An outline is given of a recently discovered technique for building a quantum effective action that is completely independent of gauge-fixing choices and ghost determinants. One makes maximum use of the geometry and fibre-bundle structure of the space of field histories and introduces a set of nonlocal composite fields: the geodesic normal fields based on Vilkovisky's connection on the space of histories. The closed-time-path formalism of Schwinger, Bakshi, Mahantappa {\it et al} can be adapted for these fields, and a set of gauge-fixing-independent dynamical equations for their expectation values (starting from given initial conditions) can be computed. An obvious application for such equations is to the study of the formation and radiativ...
AbstractIn the recently proposed non-local theory of quantum gravity one can avoid massive tensor gh...
Classical methods of differential geometry are used to construct equations of motion for particles i...
Usually, General Relativity (GR) is known to be unrenormalizable perturbatively from the viewpoint o...
A quantum effective action for gauge field theories is constructed that is gauge invariant and indep...
Our purpose is to explore generalized approaches to the quantization of gravity. In particular, we s...
Recent work in the literature has proposed the use of non-local boundary conditions in Euclidean qua...
Nonlocal boundary conditions for Euclidean quantum gravity have been proposed in the recent literatu...
In the recently proposed non-local theory of quantum gravity one can avoid massive tensor ghosts at ...
We review quantum gravity model building using the new formalism of 'quantum Riemannian geometry' to...
We present the formalism of computing one-loop effective action for Quantum Gravitation using non-lo...
The consistent definition of a quantum gravity theory has to overcome several obstacles. Here we tak...
We describe the construction of quantum gravity, i.e. of a theory of self-interacting massless spin-...
In the Wheeler-DeWitt framework, by a gauge fixing procedure, we set up a scheme to recover a Schr\"...
It is natural to consider a quantum system in the continuum limit ofspace-time configuration. Incorp...
We argue that four-dimensional quantum gravity may be essentially renormalizable provided one relaxe...
AbstractIn the recently proposed non-local theory of quantum gravity one can avoid massive tensor gh...
Classical methods of differential geometry are used to construct equations of motion for particles i...
Usually, General Relativity (GR) is known to be unrenormalizable perturbatively from the viewpoint o...
A quantum effective action for gauge field theories is constructed that is gauge invariant and indep...
Our purpose is to explore generalized approaches to the quantization of gravity. In particular, we s...
Recent work in the literature has proposed the use of non-local boundary conditions in Euclidean qua...
Nonlocal boundary conditions for Euclidean quantum gravity have been proposed in the recent literatu...
In the recently proposed non-local theory of quantum gravity one can avoid massive tensor ghosts at ...
We review quantum gravity model building using the new formalism of 'quantum Riemannian geometry' to...
We present the formalism of computing one-loop effective action for Quantum Gravitation using non-lo...
The consistent definition of a quantum gravity theory has to overcome several obstacles. Here we tak...
We describe the construction of quantum gravity, i.e. of a theory of self-interacting massless spin-...
In the Wheeler-DeWitt framework, by a gauge fixing procedure, we set up a scheme to recover a Schr\"...
It is natural to consider a quantum system in the continuum limit ofspace-time configuration. Incorp...
We argue that four-dimensional quantum gravity may be essentially renormalizable provided one relaxe...
AbstractIn the recently proposed non-local theory of quantum gravity one can avoid massive tensor gh...
Classical methods of differential geometry are used to construct equations of motion for particles i...
Usually, General Relativity (GR) is known to be unrenormalizable perturbatively from the viewpoint o...