Abstract
Generalizing from flat to arbitrary spacetime, we develop the basic formalism of differential geometry, which is the mathematical foundation of the general theory of relativity. Vectors, tensors and the important concept of the covariant derivative are introduced. The latter allows us to compare vectors and tensors at different points. The generalization of symmetry transformations with Killing fields is also introduced.
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Notes
- 1.
In fact this choice is not unique. There are at least two frequently used local cartesian coordinate systems: Riemann normal coordinates and Fermi normal coordinates.
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Note that in flat spacetime we have the relations \(\frac{\partial }{\partial x^\mu } =(\partial _t, \partial _x,\partial _y,\partial _z)=\partial _\mu \equiv _{,\mu }\) and \(\frac{\partial }{\partial x_\mu } =(\partial _t, -\partial _x,-\partial _y,-\partial _z)=\partial ^\mu \equiv ^{,\mu }\)
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Killing, Wilhelm Karl Joseph, German mathematician, *Burbach 10.5.1847, †Münster 11.2.1923.
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Lie, Sophus, Norwegian mathematician, *Nordfjordeit 17.12.1842, †Kristiania 18.2.1899.
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Hentschke, R., Hölbling, C. (2020). Introduction to Multidimensional Calculus. In: A Short Course in General Relativity and Cosmology. Undergraduate Lecture Notes in Physics. Springer, Cham. https://doi.org/10.1007/978-3-030-46384-7_3
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DOI: https://doi.org/10.1007/978-3-030-46384-7_3
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