Abstract
Parametric manifolds are reparametrization-invariant geometric structures describing space-time and internal degrees of freedom in a unified framework. Using the theory of parametric spinors, a decomposition of the space-time in General Relativity is developed with respect to the 3-space of trajectories of a time-like or space-like vector field. The parametric 3+1 decomposition surpasses the ADM formalism in generality since it is possible even in space-times which do not admit a space-like foliation. (author) 33 refs.
Perjes, Z
[1]
- Hungarian Academy of Sciences, Budapest (Hungary). Central Research Inst. for Physics
Citation Formats
Perjes, Z.
The parametric manifold picture of space-time.
Hungary: N. p.,
1992.
Web.
Perjes, Z.
The parametric manifold picture of space-time.
Hungary.
Perjes, Z.
1992.
"The parametric manifold picture of space-time."
Hungary.
@misc{etde_10119553,
title = {The parametric manifold picture of space-time}
author = {Perjes, Z}
abstractNote = {Parametric manifolds are reparametrization-invariant geometric structures describing space-time and internal degrees of freedom in a unified framework. Using the theory of parametric spinors, a decomposition of the space-time in General Relativity is developed with respect to the 3-space of trajectories of a time-like or space-like vector field. The parametric 3+1 decomposition surpasses the ADM formalism in generality since it is possible even in space-times which do not admit a space-like foliation. (author) 33 refs.}
place = {Hungary}
year = {1992}
month = {Mar}
}
title = {The parametric manifold picture of space-time}
author = {Perjes, Z}
abstractNote = {Parametric manifolds are reparametrization-invariant geometric structures describing space-time and internal degrees of freedom in a unified framework. Using the theory of parametric spinors, a decomposition of the space-time in General Relativity is developed with respect to the 3-space of trajectories of a time-like or space-like vector field. The parametric 3+1 decomposition surpasses the ADM formalism in generality since it is possible even in space-times which do not admit a space-like foliation. (author) 33 refs.}
place = {Hungary}
year = {1992}
month = {Mar}
}