Towards Full ‘Galilei General Relativity’: Bargmann-Minkowski and Bargmann-Galilei Spacetimes
- ORNL
Galilei-Newton spacetime $$\mathbb{G}$$ with its Galilei group can be understood as a `degeneration' as $$c \rightarrow \infty$$ of Minkowski spacetime $$\mathbb{M}$$ with its Poincar\'e group. $$\mathbb{G}$$ does not have a spacetime metric and its Galilei symmetry transformations do not include energy; but Bargmann-Galilei spacetime $$B\mathbb{G}$$, a 5-dimensional extension that preserves Galilei physics, remedies these infelicities. Here an analogous Bargmann-Minkowski spacetime $$B\mathbb{M}$$ is described. While not necessary for Poincar\'e physics, it may illuminate a path towards a more extensive `Galilei general relativity' than is presently known, which would be a useful---and conceptually and mathematically sound---approximation in astrophysical scenarios such as core-collapse supernovae.
- Research Organization:
- Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
- Sponsoring Organization:
- USDOE; USDOE Office of Science (SC), Nuclear Physics (NP) (SC-26)
- DOE Contract Number:
- AC05-00OR22725
- OSTI ID:
- 1999050
- Country of Publication:
- United States
- Language:
- English
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