The 4+1 formalism in general relativity (GR) prescribes field equations for the spacetime metric γμνx,τ which is local in the spacetime coordinates x and evolves according to an external “worldtime” τ. This formalism extends to GR the Stueckelberg Horwitz Piron (SHP) framework, developed to address the various issues known as the problem of time as they appear in electrodynamics. SHP field theories exhibit a formal 5D symmetry on (x,τ) that is strategically broken to 4+1 representations of the Lorentz group, resulting in a manifestly covariant canonical formalism describing the τ-evolution of spacetime structures as an initial value problem. Einstein equations for γμνx,τ are found by constructing a 5D pseudo-manifold (combining 4D geometry ...
International audienceThe Lorentzian metric structure used in any field theory allows one to impleme...
Élie Cartan’s invariant integral formalism is extended to gauge field theory, including general rela...
No! We show that the field equations of Einstein–Gauss–Bonnet theory defined in generic $$D>4$$ dime...
It is the author's belief that a perfect theory will eventually be formulated, where geometry and ph...
Abstract We show that Geroch decomposition leads us to Maxwell-like representation of gravity in (3 ...
A foundation is laid for future analyses of gravitation theories. This foundation is applicable to a...
We investigate Lorentzian structures in the four-dimensional space-time, supplemented either by a co...
Recently a new 4D Einstein–Gauss–Bonnet theory has been introduced (Glavan and Lin in Phys Rev Lett ...
We show how a foliated 4-dimensional FLRW-metric becomes a gravitational instanton, if the spatial m...
We consider the five-dimensional Einstein–Gauss–Bonnet gravity, which can be obtained by means of an...
We discussed a mechanism that allows the universe to start from lower dimension (d < 4) in its ve...
The law of gravitational attraction is a window on three formal approaches to laws of nature based o...
In four dimensions complexified general relativity (GR) can be non-trivially deformed: there exists ...
The Poisson-Laplace equation is a working and acceptable equation of gravitation which is mostly use...
This graduate-level, course-based text is devoted to the 3+1 formalism of general relativity, which ...
International audienceThe Lorentzian metric structure used in any field theory allows one to impleme...
Élie Cartan’s invariant integral formalism is extended to gauge field theory, including general rela...
No! We show that the field equations of Einstein–Gauss–Bonnet theory defined in generic $$D>4$$ dime...
It is the author's belief that a perfect theory will eventually be formulated, where geometry and ph...
Abstract We show that Geroch decomposition leads us to Maxwell-like representation of gravity in (3 ...
A foundation is laid for future analyses of gravitation theories. This foundation is applicable to a...
We investigate Lorentzian structures in the four-dimensional space-time, supplemented either by a co...
Recently a new 4D Einstein–Gauss–Bonnet theory has been introduced (Glavan and Lin in Phys Rev Lett ...
We show how a foliated 4-dimensional FLRW-metric becomes a gravitational instanton, if the spatial m...
We consider the five-dimensional Einstein–Gauss–Bonnet gravity, which can be obtained by means of an...
We discussed a mechanism that allows the universe to start from lower dimension (d < 4) in its ve...
The law of gravitational attraction is a window on three formal approaches to laws of nature based o...
In four dimensions complexified general relativity (GR) can be non-trivially deformed: there exists ...
The Poisson-Laplace equation is a working and acceptable equation of gravitation which is mostly use...
This graduate-level, course-based text is devoted to the 3+1 formalism of general relativity, which ...
International audienceThe Lorentzian metric structure used in any field theory allows one to impleme...
Élie Cartan’s invariant integral formalism is extended to gauge field theory, including general rela...
No! We show that the field equations of Einstein–Gauss–Bonnet theory defined in generic $$D>4$$ dime...