faculty of Mathematics and Computer Science, Transilvania University in Brasov, 500091 Brasov, Romania
3
Faculty of Humanities and Natural Sciences, University of Presov in Presov, 081 16 Presov, Slovakia
* Correspondence: jan.brajercik@unipo.sk
† Current address: Faculty of Humanities and Natural Sciences, University of Presov in Presov, 17. Novembra 1,
081 16 Presov, Slovakia.
‡ These authors contributed equally to this work.
Abstract: This paper is devoted to the geometric theory of a Schwarzschild spacetime, a basic objective
in applications of the classical general relativity theory. In a broader sense, a Schwarzschild spacetime is
a smooth manifold, endowed with an action of the special orthogonal group SO(3) and a Schwarzschild
metric, an SO(3)-invariant metric field, satisfying the Einstein equations. We prove the existence of and
find all Schwarzschild metrics on two topologically non-equivalent manifolds, R × (R
3
\{(0, 0, 0)})
and S
1
× (R
3
\{(0, 0, 0)}). The method includes a classification of SO(3)-invariant, time-translation
invariant and time-reflection invariant metrics on R × (R
3
\{(0, 0, 0)}) and a winding mapping of
the real line R onto the circle S
1
. The resulting family of Schwarzschild metrics is parametrized by an
arbitrary function and two real parameters, the integration constants. For any Schwarzschild metric,
one of the parameters determines a submanifold, where the metric is not defined, the Schwarzschild
sphere. In particular, the family admits a global metric whose Schwarzschild sphere is empty. These
results transfer to S
1
× (R
3
\{(0, 0, 0)}) by the winding mapping. All our assertions are derived
independently of the signature of the Schwarzschild metric; the signature can be chosen as an
independent axiom.
Keywords: manifold topology; Einstein equations; spherical symmetry; Schwarzschild spacetime;
special orthogonal group; SO(3)-action; invariant metric
1. Introduction
In this paper, a Schwarzschild spacetime, or a spherically symmetric spacetime, is a smooth
4-dimensional manifold X endowed with a left action of the special orthogonal group SO(3)
and a non-singular, symmetric (0, 2)-tensor field g, satisfying the following two conditions:
(1) g is SO(3)-invariant.
(2) g solves the Einstein vacuum equations.
where g is a Schwarzschild metric on X.
Standard topological properties are required: X is Hausdorff, second countable, and
connected. As g can be understood as an extremal of an integral variational functional, the
Hilbert variational functional, no a priori restrictions of the signature of g are imposed.
In this paper, we revisit and extend several constructions of classical general relativ-
ity theory, especially the theory of spherically symmetric spacetimes (Einstein 1915 [1],
Hilbert 1915 [2], Schwarzschild 1916 [3]). Since Schwarzschild, spherically symmetric mod-
els became a principal application of the theory, stimulating extensive research on the basis
of classical differential geometry on Riemannian spaces (see Hawking, Ellis 1973 [4] and,
for a more comprehensive contemporary discussion De Felice, Clarke 1990 [5], and Kriele
1999 [6]). Less is known, however, on the effort focused on a deeper understanding of what
is going on from the topological point of view. For first steps in this direction, we refer to
Axioms 2022, 11, 693. https://doi.org/10.3390/axioms11120693 https://www.mdpi.com/journal/axioms